Palace is an open-source 3D electromagnetic simulator supporting eigenmode, driven (S-parameter), and electrostatic simulations. This notebook demonstrates using the gsim.palace API to run a driven simulation on a CPW (coplanar waveguide) structure with wave ports.
Requirements:
- IHP PDK:
uv pip install ihp-gdsfactory - GDSFactory+ account for cloud simulation
Define GSG electrode¶
import gdsfactory as gf
from ihp import LAYER, PDK
PDK.activate()
@gf.cell
def gsg_electrode(
length: float = 800,
s_width: float = 20,
g_width: float = 40,
gap_width: float = 15,
layer=LAYER.TopMetal2drawing,
) -> gf.Component:
"""
Create a GSG (Ground-Signal-Ground) electrode.
Args:
length: horizontal length of the electrodes
s_width: width of the signal (center) electrode
g_width: width of the ground electrodes
gap_width: gap between signal and ground electrodes
layer: layer for the metal
"""
c = gf.Component()
r1 = c << gf.c.rectangle((length, g_width), centered=True, layer=layer)
r1.move((0, (g_width + s_width) / 2 + gap_width))
_r2 = c << gf.c.rectangle((length, s_width), centered=True, layer=layer)
r3 = c << gf.c.rectangle((length, g_width), centered=True, layer=layer)
r3.move((0, -(g_width + s_width) / 2 - gap_width))
c.add_port(
name="o1",
center=(-length / 2, 0),
width=s_width,
orientation=180,
port_type="electrical",
layer=layer,
)
c.add_port(
name="o2",
center=(length / 2, 0),
width=s_width,
orientation=0,
port_type="electrical",
layer=layer,
)
return c
c = gsg_electrode()
cc = c.copy()
cc.draw_ports()
cc
Configure simulation¶
from gsim.common.stack import get_stack
from gsim.palace import DrivenSim
sim = DrivenSim()
sim.set_output_dir("./palace-sim-cpw-waveport")
sim.set_geometry(c)
stack = get_stack() # auto-detects active PDK
sim.set_stack(stack)
sim.set_airbox(margin_x=0.0, margin_y=50, z_above=100.0, z_below=100.0)
# Wave ports — max_size fills the full domain boundary
sim.add_wave_port("o1", layer="topmetal2", max_size=True, mode=1, excited=True)
sim.add_wave_port("o2", layer="topmetal2", max_size=True, mode=1, excited=False)
sim.set_driven(fmin=1e9, fmax=100e9, num_points=300)
print(sim.validate_config())
Validation: PASSED
Generate mesh¶
Mesh Summary
========================================
Dimensions: 800.0 x 130.0 x 217.9 µm
Nodes: 31,782
Elements: 225,787
Tetrahedra: 157,469
Edge length: 1.16 - 76.42 µm
Quality: 0.643 (min: 0.000)
SICN: 0.695 (all valid)
----------------------------------------
Volumes (3):
- si [1]
- sin [2]
- air [3]
Surfaces (10):
- topmetal2_xy [4]
- topmetal2_z [5]
- P1 [6]
- P2 [7]
- si__None [8]
- si__sin [9]
- air__si [10]
- sin__None [11]
- air__sin [12]
- air__None [13]
----------------------------------------
Mesh: palace-sim-cpw-waveport/palace.msh
sim.plot_mesh(
style="solid",
transparent_groups=["air__None", "SiO2__None", "SiO2__passive", "air__passive"],
interactive=True,
)
Widget(value='<iframe src="http://localhost:39883/index.html?ui=P_0x7aee86368440_0&reconnect=auto" class="pyvi…
Run simulation¶
Running Palace simulation in palace-sim-cpw-waveport via Apptainer
Command: apptainer run /home/martin/Desktop/palace/Palace.sif -np 32 config.json
Processes: 32
>> /usr/lib64/mpich/bin/mpirun -n 32 /opt/palace/bin/palace-x86_64.bin config.json
_____________ _______
_____ __ \____ __ /____ ____________
____ /_/ / __ ` / / __ ` / ___/ _ \
___ _____/ /_/ / / /_/ / /__/ ___/
/__/ \___,__/__/\___,__/\_____\_____/
[38;2;255;255;000m--> Warning![0m
Output folder is not empty; program will overwrite content! (output/palace)
Git changeset ID: v0.14.0-305-g51d61b03
Running with 32 MPI processes, 1 OpenMP thread
Device configuration: omp,cpu
Memory configuration: host-std
libCEED backend: /cpu/self/xsmm/blocked
Added 12868 duplicate vertices for interior boundaries in the mesh
Added 24140 duplicate boundary elements for interior boundaries in the mesh
Finished partitioning mesh into 32 subdomains
Characteristic length and time scales:
L₀ = 8.000e-04 m, t₀ = 2.669e-03 ns
Mesh curvature order: 1
Mesh bounding box:
(Xmin, Ymin, Zmin) = (-4.000e-04, -6.500e-05, -1.020e-04) m
(Xmax, Ymax, Zmax) = (+4.000e-04, +6.500e-05, +1.159e-04) m
Parallel Mesh Stats:
minimum average maximum total
vertices 1102 1395 1986 44650
edges 6538 7386 8919 236365
faces 10216 10912 11933 349187
elements 4775 4920 5060 157469
neighbors 1 5 12
minimum maximum
h 0.000488503 0.0726176
kappa 1.06644 9588.47
Configuring Robin absorbing BC (order 2) at attributes:
8, 11, 13
Configuring Robin finite conductivity BC at attributes:
4: σ = 3.770e+07 S/m, h = 3.000e-06 m, n = (-0.0,+0.0,+1.0)
5: σ = 3.770e+07 S/m, h = 3.000e-06 m, n = (-0.0,+1.0,-0.0)
Configuring Robin impedance BC for wave ports at attributes:
6: Index = 1, mode = 1, d = 0.000e+00 m, n = (-1.0,+0.0,+0.0)
7: Index = 2, mode = 1, d = 0.000e+00 m, n = (+1.0,-0.0,+0.0)
Configuring wave port excitation source term at attributes:
6: Index = 1
Computing adaptive fast frequency response for:
Excitation with index 1 has contributions from:
Wave port 1
Beginning PROM construction offline phase:
300 points for frequency sweep over [1.000e+00, 1.000e+02] GHz
Assembling system matrices, number of global unknowns:
H1 (p = 2): 281015, ND (p = 2): 1171104, RT (p = 2): 1519968
Operator assembly level: Partial
Mesh geometries:
Tetrahedron: P = 20, Q = 11 (quadrature order = 4)
SuperLUSolver: Using 2D processor grid 4 x 8
Assembling multigrid hierarchy:
Level 0 (p = 1): 236365 unknowns
Level 1 (p = 2): 1171104 unknowns
Level 0 (auxiliary) (p = 1): 44650 unknowns
Level 1 (auxiliary) (p = 2): 281015 unknowns
Residual norms for GMRES solve
matrix dimension 236365
nonzeros in A 3276301
nonzeros in L 24813022
nonzeros in U 24813022
nonzeros in L+U 49389679
fill ratio 15.1
nonzeros in LSUB 8903849
** Memory Usage **********************************
** Total highmark (MB):
Sum-of-all : 6121.23 | Avg : 191.29 | Max : 202.14
Max at rank 0, different stages (MB):
. symbfact 93.28
. distribution 202.14
. numfact 64.14
** NUMfact space (MB): (sum-of-all-processes)
L\U : 424.74 | Total : 1714.60
. max at rank 0, max L+U memory (MB): 21.39
. max at rank 0, peak buffer (MB): 42.75
**************************************************
** number of Tiny Pivots: 0
0 (restart 0) KSP residual norm 1.437026e+01
1 (restart 0) KSP residual norm 8.857565e-01
2 (restart 0) KSP residual norm 5.792461e-01
3 (restart 0) KSP residual norm 2.637307e-01
4 (restart 0) KSP residual norm 9.680516e-02
5 (restart 0) KSP residual norm 5.520069e-02
6 (restart 0) KSP residual norm 2.403880e-02
7 (restart 0) KSP residual norm 1.076663e-02
8 (restart 0) KSP residual norm 6.354224e-03
9 (restart 0) KSP residual norm 2.986658e-03
10 (restart 0) KSP residual norm 1.430765e-03
11 (restart 0) KSP residual norm 6.925066e-04
12 (restart 0) KSP residual norm 3.569574e-04
13 (restart 0) KSP residual norm 1.888039e-04
14 (restart 0) KSP residual norm 9.334298e-05
15 (restart 0) KSP residual norm 4.872965e-05
16 (restart 0) KSP residual norm 2.692565e-05
17 (restart 0) KSP residual norm 1.262970e-05
GMRES solver converged in 17 iterations (avg. reduction factor: 4.403e-01)
Field energy E (4.500e-04 J) + H (7.455e-04 J) = 1.195e-03 J
Residual norms for GMRES solve
** Memory Usage **********************************
** Total highmark (MB):
Sum-of-all : 4298.50 | Avg : 134.33 | Max : 143.07
Max at rank 0, different stages (MB):
. symbfact 0.00
. distribution 143.07
. numfact 64.14
** NUMfact space (MB): (sum-of-all-processes)
L\U : 424.74 | Total : 1714.60
. max at rank 0, max L+U memory (MB): 21.39
. max at rank 0, peak buffer (MB): 42.75
**************************************************
** number of Tiny Pivots: 0
0 (restart 0) KSP residual norm 3.870970e+01
1 (restart 0) KSP residual norm 1.343310e+01
2 (restart 0) KSP residual norm 2.877341e+00
3 (restart 0) KSP residual norm 2.121828e+00
4 (restart 0) KSP residual norm 7.522934e-01
5 (restart 0) KSP residual norm 2.040666e-01
6 (restart 0) KSP residual norm 1.063096e-01
7 (restart 0) KSP residual norm 2.795640e-02
8 (restart 0) KSP residual norm 1.405320e-02
9 (restart 0) KSP residual norm 6.217120e-03
10 (restart 0) KSP residual norm 3.547154e-03
11 (restart 0) KSP residual norm 1.308864e-03
12 (restart 0) KSP residual norm 8.909906e-04
13 (restart 0) KSP residual norm 3.173387e-04
14 (restart 0) KSP residual norm 1.851786e-04
15 (restart 0) KSP residual norm 8.850850e-05
16 (restart 0) KSP residual norm 5.262272e-05
17 (restart 0) KSP residual norm 2.677062e-05
GMRES solver converged in 17 iterations (avg. reduction factor: 4.341e-01)
Field energy E (4.432e-04 J) + H (5.322e-04 J) = 9.754e-04 J
Residual norms for GMRES solve
** Memory Usage **********************************
** Total highmark (MB):
Sum-of-all : 4298.50 | Avg : 134.33 | Max : 143.07
Max at rank 0, different stages (MB):
. symbfact 0.00
. distribution 143.07
. numfact 64.14
** NUMfact space (MB): (sum-of-all-processes)
L\U : 424.74 | Total : 1714.60
. max at rank 0, max L+U memory (MB): 21.39
. max at rank 0, peak buffer (MB): 42.75
**************************************************
** number of Tiny Pivots: 0
0 (restart 0) KSP residual norm 1.041158e+02
1 (restart 0) KSP residual norm 6.358696e+00
2 (restart 0) KSP residual norm 1.343908e+00
3 (restart 0) KSP residual norm 3.791705e-01
4 (restart 0) KSP residual norm 1.296702e-01
5 (restart 0) KSP residual norm 6.934422e-02
6 (restart 0) KSP residual norm 2.561908e-02
7 (restart 0) KSP residual norm 1.198874e-02
8 (restart 0) KSP residual norm 6.103337e-03
9 (restart 0) KSP residual norm 2.753844e-03
10 (restart 0) KSP residual norm 1.341485e-03
11 (restart 0) KSP residual norm 5.601082e-04
12 (restart 0) KSP residual norm 2.628957e-04
13 (restart 0) KSP residual norm 1.356185e-04
14 (restart 0) KSP residual norm 6.393873e-05
GMRES solver converged in 14 iterations (avg. reduction factor: 3.600e-01)
Greedy iteration 1 (n = 4): ω* = 7.010e+01 GHz (1.175e+00), error = 1.562e-01
Field energy E (4.271e-04 J) + H (5.444e-04 J) = 9.715e-04 J
Residual norms for GMRES solve
** Memory Usage **********************************
** Total highmark (MB):
Sum-of-all : 4298.50 | Avg : 134.33 | Max : 143.07
Max at rank 0, different stages (MB):
. symbfact 0.00
. distribution 143.07
. numfact 64.14
** NUMfact space (MB): (sum-of-all-processes)
L\U : 424.74 | Total : 1714.60
. max at rank 0, max L+U memory (MB): 21.39
. max at rank 0, peak buffer (MB): 42.75
**************************************************
** number of Tiny Pivots: 0
0 (restart 0) KSP residual norm 2.099524e+01
1 (restart 0) KSP residual norm 2.737448e+00
2 (restart 0) KSP residual norm 2.304398e+00
3 (restart 0) KSP residual norm 7.382467e-01
4 (restart 0) KSP residual norm 1.177362e-01
5 (restart 0) KSP residual norm 4.742292e-02
6 (restart 0) KSP residual norm 1.699722e-02
7 (restart 0) KSP residual norm 6.904003e-03
8 (restart 0) KSP residual norm 3.745203e-03
9 (restart 0) KSP residual norm 1.724921e-03
10 (restart 0) KSP residual norm 7.703708e-04
11 (restart 0) KSP residual norm 3.154492e-04
12 (restart 0) KSP residual norm 1.220824e-04
13 (restart 0) KSP residual norm 5.593908e-05
14 (restart 0) KSP residual norm 2.817982e-05
15 (restart 0) KSP residual norm 1.472389e-05
GMRES solver converged in 15 iterations (avg. reduction factor: 3.888e-01)
Greedy iteration 2 (n = 6): ω* = 2.965e+01 GHz (4.972e-01), error = 5.275e-02
Field energy E (4.335e-04 J) + H (5.638e-04 J) = 9.973e-04 J
Residual norms for GMRES solve
** Memory Usage **********************************
** Total highmark (MB):
Sum-of-all : 4298.50 | Avg : 134.33 | Max : 143.07
Max at rank 0, different stages (MB):
. symbfact 0.00
. distribution 143.07
. numfact 64.14
** NUMfact space (MB): (sum-of-all-processes)
L\U : 424.74 | Total : 1714.60
. max at rank 0, max L+U memory (MB): 21.39
. max at rank 0, peak buffer (MB): 42.75
**************************************************
** number of Tiny Pivots: 0
0 (restart 0) KSP residual norm 8.901491e+01
1 (restart 0) KSP residual norm 9.713437e+00
2 (restart 0) KSP residual norm 1.757565e+00
3 (restart 0) KSP residual norm 6.571890e-01
4 (restart 0) KSP residual norm 4.091488e-01
5 (restart 0) KSP residual norm 1.404823e-01
6 (restart 0) KSP residual norm 7.503538e-02
7 (restart 0) KSP residual norm 1.877109e-02
8 (restart 0) KSP residual norm 9.577813e-03
9 (restart 0) KSP residual norm 4.924907e-03
10 (restart 0) KSP residual norm 2.485644e-03
11 (restart 0) KSP residual norm 1.175951e-03
12 (restart 0) KSP residual norm 5.673710e-04
13 (restart 0) KSP residual norm 2.609869e-04
14 (restart 0) KSP residual norm 1.080851e-04
15 (restart 0) KSP residual norm 6.683098e-05
GMRES solver converged in 15 iterations (avg. reduction factor: 3.906e-01)
Greedy iteration 3 (n = 8): ω* = 8.795e+01 GHz (1.475e+00), error = 1.087e-03, memory = 1/2
Field energy E (4.362e-04 J) + H (5.365e-04 J) = 9.727e-04 J
Residual norms for GMRES solve
** Memory Usage **********************************
** Total highmark (MB):
Sum-of-all : 4298.50 | Avg : 134.33 | Max : 143.07
Max at rank 0, different stages (MB):
. symbfact 0.00
. distribution 143.07
. numfact 64.14
** NUMfact space (MB): (sum-of-all-processes)
L\U : 424.74 | Total : 1714.60
. max at rank 0, max L+U memory (MB): 21.39
. max at rank 0, peak buffer (MB): 42.75
**************************************************
** number of Tiny Pivots: 0
0 (restart 0) KSP residual norm 1.618304e+01
1 (restart 0) KSP residual norm 1.259568e+00
2 (restart 0) KSP residual norm 3.181363e-01
3 (restart 0) KSP residual norm 1.472600e-01
4 (restart 0) KSP residual norm 6.438166e-02
5 (restart 0) KSP residual norm 2.970206e-02
6 (restart 0) KSP residual norm 8.932731e-03
7 (restart 0) KSP residual norm 5.745464e-03
8 (restart 0) KSP residual norm 1.874961e-03
9 (restart 0) KSP residual norm 1.166386e-03
10 (restart 0) KSP residual norm 4.389582e-04
11 (restart 0) KSP residual norm 2.212559e-04
12 (restart 0) KSP residual norm 1.095197e-04
13 (restart 0) KSP residual norm 4.645028e-05
14 (restart 0) KSP residual norm 2.274125e-05
15 (restart 0) KSP residual norm 1.308180e-05
GMRES solver converged in 15 iterations (avg. reduction factor: 3.925e-01)
Greedy iteration 4 (n = 10): ω* = 1.177e+01 GHz (1.974e-01), error = 1.216e-02, memory = 2/2
Field energy E (4.458e-04 J) + H (5.911e-04 J) = 1.037e-03 J
Adaptive sampling converged with 6 frequency samples:
n = 12, error = 1.216e-02, tol = 2.000e-02, memory = 2/2
Sampled frequencies (GHz): 1.000e+00, 1.000e+02, 7.010e+01, 2.965e+01,
8.795e+01, 1.177e+01
Sample errors: inf, inf, 1.562e-01, 5.275e-02, 1.087e-03,
1.216e-02
Total offline phase elapsed time: 1.51e+02 s
Beginning fast frequency sweep online phase
It 1/300: ω/2π = 1.000e+00 GHz (total elapsed time = 1.51e+02 s)
Calculating boundary modes at wave ports for ω/2π = 1.000e+00 GHz (1.677e-02)
Port 1, mode 1: kₙ = 7.042e+01-3.239e-03i m⁻¹
Port 2, mode 1: kₙ = 7.042e+01-3.239e-03i m⁻¹
Sol. ||E|| = 1.462411e+01
Field energy E (4.500e-04 J) + H (7.455e-04 J) = 1.195e-03 J
S[1][1] = -7.173e-01+2.197e-03i, |S[1][1]| = -2.886e+00, arg(S[1][1]) = +1.798e+02
S[2][1] = +2.798e-01-6.446e-03i, |S[2][1]| = -1.106e+01, arg(S[2][1]) = -1.320e+00
It 2/300: ω/2π = 1.331e+00 GHz (total elapsed time = 1.52e+02 s)
Calculating boundary modes at wave ports for ω/2π = 1.331e+00 GHz (2.232e-02)
Port 1, mode 1: kₙ = 9.374e+01-4.312e-03i m⁻¹
Port 2, mode 1: kₙ = 9.374e+01-4.312e-03i m⁻¹
Sol. ||E|| = 1.462224e+01
Field energy E (4.497e-04 J) + H (7.164e-04 J) = 1.166e-03 J
S[1][1] = -7.171e-01+2.743e-03i, |S[1][1]| = -2.889e+00, arg(S[1][1]) = +1.798e+02
S[2][1] = +2.795e-01-8.454e-03i, |S[2][1]| = -1.107e+01, arg(S[2][1]) = -1.732e+00
It 3/300: ω/2π = 1.662e+00 GHz (total elapsed time = 1.52e+02 s)
Calculating boundary modes at wave ports for ω/2π = 1.662e+00 GHz (2.787e-02)
Port 1, mode 1: kₙ = 1.171e+02-5.385e-03i m⁻¹
Port 2, mode 1: kₙ = 1.171e+02-5.384e-03i m⁻¹
Sol. ||E|| = 1.462092e+01
Field energy E (4.496e-04 J) + H (6.956e-04 J) = 1.145e-03 J
S[1][1] = -7.169e-01+3.266e-03i, |S[1][1]| = -2.891e+00, arg(S[1][1]) = +1.797e+02
S[2][1] = +2.793e-01-1.041e-02i, |S[2][1]| = -1.107e+01, arg(S[2][1]) = -2.136e+00
It 4/300: ω/2π = 1.993e+00 GHz (total elapsed time = 1.53e+02 s)
Calculating boundary modes at wave ports for ω/2π = 1.993e+00 GHz (3.342e-02)
Port 1, mode 1: kₙ = 1.404e+02-6.457e-03i m⁻¹
Port 2, mode 1: kₙ = 1.404e+02-6.457e-03i m⁻¹
Sol. ||E|| = 1.462001e+01
Field energy E (4.494e-04 J) + H (6.801e-04 J) = 1.130e-03 J
S[1][1] = -7.167e-01+3.776e-03i, |S[1][1]| = -2.894e+00, arg(S[1][1]) = +1.797e+02
S[2][1] = +2.790e-01-1.235e-02i, |S[2][1]| = -1.108e+01, arg(S[2][1]) = -2.535e+00
It 5/300: ω/2π = 2.324e+00 GHz (total elapsed time = 1.53e+02 s)
Calculating boundary modes at wave ports for ω/2π = 2.324e+00 GHz (3.897e-02)
Port 1, mode 1: kₙ = 1.637e+02-7.530e-03i m⁻¹
Port 2, mode 1: kₙ = 1.637e+02-7.529e-03i m⁻¹
Sol. ||E|| = 1.461934e+01
Field energy E (4.494e-04 J) + H (6.681e-04 J) = 1.117e-03 J
S[1][1] = -7.165e-01+4.277e-03i, |S[1][1]| = -2.896e+00, arg(S[1][1]) = +1.797e+02
S[2][1] = +2.787e-01-1.428e-02i, |S[2][1]| = -1.108e+01, arg(S[2][1]) = -2.932e+00
It 6/300: ω/2π = 2.656e+00 GHz (total elapsed time = 1.53e+02 s)
Calculating boundary modes at wave ports for ω/2π = 2.656e+00 GHz (4.452e-02)
Port 1, mode 1: kₙ = 1.870e+02-8.603e-03i m⁻¹
Port 2, mode 1: kₙ = 1.870e+02-8.602e-03i m⁻¹
Sol. ||E|| = 1.461876e+01
Field energy E (4.493e-04 J) + H (6.584e-04 J) = 1.108e-03 J
S[1][1] = -7.163e-01+4.770e-03i, |S[1][1]| = -2.898e+00, arg(S[1][1]) = +1.796e+02
S[2][1] = +2.784e-01-1.620e-02i, |S[2][1]| = -1.109e+01, arg(S[2][1]) = -3.329e+00
It 7/300: ω/2π = 2.987e+00 GHz (total elapsed time = 1.54e+02 s)
Calculating boundary modes at wave ports for ω/2π = 2.987e+00 GHz (5.008e-02)
Port 1, mode 1: kₙ = 2.103e+02-9.675e-03i m⁻¹
Port 2, mode 1: kₙ = 2.103e+02-9.674e-03i m⁻¹
Sol. ||E|| = 1.461818e+01
Field energy E (4.492e-04 J) + H (6.505e-04 J) = 1.100e-03 J
S[1][1] = -7.161e-01+5.257e-03i, |S[1][1]| = -2.901e+00, arg(S[1][1]) = +1.796e+02
S[2][1] = +2.781e-01-1.811e-02i, |S[2][1]| = -1.110e+01, arg(S[2][1]) = -3.725e+00
It 8/300: ω/2π = 3.318e+00 GHz (total elapsed time = 1.54e+02 s)
Calculating boundary modes at wave ports for ω/2π = 3.318e+00 GHz (5.563e-02)
Port 1, mode 1: kₙ = 2.336e+02-1.075e-02i m⁻¹
Port 2, mode 1: kₙ = 2.336e+02-1.075e-02i m⁻¹
Sol. ||E|| = 1.461754e+01
Field energy E (4.491e-04 J) + H (6.439e-04 J) = 1.093e-03 J
S[1][1] = -7.158e-01+5.738e-03i, |S[1][1]| = -2.903e+00, arg(S[1][1]) = +1.795e+02
S[2][1] = +2.778e-01-2.001e-02i, |S[2][1]| = -1.110e+01, arg(S[2][1]) = -4.120e+00
It 9/300: ω/2π = 3.649e+00 GHz (total elapsed time = 1.54e+02 s)
Calculating boundary modes at wave ports for ω/2π = 3.649e+00 GHz (6.118e-02)
Port 1, mode 1: kₙ = 2.570e+02-1.182e-02i m⁻¹
Port 2, mode 1: kₙ = 2.570e+02-1.182e-02i m⁻¹
Sol. ||E|| = 1.461680e+01
Field energy E (4.491e-04 J) + H (6.382e-04 J) = 1.087e-03 J
S[1][1] = -7.156e-01+6.215e-03i, |S[1][1]| = -2.906e+00, arg(S[1][1]) = +1.795e+02
S[2][1] = +2.775e-01-2.192e-02i, |S[2][1]| = -1.111e+01, arg(S[2][1]) = -4.516e+00
It 10/300: ω/2π = 3.980e+00 GHz (total elapsed time = 1.54e+02 s)
Calculating boundary modes at wave ports for ω/2π = 3.980e+00 GHz (6.673e-02)
Port 1, mode 1: kₙ = 2.803e+02-1.289e-02i m⁻¹
Port 2, mode 1: kₙ = 2.803e+02-1.289e-02i m⁻¹
Sol. ||E|| = 1.461597e+01
Field energy E (4.490e-04 J) + H (6.333e-04 J) = 1.082e-03 J
S[1][1] = -7.154e-01+6.687e-03i, |S[1][1]| = -2.909e+00, arg(S[1][1]) = +1.795e+02
S[2][1] = +2.771e-01-2.381e-02i, |S[2][1]| = -1.111e+01, arg(S[2][1]) = -4.912e+00
It 11/300: ω/2π = 4.311e+00 GHz (total elapsed time = 1.55e+02 s)
Calculating boundary modes at wave ports for ω/2π = 4.311e+00 GHz (7.228e-02)
Port 1, mode 1: kₙ = 3.036e+02-1.397e-02i m⁻¹
Port 2, mode 1: kₙ = 3.036e+02-1.396e-02i m⁻¹
Sol. ||E|| = 1.461501e+01
Field energy E (4.489e-04 J) + H (6.291e-04 J) = 1.078e-03 J
S[1][1] = -7.151e-01+7.155e-03i, |S[1][1]| = -2.912e+00, arg(S[1][1]) = +1.794e+02
S[2][1] = +2.767e-01-2.571e-02i, |S[2][1]| = -1.112e+01, arg(S[2][1]) = -5.307e+00
It 12/300: ω/2π = 4.642e+00 GHz (total elapsed time = 1.55e+02 s)
Calculating boundary modes at wave ports for ω/2π = 4.642e+00 GHz (7.783e-02)
Port 1, mode 1: kₙ = 3.269e+02-1.504e-02i m⁻¹
Port 2, mode 1: kₙ = 3.269e+02-1.504e-02i m⁻¹
Sol. ||E|| = 1.461394e+01
Field energy E (4.489e-04 J) + H (6.254e-04 J) = 1.074e-03 J
S[1][1] = -7.149e-01+7.620e-03i, |S[1][1]| = -2.915e+00, arg(S[1][1]) = +1.794e+02
S[2][1] = +2.763e-01-2.760e-02i, |S[2][1]| = -1.113e+01, arg(S[2][1]) = -5.703e+00
It 13/300: ω/2π = 4.973e+00 GHz (total elapsed time = 1.55e+02 s)
Calculating boundary modes at wave ports for ω/2π = 4.973e+00 GHz (8.339e-02)
Port 1, mode 1: kₙ = 3.502e+02-1.611e-02i m⁻¹
Port 2, mode 1: kₙ = 3.502e+02-1.611e-02i m⁻¹
Sol. ||E|| = 1.461276e+01
Field energy E (4.488e-04 J) + H (6.221e-04 J) = 1.071e-03 J
S[1][1] = -7.146e-01+8.082e-03i, |S[1][1]| = -2.918e+00, arg(S[1][1]) = +1.794e+02
S[2][1] = +2.759e-01-2.948e-02i, |S[2][1]| = -1.114e+01, arg(S[2][1]) = -6.098e+00
It 14/300: ω/2π = 5.304e+00 GHz (total elapsed time = 1.56e+02 s)
Calculating boundary modes at wave ports for ω/2π = 5.304e+00 GHz (8.894e-02)
Port 1, mode 1: kₙ = 3.736e+02-1.718e-02i m⁻¹
Port 2, mode 1: kₙ = 3.736e+02-1.718e-02i m⁻¹
Sol. ||E|| = 1.461147e+01
Field energy E (4.487e-04 J) + H (6.192e-04 J) = 1.068e-03 J
S[1][1] = -7.143e-01+8.540e-03i, |S[1][1]| = -2.921e+00, arg(S[1][1]) = +1.793e+02
S[2][1] = +2.755e-01-3.136e-02i, |S[2][1]| = -1.114e+01, arg(S[2][1]) = -6.494e+00
It 15/300: ω/2π = 5.635e+00 GHz (total elapsed time = 1.56e+02 s)
Calculating boundary modes at wave ports for ω/2π = 5.635e+00 GHz (9.449e-02)
Port 1, mode 1: kₙ = 3.969e+02-1.826e-02i m⁻¹
Port 2, mode 1: kₙ = 3.969e+02-1.825e-02i m⁻¹
Sol. ||E|| = 1.461007e+01
Field energy E (4.486e-04 J) + H (6.165e-04 J) = 1.065e-03 J
S[1][1] = -7.141e-01+8.995e-03i, |S[1][1]| = -2.925e+00, arg(S[1][1]) = +1.793e+02
S[2][1] = +2.750e-01-3.323e-02i, |S[2][1]| = -1.115e+01, arg(S[2][1]) = -6.890e+00
It 16/300: ω/2π = 5.967e+00 GHz (total elapsed time = 1.56e+02 s)
Calculating boundary modes at wave ports for ω/2π = 5.967e+00 GHz (1.000e-01)
Port 1, mode 1: kₙ = 4.202e+02-1.933e-02i m⁻¹
Port 2, mode 1: kₙ = 4.202e+02-1.933e-02i m⁻¹
Sol. ||E|| = 1.460856e+01
Field energy E (4.485e-04 J) + H (6.142e-04 J) = 1.063e-03 J
S[1][1] = -7.138e-01+9.447e-03i, |S[1][1]| = -2.928e+00, arg(S[1][1]) = +1.792e+02
S[2][1] = +2.745e-01-3.509e-02i, |S[2][1]| = -1.116e+01, arg(S[2][1]) = -7.286e+00
It 17/300: ω/2π = 6.298e+00 GHz (total elapsed time = 1.56e+02 s)
Calculating boundary modes at wave ports for ω/2π = 6.298e+00 GHz (1.056e-01)
Port 1, mode 1: kₙ = 4.435e+02-2.040e-02i m⁻¹
Port 2, mode 1: kₙ = 4.435e+02-2.040e-02i m⁻¹
Sol. ||E|| = 1.460696e+01
Field energy E (4.484e-04 J) + H (6.120e-04 J) = 1.060e-03 J
S[1][1] = -7.135e-01+9.895e-03i, |S[1][1]| = -2.932e+00, arg(S[1][1]) = +1.792e+02
S[2][1] = +2.740e-01-3.696e-02i, |S[2][1]| = -1.117e+01, arg(S[2][1]) = -7.682e+00
It 18/300: ω/2π = 6.629e+00 GHz (total elapsed time = 1.57e+02 s)
Calculating boundary modes at wave ports for ω/2π = 6.629e+00 GHz (1.111e-01)
Port 1, mode 1: kₙ = 4.668e+02-2.147e-02i m⁻¹
Port 2, mode 1: kₙ = 4.668e+02-2.147e-02i m⁻¹
Sol. ||E|| = 1.460525e+01
Field energy E (4.482e-04 J) + H (6.100e-04 J) = 1.058e-03 J
S[1][1] = -7.131e-01+1.034e-02i, |S[1][1]| = -2.935e+00, arg(S[1][1]) = +1.792e+02
S[2][1] = +2.734e-01-3.881e-02i, |S[2][1]| = -1.118e+01, arg(S[2][1]) = -8.079e+00
It 19/300: ω/2π = 6.960e+00 GHz (total elapsed time = 1.57e+02 s)
Calculating boundary modes at wave ports for ω/2π = 6.960e+00 GHz (1.167e-01)
Port 1, mode 1: kₙ = 4.901e+02-2.255e-02i m⁻¹
Port 2, mode 1: kₙ = 4.901e+02-2.254e-02i m⁻¹
Sol. ||E|| = 1.460345e+01
Field energy E (4.481e-04 J) + H (6.082e-04 J) = 1.056e-03 J
S[1][1] = -7.128e-01+1.078e-02i, |S[1][1]| = -2.939e+00, arg(S[1][1]) = +1.791e+02
S[2][1] = +2.728e-01-4.066e-02i, |S[2][1]| = -1.119e+01, arg(S[2][1]) = -8.475e+00
It 20/300: ω/2π = 7.291e+00 GHz (total elapsed time = 1.57e+02 s)
Calculating boundary modes at wave ports for ω/2π = 7.291e+00 GHz (1.222e-01)
Port 1, mode 1: kₙ = 5.135e+02-2.362e-02i m⁻¹
Port 2, mode 1: kₙ = 5.135e+02-2.362e-02i m⁻¹
Sol. ||E|| = 1.460155e+01
Field energy E (4.480e-04 J) + H (6.065e-04 J) = 1.055e-03 J
S[1][1] = -7.125e-01+1.122e-02i, |S[1][1]| = -2.943e+00, arg(S[1][1]) = +1.791e+02
S[2][1] = +2.723e-01-4.250e-02i, |S[2][1]| = -1.120e+01, arg(S[2][1]) = -8.872e+00
It 21/300: ω/2π = 7.622e+00 GHz (total elapsed time = 1.58e+02 s)
Calculating boundary modes at wave ports for ω/2π = 7.622e+00 GHz (1.278e-01)
Port 1, mode 1: kₙ = 5.368e+02-2.469e-02i m⁻¹
Port 2, mode 1: kₙ = 5.368e+02-2.469e-02i m⁻¹
Sol. ||E|| = 1.459956e+01
Field energy E (4.479e-04 J) + H (6.050e-04 J) = 1.053e-03 J
S[1][1] = -7.121e-01+1.166e-02i, |S[1][1]| = -2.948e+00, arg(S[1][1]) = +1.791e+02
S[2][1] = +2.716e-01-4.433e-02i, |S[2][1]| = -1.121e+01, arg(S[2][1]) = -9.269e+00
It 22/300: ω/2π = 7.953e+00 GHz (total elapsed time = 1.58e+02 s)
Calculating boundary modes at wave ports for ω/2π = 7.953e+00 GHz (1.333e-01)
Port 1, mode 1: kₙ = 5.601e+02-2.576e-02i m⁻¹
Port 2, mode 1: kₙ = 5.601e+02-2.576e-02i m⁻¹
Sol. ||E|| = 1.459747e+01
Field energy E (4.477e-04 J) + H (6.035e-04 J) = 1.051e-03 J
S[1][1] = -7.118e-01+1.209e-02i, |S[1][1]| = -2.952e+00, arg(S[1][1]) = +1.790e+02
S[2][1] = +2.710e-01-4.616e-02i, |S[2][1]| = -1.122e+01, arg(S[2][1]) = -9.666e+00
It 23/300: ω/2π = 8.284e+00 GHz (total elapsed time = 1.58e+02 s)
Calculating boundary modes at wave ports for ω/2π = 8.284e+00 GHz (1.389e-01)
Port 1, mode 1: kₙ = 5.834e+02-2.684e-02i m⁻¹
Port 2, mode 1: kₙ = 5.834e+02-2.683e-02i m⁻¹
Sol. ||E|| = 1.459528e+01
Field energy E (4.476e-04 J) + H (6.021e-04 J) = 1.050e-03 J
S[1][1] = -7.114e-01+1.252e-02i, |S[1][1]| = -2.956e+00, arg(S[1][1]) = +1.790e+02
S[2][1] = +2.703e-01-4.798e-02i, |S[2][1]| = -1.123e+01, arg(S[2][1]) = -1.006e+01
It 24/300: ω/2π = 8.615e+00 GHz (total elapsed time = 1.58e+02 s)
Calculating boundary modes at wave ports for ω/2π = 8.615e+00 GHz (1.445e-01)
Port 1, mode 1: kₙ = 6.067e+02-2.791e-02i m⁻¹
Port 2, mode 1: kₙ = 6.067e+02-2.791e-02i m⁻¹
Sol. ||E|| = 1.459301e+01
Field energy E (4.474e-04 J) + H (6.008e-04 J) = 1.048e-03 J
S[1][1] = -7.110e-01+1.294e-02i, |S[1][1]| = -2.961e+00, arg(S[1][1]) = +1.790e+02
S[2][1] = +2.697e-01-4.979e-02i, |S[2][1]| = -1.124e+01, arg(S[2][1]) = -1.046e+01
It 25/300: ω/2π = 8.946e+00 GHz (total elapsed time = 1.59e+02 s)
Calculating boundary modes at wave ports for ω/2π = 8.946e+00 GHz (1.500e-01)
Port 1, mode 1: kₙ = 6.301e+02-2.898e-02i m⁻¹
Port 2, mode 1: kₙ = 6.301e+02-2.898e-02i m⁻¹
Sol. ||E|| = 1.459065e+01
Field energy E (4.473e-04 J) + H (5.996e-04 J) = 1.047e-03 J
S[1][1] = -7.106e-01+1.336e-02i, |S[1][1]| = -2.966e+00, arg(S[1][1]) = +1.789e+02
S[2][1] = +2.690e-01-5.160e-02i, |S[2][1]| = -1.125e+01, arg(S[2][1]) = -1.086e+01
It 26/300: ω/2π = 9.278e+00 GHz (total elapsed time = 1.59e+02 s)
Calculating boundary modes at wave ports for ω/2π = 9.278e+00 GHz (1.556e-01)
Port 1, mode 1: kₙ = 6.534e+02-3.005e-02i m⁻¹
Port 2, mode 1: kₙ = 6.534e+02-3.005e-02i m⁻¹
Sol. ||E|| = 1.458821e+01
Field energy E (4.471e-04 J) + H (5.985e-04 J) = 1.046e-03 J
S[1][1] = -7.102e-01+1.378e-02i, |S[1][1]| = -2.970e+00, arg(S[1][1]) = +1.789e+02
S[2][1] = +2.682e-01-5.340e-02i, |S[2][1]| = -1.126e+01, arg(S[2][1]) = -1.126e+01
It 27/300: ω/2π = 9.609e+00 GHz (total elapsed time = 1.59e+02 s)
Calculating boundary modes at wave ports for ω/2π = 9.609e+00 GHz (1.611e-01)
Port 1, mode 1: kₙ = 6.767e+02-3.113e-02i m⁻¹
Port 2, mode 1: kₙ = 6.767e+02-3.112e-02i m⁻¹
Sol. ||E|| = 1.458569e+01
Field energy E (4.469e-04 J) + H (5.973e-04 J) = 1.044e-03 J
S[1][1] = -7.098e-01+1.420e-02i, |S[1][1]| = -2.975e+00, arg(S[1][1]) = +1.789e+02
S[2][1] = +2.675e-01-5.519e-02i, |S[2][1]| = -1.127e+01, arg(S[2][1]) = -1.166e+01
It 28/300: ω/2π = 9.940e+00 GHz (total elapsed time = 1.60e+02 s)
Calculating boundary modes at wave ports for ω/2π = 9.940e+00 GHz (1.667e-01)
Port 1, mode 1: kₙ = 7.000e+02-3.220e-02i m⁻¹
Port 2, mode 1: kₙ = 7.000e+02-3.220e-02i m⁻¹
Sol. ||E|| = 1.458309e+01
Field energy E (4.468e-04 J) + H (5.963e-04 J) = 1.043e-03 J
S[1][1] = -7.094e-01+1.461e-02i, |S[1][1]| = -2.980e+00, arg(S[1][1]) = +1.788e+02
S[2][1] = +2.667e-01-5.697e-02i, |S[2][1]| = -1.129e+01, arg(S[2][1]) = -1.206e+01
It 29/300: ω/2π = 1.027e+01 GHz (total elapsed time = 1.60e+02 s)
Calculating boundary modes at wave ports for ω/2π = 1.027e+01 GHz (1.722e-01)
Port 1, mode 1: kₙ = 7.233e+02-3.327e-02i m⁻¹
Port 2, mode 1: kₙ = 7.233e+02-3.327e-02i m⁻¹
Sol. ||E|| = 1.458041e+01
Field energy E (4.466e-04 J) + H (5.952e-04 J) = 1.042e-03 J
S[1][1] = -7.090e-01+1.502e-02i, |S[1][1]| = -2.985e+00, arg(S[1][1]) = +1.788e+02
S[2][1] = +2.659e-01-5.874e-02i, |S[2][1]| = -1.130e+01, arg(S[2][1]) = -1.246e+01
It 30/300: ω/2π = 1.060e+01 GHz (total elapsed time = 1.60e+02 s)
Calculating boundary modes at wave ports for ω/2π = 1.060e+01 GHz (1.778e-01)
Port 1, mode 1: kₙ = 7.466e+02-3.435e-02i m⁻¹
Port 2, mode 1: kₙ = 7.466e+02-3.434e-02i m⁻¹
Sol. ||E|| = 1.457767e+01
Field energy E (4.464e-04 J) + H (5.943e-04 J) = 1.041e-03 J
S[1][1] = -7.085e-01+1.542e-02i, |S[1][1]| = -2.991e+00, arg(S[1][1]) = +1.788e+02
S[2][1] = +2.651e-01-6.051e-02i, |S[2][1]| = -1.131e+01, arg(S[2][1]) = -1.286e+01
It 31/300: ω/2π = 1.093e+01 GHz (total elapsed time = 1.60e+02 s)
Calculating boundary modes at wave ports for ω/2π = 1.093e+01 GHz (1.833e-01)
Port 1, mode 1: kₙ = 7.700e+02-3.542e-02i m⁻¹
Port 2, mode 1: kₙ = 7.700e+02-3.542e-02i m⁻¹
Sol. ||E|| = 1.457486e+01
Field energy E (4.463e-04 J) + H (5.933e-04 J) = 1.040e-03 J
S[1][1] = -7.081e-01+1.582e-02i, |S[1][1]| = -2.996e+00, arg(S[1][1]) = +1.787e+02
S[2][1] = +2.643e-01-6.226e-02i, |S[2][1]| = -1.132e+01, arg(S[2][1]) = -1.326e+01
It 32/300: ω/2π = 1.126e+01 GHz (total elapsed time = 1.61e+02 s)
Calculating boundary modes at wave ports for ω/2π = 1.126e+01 GHz (1.889e-01)
Port 1, mode 1: kₙ = 7.933e+02-3.649e-02i m⁻¹
Port 2, mode 1: kₙ = 7.933e+02-3.649e-02i m⁻¹
Sol. ||E|| = 1.457198e+01
Field energy E (4.461e-04 J) + H (5.924e-04 J) = 1.038e-03 J
S[1][1] = -7.076e-01+1.622e-02i, |S[1][1]| = -3.001e+00, arg(S[1][1]) = +1.787e+02
S[2][1] = +2.634e-01-6.401e-02i, |S[2][1]| = -1.134e+01, arg(S[2][1]) = -1.366e+01
It 33/300: ω/2π = 1.160e+01 GHz (total elapsed time = 1.61e+02 s)
Calculating boundary modes at wave ports for ω/2π = 1.160e+01 GHz (1.944e-01)
Port 1, mode 1: kₙ = 8.166e+02-3.756e-02i m⁻¹
Port 2, mode 1: kₙ = 8.166e+02-3.756e-02i m⁻¹
Sol. ||E|| = 1.456905e+01
Field energy E (4.459e-04 J) + H (5.915e-04 J) = 1.037e-03 J
S[1][1] = -7.072e-01+1.662e-02i, |S[1][1]| = -3.007e+00, arg(S[1][1]) = +1.787e+02
S[2][1] = +2.625e-01-6.575e-02i, |S[2][1]| = -1.135e+01, arg(S[2][1]) = -1.406e+01
It 34/300: ω/2π = 1.193e+01 GHz (total elapsed time = 1.61e+02 s)
Calculating boundary modes at wave ports for ω/2π = 1.193e+01 GHz (2.000e-01)
Port 1, mode 1: kₙ = 8.399e+02-3.864e-02i m⁻¹
Port 2, mode 1: kₙ = 8.399e+02-3.863e-02i m⁻¹
Sol. ||E|| = 1.456605e+01
Field energy E (4.457e-04 J) + H (5.906e-04 J) = 1.036e-03 J
S[1][1] = -7.067e-01+1.701e-02i, |S[1][1]| = -3.013e+00, arg(S[1][1]) = +1.786e+02
S[2][1] = +2.616e-01-6.749e-02i, |S[2][1]| = -1.137e+01, arg(S[2][1]) = -1.446e+01
It 35/300: ω/2π = 1.226e+01 GHz (total elapsed time = 1.62e+02 s)
Calculating boundary modes at wave ports for ω/2π = 1.226e+01 GHz (2.055e-01)
Port 1, mode 1: kₙ = 8.632e+02-3.971e-02i m⁻¹
Port 2, mode 1: kₙ = 8.632e+02-3.971e-02i m⁻¹
Sol. ||E|| = 1.456300e+01
Field energy E (4.455e-04 J) + H (5.898e-04 J) = 1.035e-03 J
S[1][1] = -7.062e-01+1.741e-02i, |S[1][1]| = -3.018e+00, arg(S[1][1]) = +1.786e+02
S[2][1] = +2.607e-01-6.921e-02i, |S[2][1]| = -1.138e+01, arg(S[2][1]) = -1.487e+01
It 36/300: ω/2π = 1.259e+01 GHz (total elapsed time = 1.62e+02 s)
Calculating boundary modes at wave ports for ω/2π = 1.259e+01 GHz (2.111e-01)
Port 1, mode 1: kₙ = 8.865e+02-4.078e-02i m⁻¹
Port 2, mode 1: kₙ = 8.865e+02-4.078e-02i m⁻¹
Sol. ||E|| = 1.455989e+01
Field energy E (4.453e-04 J) + H (5.890e-04 J) = 1.034e-03 J
S[1][1] = -7.057e-01+1.779e-02i, |S[1][1]| = -3.024e+00, arg(S[1][1]) = +1.786e+02
S[2][1] = +2.598e-01-7.092e-02i, |S[2][1]| = -1.140e+01, arg(S[2][1]) = -1.527e+01
It 37/300: ω/2π = 1.292e+01 GHz (total elapsed time = 1.62e+02 s)
Calculating boundary modes at wave ports for ω/2π = 1.292e+01 GHz (2.166e-01)
Port 1, mode 1: kₙ = 9.099e+02-4.185e-02i m⁻¹
Port 2, mode 1: kₙ = 9.099e+02-4.185e-02i m⁻¹
Sol. ||E|| = 1.455673e+01
Field energy E (4.451e-04 J) + H (5.882e-04 J) = 1.033e-03 J
S[1][1] = -7.053e-01+1.818e-02i, |S[1][1]| = -3.030e+00, arg(S[1][1]) = +1.785e+02
S[2][1] = +2.588e-01-7.263e-02i, |S[2][1]| = -1.141e+01, arg(S[2][1]) = -1.567e+01
It 38/300: ω/2π = 1.325e+01 GHz (total elapsed time = 1.62e+02 s)
Calculating boundary modes at wave ports for ω/2π = 1.325e+01 GHz (2.222e-01)
Port 1, mode 1: kₙ = 9.332e+02-4.293e-02i m⁻¹
Port 2, mode 1: kₙ = 9.332e+02-4.292e-02i m⁻¹
Sol. ||E|| = 1.455352e+01
Field energy E (4.449e-04 J) + H (5.874e-04 J) = 1.032e-03 J
S[1][1] = -7.047e-01+1.856e-02i, |S[1][1]| = -3.036e+00, arg(S[1][1]) = +1.785e+02
S[2][1] = +2.579e-01-7.433e-02i, |S[2][1]| = -1.143e+01, arg(S[2][1]) = -1.608e+01
It 39/300: ω/2π = 1.358e+01 GHz (total elapsed time = 1.63e+02 s)
Calculating boundary modes at wave ports for ω/2π = 1.358e+01 GHz (2.277e-01)
Port 1, mode 1: kₙ = 9.565e+02-4.400e-02i m⁻¹
Port 2, mode 1: kₙ = 9.565e+02-4.400e-02i m⁻¹
Sol. ||E|| = 1.455027e+01
Field energy E (4.447e-04 J) + H (5.867e-04 J) = 1.031e-03 J
S[1][1] = -7.042e-01+1.894e-02i, |S[1][1]| = -3.042e+00, arg(S[1][1]) = +1.785e+02
S[2][1] = +2.569e-01-7.601e-02i, |S[2][1]| = -1.144e+01, arg(S[2][1]) = -1.649e+01
It 40/300: ω/2π = 1.391e+01 GHz (total elapsed time = 1.63e+02 s)
Calculating boundary modes at wave ports for ω/2π = 1.391e+01 GHz (2.333e-01)
Port 1, mode 1: kₙ = 9.798e+02-4.507e-02i m⁻¹
Port 2, mode 1: kₙ = 9.798e+02-4.507e-02i m⁻¹
Sol. ||E|| = 1.454696e+01
Field energy E (4.445e-04 J) + H (5.859e-04 J) = 1.030e-03 J
S[1][1] = -7.037e-01+1.932e-02i, |S[1][1]| = -3.049e+00, arg(S[1][1]) = +1.784e+02
S[2][1] = +2.558e-01-7.769e-02i, |S[2][1]| = -1.146e+01, arg(S[2][1]) = -1.689e+01
It 41/300: ω/2π = 1.424e+01 GHz (total elapsed time = 1.63e+02 s)
Calculating boundary modes at wave ports for ω/2π = 1.424e+01 GHz (2.388e-01)
Port 1, mode 1: kₙ = 1.003e+03-4.614e-02i m⁻¹
Port 2, mode 1: kₙ = 1.003e+03-4.614e-02i m⁻¹
Sol. ||E|| = 1.454361e+01
Field energy E (4.443e-04 J) + H (5.852e-04 J) = 1.030e-03 J
S[1][1] = -7.032e-01+1.970e-02i, |S[1][1]| = -3.055e+00, arg(S[1][1]) = +1.784e+02
S[2][1] = +2.548e-01-7.936e-02i, |S[2][1]| = -1.147e+01, arg(S[2][1]) = -1.730e+01
It 42/300: ω/2π = 1.458e+01 GHz (total elapsed time = 1.64e+02 s)
Calculating boundary modes at wave ports for ω/2π = 1.458e+01 GHz (2.444e-01)
Port 1, mode 1: kₙ = 1.026e+03-4.722e-02i m⁻¹
Port 2, mode 1: kₙ = 1.026e+03-4.721e-02i m⁻¹
Sol. ||E|| = 1.454022e+01
Field energy E (4.441e-04 J) + H (5.845e-04 J) = 1.029e-03 J
S[1][1] = -7.027e-01+2.007e-02i, |S[1][1]| = -3.061e+00, arg(S[1][1]) = +1.784e+02
S[2][1] = +2.538e-01-8.102e-02i, |S[2][1]| = -1.149e+01, arg(S[2][1]) = -1.771e+01
It 43/300: ω/2π = 1.491e+01 GHz (total elapsed time = 1.64e+02 s)
Calculating boundary modes at wave ports for ω/2π = 1.491e+01 GHz (2.499e-01)
Port 1, mode 1: kₙ = 1.050e+03-4.829e-02i m⁻¹
Port 2, mode 1: kₙ = 1.050e+03-4.829e-02i m⁻¹
Sol. ||E|| = 1.453679e+01
Field energy E (4.439e-04 J) + H (5.838e-04 J) = 1.028e-03 J
S[1][1] = -7.021e-01+2.045e-02i, |S[1][1]| = -3.068e+00, arg(S[1][1]) = +1.783e+02
S[2][1] = +2.527e-01-8.267e-02i, |S[2][1]| = -1.151e+01, arg(S[2][1]) = -1.812e+01
It 44/300: ω/2π = 1.524e+01 GHz (total elapsed time = 1.64e+02 s)
Calculating boundary modes at wave ports for ω/2π = 1.524e+01 GHz (2.555e-01)
Port 1, mode 1: kₙ = 1.073e+03-4.936e-02i m⁻¹
Port 2, mode 1: kₙ = 1.073e+03-4.936e-02i m⁻¹
Sol. ||E|| = 1.453332e+01
Field energy E (4.437e-04 J) + H (5.831e-04 J) = 1.027e-03 J
S[1][1] = -7.016e-01+2.082e-02i, |S[1][1]| = -3.075e+00, arg(S[1][1]) = +1.783e+02
S[2][1] = +2.516e-01-8.431e-02i, |S[2][1]| = -1.152e+01, arg(S[2][1]) = -1.853e+01
It 45/300: ω/2π = 1.557e+01 GHz (total elapsed time = 1.64e+02 s)
Calculating boundary modes at wave ports for ω/2π = 1.557e+01 GHz (2.610e-01)
Port 1, mode 1: kₙ = 1.096e+03-5.043e-02i m⁻¹
Port 2, mode 1: kₙ = 1.096e+03-5.043e-02i m⁻¹
Sol. ||E|| = 1.452981e+01
Field energy E (4.435e-04 J) + H (5.825e-04 J) = 1.026e-03 J
S[1][1] = -7.010e-01+2.119e-02i, |S[1][1]| = -3.081e+00, arg(S[1][1]) = +1.783e+02
S[2][1] = +2.505e-01-8.595e-02i, |S[2][1]| = -1.154e+01, arg(S[2][1]) = -1.894e+01
It 46/300: ω/2π = 1.590e+01 GHz (total elapsed time = 1.65e+02 s)
Calculating boundary modes at wave ports for ω/2π = 1.590e+01 GHz (2.666e-01)
Port 1, mode 1: kₙ = 1.120e+03-5.151e-02i m⁻¹
Port 2, mode 1: kₙ = 1.120e+03-5.150e-02i m⁻¹
Sol. ||E|| = 1.452627e+01
Field energy E (4.433e-04 J) + H (5.818e-04 J) = 1.025e-03 J
S[1][1] = -7.005e-01+2.155e-02i, |S[1][1]| = -3.088e+00, arg(S[1][1]) = +1.782e+02
S[2][1] = +2.494e-01-8.757e-02i, |S[2][1]| = -1.156e+01, arg(S[2][1]) = -1.935e+01
It 47/300: ω/2π = 1.623e+01 GHz (total elapsed time = 1.65e+02 s)
Calculating boundary modes at wave ports for ω/2π = 1.623e+01 GHz (2.721e-01)
Port 1, mode 1: kₙ = 1.143e+03-5.258e-02i m⁻¹
Port 2, mode 1: kₙ = 1.143e+03-5.258e-02i m⁻¹
Sol. ||E|| = 1.452269e+01
Field energy E (4.430e-04 J) + H (5.812e-04 J) = 1.024e-03 J
S[1][1] = -6.999e-01+2.192e-02i, |S[1][1]| = -3.095e+00, arg(S[1][1]) = +1.782e+02
S[2][1] = +2.482e-01-8.918e-02i, |S[2][1]| = -1.158e+01, arg(S[2][1]) = -1.976e+01
It 48/300: ω/2π = 1.656e+01 GHz (total elapsed time = 1.65e+02 s)
Calculating boundary modes at wave ports for ω/2π = 1.656e+01 GHz (2.777e-01)
Port 1, mode 1: kₙ = 1.166e+03-5.365e-02i m⁻¹
Port 2, mode 1: kₙ = 1.166e+03-5.365e-02i m⁻¹
Sol. ||E|| = 1.451908e+01
Field energy E (4.428e-04 J) + H (5.806e-04 J) = 1.023e-03 J
S[1][1] = -6.993e-01+2.228e-02i, |S[1][1]| = -3.102e+00, arg(S[1][1]) = +1.782e+02
S[2][1] = +2.471e-01-9.079e-02i, |S[2][1]| = -1.159e+01, arg(S[2][1]) = -2.018e+01
It 49/300: ω/2π = 1.689e+01 GHz (total elapsed time = 1.66e+02 s)
Calculating boundary modes at wave ports for ω/2π = 1.689e+01 GHz (2.832e-01)
Port 1, mode 1: kₙ = 1.190e+03-5.472e-02i m⁻¹
Port 2, mode 1: kₙ = 1.190e+03-5.472e-02i m⁻¹
Sol. ||E|| = 1.451544e+01
Field energy E (4.426e-04 J) + H (5.799e-04 J) = 1.023e-03 J
S[1][1] = -6.988e-01+2.265e-02i, |S[1][1]| = -3.109e+00, arg(S[1][1]) = +1.781e+02
S[2][1] = +2.459e-01-9.238e-02i, |S[2][1]| = -1.161e+01, arg(S[2][1]) = -2.059e+01
It 50/300: ω/2π = 1.722e+01 GHz (total elapsed time = 1.66e+02 s)
Calculating boundary modes at wave ports for ω/2π = 1.722e+01 GHz (2.888e-01)
Port 1, mode 1: kₙ = 1.213e+03-5.580e-02i m⁻¹
Port 2, mode 1: kₙ = 1.213e+03-5.579e-02i m⁻¹
Sol. ||E|| = 1.451177e+01
Field energy E (4.424e-04 J) + H (5.794e-04 J) = 1.022e-03 J
S[1][1] = -6.982e-01+2.301e-02i, |S[1][1]| = -3.116e+00, arg(S[1][1]) = +1.781e+02
S[2][1] = +2.447e-01-9.396e-02i, |S[2][1]| = -1.163e+01, arg(S[2][1]) = -2.101e+01
It 51/300: ω/2π = 1.756e+01 GHz (total elapsed time = 1.66e+02 s)
Calculating boundary modes at wave ports for ω/2π = 1.756e+01 GHz (2.943e-01)
Port 1, mode 1: kₙ = 1.236e+03-5.687e-02i m⁻¹
Port 2, mode 1: kₙ = 1.236e+03-5.687e-02i m⁻¹
Sol. ||E|| = 1.450807e+01
Field energy E (4.421e-04 J) + H (5.788e-04 J) = 1.021e-03 J
S[1][1] = -6.976e-01+2.337e-02i, |S[1][1]| = -3.123e+00, arg(S[1][1]) = +1.781e+02
S[2][1] = +2.435e-01-9.554e-02i, |S[2][1]| = -1.165e+01, arg(S[2][1]) = -2.143e+01
It 52/300: ω/2π = 1.789e+01 GHz (total elapsed time = 1.66e+02 s)
Calculating boundary modes at wave ports for ω/2π = 1.789e+01 GHz (2.999e-01)
Port 1, mode 1: kₙ = 1.260e+03-5.794e-02i m⁻¹
Port 2, mode 1: kₙ = 1.260e+03-5.794e-02i m⁻¹
Sol. ||E|| = 1.450434e+01
Field energy E (4.419e-04 J) + H (5.782e-04 J) = 1.020e-03 J
S[1][1] = -6.970e-01+2.372e-02i, |S[1][1]| = -3.130e+00, arg(S[1][1]) = +1.781e+02
S[2][1] = +2.422e-01-9.710e-02i, |S[2][1]| = -1.167e+01, arg(S[2][1]) = -2.184e+01
It 53/300: ω/2π = 1.822e+01 GHz (total elapsed time = 1.67e+02 s)
Calculating boundary modes at wave ports for ω/2π = 1.822e+01 GHz (3.054e-01)
Port 1, mode 1: kₙ = 1.283e+03-5.901e-02i m⁻¹
Port 2, mode 1: kₙ = 1.283e+03-5.901e-02i m⁻¹
Sol. ||E|| = 1.450059e+01
Field energy E (4.417e-04 J) + H (5.776e-04 J) = 1.019e-03 J
S[1][1] = -6.964e-01+2.408e-02i, |S[1][1]| = -3.138e+00, arg(S[1][1]) = +1.780e+02
S[2][1] = +2.410e-01-9.865e-02i, |S[2][1]| = -1.169e+01, arg(S[2][1]) = -2.226e+01
It 54/300: ω/2π = 1.855e+01 GHz (total elapsed time = 1.67e+02 s)
Calculating boundary modes at wave ports for ω/2π = 1.855e+01 GHz (3.110e-01)
Port 1, mode 1: kₙ = 1.306e+03-6.009e-02i m⁻¹
Port 2, mode 1: kₙ = 1.306e+03-6.008e-02i m⁻¹
Sol. ||E|| = 1.449682e+01
Field energy E (4.415e-04 J) + H (5.771e-04 J) = 1.019e-03 J
S[1][1] = -6.958e-01+2.444e-02i, |S[1][1]| = -3.145e+00, arg(S[1][1]) = +1.780e+02
S[2][1] = +2.397e-01-1.002e-01i, |S[2][1]| = -1.171e+01, arg(S[2][1]) = -2.268e+01
It 55/300: ω/2π = 1.888e+01 GHz (total elapsed time = 1.67e+02 s)
Calculating boundary modes at wave ports for ω/2π = 1.888e+01 GHz (3.165e-01)
Port 1, mode 1: kₙ = 1.330e+03-6.116e-02i m⁻¹
Port 2, mode 1: kₙ = 1.330e+03-6.116e-02i m⁻¹
Sol. ||E|| = 1.449302e+01
Field energy E (4.412e-04 J) + H (5.765e-04 J) = 1.018e-03 J
S[1][1] = -6.952e-01+2.479e-02i, |S[1][1]| = -3.153e+00, arg(S[1][1]) = +1.780e+02
S[2][1] = +2.384e-01-1.017e-01i, |S[2][1]| = -1.173e+01, arg(S[2][1]) = -2.311e+01
It 56/300: ω/2π = 1.921e+01 GHz (total elapsed time = 1.67e+02 s)
Calculating boundary modes at wave ports for ω/2π = 1.921e+01 GHz (3.221e-01)
Port 1, mode 1: kₙ = 1.353e+03-6.223e-02i m⁻¹
Port 2, mode 1: kₙ = 1.353e+03-6.223e-02i m⁻¹
Sol. ||E|| = 1.448921e+01
Field energy E (4.410e-04 J) + H (5.760e-04 J) = 1.017e-03 J
S[1][1] = -6.945e-01+2.514e-02i, |S[1][1]| = -3.160e+00, arg(S[1][1]) = +1.779e+02
S[2][1] = +2.371e-01-1.033e-01i, |S[2][1]| = -1.175e+01, arg(S[2][1]) = -2.353e+01
It 57/300: ω/2π = 1.954e+01 GHz (total elapsed time = 1.68e+02 s)
Calculating boundary modes at wave ports for ω/2π = 1.954e+01 GHz (3.277e-01)
Port 1, mode 1: kₙ = 1.376e+03-6.330e-02i m⁻¹
Port 2, mode 1: kₙ = 1.376e+03-6.330e-02i m⁻¹
Sol. ||E|| = 1.448537e+01
Field energy E (4.408e-04 J) + H (5.755e-04 J) = 1.016e-03 J
S[1][1] = -6.939e-01+2.550e-02i, |S[1][1]| = -3.168e+00, arg(S[1][1]) = +1.779e+02
S[2][1] = +2.358e-01-1.048e-01i, |S[2][1]| = -1.177e+01, arg(S[2][1]) = -2.395e+01
It 58/300: ω/2π = 1.987e+01 GHz (total elapsed time = 1.68e+02 s)
Calculating boundary modes at wave ports for ω/2π = 1.987e+01 GHz (3.332e-01)
Port 1, mode 1: kₙ = 1.400e+03-6.438e-02i m⁻¹
Port 2, mode 1: kₙ = 1.400e+03-6.437e-02i m⁻¹
Sol. ||E|| = 1.448152e+01
Field energy E (4.405e-04 J) + H (5.750e-04 J) = 1.016e-03 J
S[1][1] = -6.933e-01+2.585e-02i, |S[1][1]| = -3.176e+00, arg(S[1][1]) = +1.779e+02
S[2][1] = +2.345e-01-1.063e-01i, |S[2][1]| = -1.179e+01, arg(S[2][1]) = -2.438e+01
It 59/300: ω/2π = 2.020e+01 GHz (total elapsed time = 1.68e+02 s)
Calculating boundary modes at wave ports for ω/2π = 2.020e+01 GHz (3.388e-01)
Port 1, mode 1: kₙ = 1.423e+03-6.545e-02i m⁻¹
Port 2, mode 1: kₙ = 1.423e+03-6.545e-02i m⁻¹
Sol. ||E|| = 1.447766e+01
Field energy E (4.403e-04 J) + H (5.745e-04 J) = 1.015e-03 J
S[1][1] = -6.927e-01+2.620e-02i, |S[1][1]| = -3.183e+00, arg(S[1][1]) = +1.778e+02
S[2][1] = +2.332e-01-1.078e-01i, |S[2][1]| = -1.181e+01, arg(S[2][1]) = -2.481e+01
It 60/300: ω/2π = 2.054e+01 GHz (total elapsed time = 1.69e+02 s)
Calculating boundary modes at wave ports for ω/2π = 2.054e+01 GHz (3.443e-01)
Port 1, mode 1: kₙ = 1.446e+03-6.652e-02i m⁻¹
Port 2, mode 1: kₙ = 1.446e+03-6.652e-02i m⁻¹
Sol. ||E|| = 1.447378e+01
Field energy E (4.400e-04 J) + H (5.740e-04 J) = 1.014e-03 J
S[1][1] = -6.920e-01+2.655e-02i, |S[1][1]| = -3.191e+00, arg(S[1][1]) = +1.778e+02
S[2][1] = +2.318e-01-1.092e-01i, |S[2][1]| = -1.183e+01, arg(S[2][1]) = -2.523e+01
It 61/300: ω/2π = 2.087e+01 GHz (total elapsed time = 1.69e+02 s)
Calculating boundary modes at wave ports for ω/2π = 2.087e+01 GHz (3.499e-01)
Port 1, mode 1: kₙ = 1.469e+03-6.760e-02i m⁻¹
Port 2, mode 1: kₙ = 1.469e+03-6.759e-02i m⁻¹
Sol. ||E|| = 1.446988e+01
Field energy E (4.398e-04 J) + H (5.735e-04 J) = 1.013e-03 J
S[1][1] = -6.914e-01+2.690e-02i, |S[1][1]| = -3.199e+00, arg(S[1][1]) = +1.778e+02
S[2][1] = +2.304e-01-1.107e-01i, |S[2][1]| = -1.185e+01, arg(S[2][1]) = -2.566e+01
It 62/300: ω/2π = 2.120e+01 GHz (total elapsed time = 1.69e+02 s)
Calculating boundary modes at wave ports for ω/2π = 2.120e+01 GHz (3.554e-01)
Port 1, mode 1: kₙ = 1.493e+03-6.867e-02i m⁻¹
Port 2, mode 1: kₙ = 1.493e+03-6.866e-02i m⁻¹
Sol. ||E|| = 1.446598e+01
Field energy E (4.396e-04 J) + H (5.731e-04 J) = 1.013e-03 J
S[1][1] = -6.907e-01+2.725e-02i, |S[1][1]| = -3.207e+00, arg(S[1][1]) = +1.777e+02
S[2][1] = +2.290e-01-1.122e-01i, |S[2][1]| = -1.187e+01, arg(S[2][1]) = -2.609e+01
It 63/300: ω/2π = 2.153e+01 GHz (total elapsed time = 1.69e+02 s)
Calculating boundary modes at wave ports for ω/2π = 2.153e+01 GHz (3.610e-01)
Port 1, mode 1: kₙ = 1.516e+03-6.974e-02i m⁻¹
Port 2, mode 1: kₙ = 1.516e+03-6.974e-02i m⁻¹
Sol. ||E|| = 1.446207e+01
Field energy E (4.393e-04 J) + H (5.726e-04 J) = 1.012e-03 J
S[1][1] = -6.901e-01+2.759e-02i, |S[1][1]| = -3.215e+00, arg(S[1][1]) = +1.777e+02
S[2][1] = +2.276e-01-1.136e-01i, |S[2][1]| = -1.189e+01, arg(S[2][1]) = -2.653e+01
It 64/300: ω/2π = 2.186e+01 GHz (total elapsed time = 1.70e+02 s)
Calculating boundary modes at wave ports for ω/2π = 2.186e+01 GHz (3.665e-01)
Port 1, mode 1: kₙ = 1.539e+03-7.081e-02i m⁻¹
Port 2, mode 1: kₙ = 1.539e+03-7.081e-02i m⁻¹
Sol. ||E|| = 1.445814e+01
Field energy E (4.391e-04 J) + H (5.721e-04 J) = 1.011e-03 J
S[1][1] = -6.894e-01+2.794e-02i, |S[1][1]| = -3.223e+00, arg(S[1][1]) = +1.777e+02
S[2][1] = +2.262e-01-1.151e-01i, |S[2][1]| = -1.191e+01, arg(S[2][1]) = -2.696e+01
It 65/300: ω/2π = 2.219e+01 GHz (total elapsed time = 1.70e+02 s)
Calculating boundary modes at wave ports for ω/2π = 2.219e+01 GHz (3.721e-01)
Port 1, mode 1: kₙ = 1.563e+03-7.189e-02i m⁻¹
Port 2, mode 1: kₙ = 1.563e+03-7.188e-02i m⁻¹
Sol. ||E|| = 1.445422e+01
Field energy E (4.388e-04 J) + H (5.717e-04 J) = 1.011e-03 J
S[1][1] = -6.888e-01+2.829e-02i, |S[1][1]| = -3.231e+00, arg(S[1][1]) = +1.776e+02
S[2][1] = +2.248e-01-1.165e-01i, |S[2][1]| = -1.193e+01, arg(S[2][1]) = -2.740e+01
It 66/300: ω/2π = 2.252e+01 GHz (total elapsed time = 1.70e+02 s)
Calculating boundary modes at wave ports for ω/2π = 2.252e+01 GHz (3.776e-01)
Port 1, mode 1: kₙ = 1.586e+03-7.296e-02i m⁻¹
Port 2, mode 1: kₙ = 1.586e+03-7.295e-02i m⁻¹
Sol. ||E|| = 1.445028e+01
Field energy E (4.386e-04 J) + H (5.713e-04 J) = 1.010e-03 J
S[1][1] = -6.881e-01+2.863e-02i, |S[1][1]| = -3.240e+00, arg(S[1][1]) = +1.776e+02
S[2][1] = +2.233e-01-1.179e-01i, |S[2][1]| = -1.195e+01, arg(S[2][1]) = -2.783e+01
It 67/300: ω/2π = 2.285e+01 GHz (total elapsed time = 1.71e+02 s)
Calculating boundary modes at wave ports for ω/2π = 2.285e+01 GHz (3.832e-01)
Port 1, mode 1: kₙ = 1.609e+03-7.403e-02i m⁻¹
Port 2, mode 1: kₙ = 1.609e+03-7.403e-02i m⁻¹
Sol. ||E|| = 1.444635e+01
Field energy E (4.384e-04 J) + H (5.708e-04 J) = 1.009e-03 J
S[1][1] = -6.874e-01+2.898e-02i, |S[1][1]| = -3.248e+00, arg(S[1][1]) = +1.776e+02
S[2][1] = +2.218e-01-1.193e-01i, |S[2][1]| = -1.198e+01, arg(S[2][1]) = -2.827e+01
It 68/300: ω/2π = 2.318e+01 GHz (total elapsed time = 1.71e+02 s)
Calculating boundary modes at wave ports for ω/2π = 2.318e+01 GHz (3.887e-01)
Port 1, mode 1: kₙ = 1.633e+03-7.510e-02i m⁻¹
Port 2, mode 1: kₙ = 1.633e+03-7.510e-02i m⁻¹
Sol. ||E|| = 1.444241e+01
Field energy E (4.381e-04 J) + H (5.704e-04 J) = 1.009e-03 J
S[1][1] = -6.867e-01+2.932e-02i, |S[1][1]| = -3.256e+00, arg(S[1][1]) = +1.776e+02
S[2][1] = +2.204e-01-1.207e-01i, |S[2][1]| = -1.200e+01, arg(S[2][1]) = -2.871e+01
It 69/300: ω/2π = 2.352e+01 GHz (total elapsed time = 1.71e+02 s)
Calculating boundary modes at wave ports for ω/2π = 2.352e+01 GHz (3.943e-01)
Port 1, mode 1: kₙ = 1.656e+03-7.618e-02i m⁻¹
Port 2, mode 1: kₙ = 1.656e+03-7.617e-02i m⁻¹
Sol. ||E|| = 1.443847e+01
Field energy E (4.379e-04 J) + H (5.700e-04 J) = 1.008e-03 J
S[1][1] = -6.861e-01+2.966e-02i, |S[1][1]| = -3.265e+00, arg(S[1][1]) = +1.775e+02
S[2][1] = +2.189e-01-1.221e-01i, |S[2][1]| = -1.202e+01, arg(S[2][1]) = -2.915e+01
It 70/300: ω/2π = 2.385e+01 GHz (total elapsed time = 1.71e+02 s)
Calculating boundary modes at wave ports for ω/2π = 2.385e+01 GHz (3.998e-01)
Port 1, mode 1: kₙ = 1.679e+03-7.725e-02i m⁻¹
Port 2, mode 1: kₙ = 1.679e+03-7.724e-02i m⁻¹
Sol. ||E|| = 1.443453e+01
Field energy E (4.376e-04 J) + H (5.696e-04 J) = 1.007e-03 J
S[1][1] = -6.854e-01+3.001e-02i, |S[1][1]| = -3.273e+00, arg(S[1][1]) = +1.775e+02
S[2][1] = +2.174e-01-1.234e-01i, |S[2][1]| = -1.204e+01, arg(S[2][1]) = -2.959e+01
It 71/300: ω/2π = 2.418e+01 GHz (total elapsed time = 1.72e+02 s)
Calculating boundary modes at wave ports for ω/2π = 2.418e+01 GHz (4.054e-01)
Port 1, mode 1: kₙ = 1.703e+03-7.832e-02i m⁻¹
Port 2, mode 1: kₙ = 1.703e+03-7.832e-02i m⁻¹
Sol. ||E|| = 1.443059e+01
Field energy E (4.374e-04 J) + H (5.692e-04 J) = 1.007e-03 J
S[1][1] = -6.847e-01+3.035e-02i, |S[1][1]| = -3.282e+00, arg(S[1][1]) = +1.775e+02
S[2][1] = +2.158e-01-1.248e-01i, |S[2][1]| = -1.206e+01, arg(S[2][1]) = -3.004e+01
It 72/300: ω/2π = 2.451e+01 GHz (total elapsed time = 1.72e+02 s)
Calculating boundary modes at wave ports for ω/2π = 2.451e+01 GHz (4.109e-01)
Port 1, mode 1: kₙ = 1.726e+03-7.939e-02i m⁻¹
Port 2, mode 1: kₙ = 1.726e+03-7.939e-02i m⁻¹
Sol. ||E|| = 1.442666e+01
Field energy E (4.371e-04 J) + H (5.689e-04 J) = 1.006e-03 J
S[1][1] = -6.840e-01+3.069e-02i, |S[1][1]| = -3.290e+00, arg(S[1][1]) = +1.774e+02
S[2][1] = +2.143e-01-1.261e-01i, |S[2][1]| = -1.209e+01, arg(S[2][1]) = -3.048e+01
It 73/300: ω/2π = 2.484e+01 GHz (total elapsed time = 1.72e+02 s)
Calculating boundary modes at wave ports for ω/2π = 2.484e+01 GHz (4.165e-01)
Port 1, mode 1: kₙ = 1.749e+03-8.047e-02i m⁻¹
Port 2, mode 1: kₙ = 1.749e+03-8.046e-02i m⁻¹
Sol. ||E|| = 1.442273e+01
Field energy E (4.369e-04 J) + H (5.685e-04 J) = 1.005e-03 J
S[1][1] = -6.833e-01+3.103e-02i, |S[1][1]| = -3.299e+00, arg(S[1][1]) = +1.774e+02
S[2][1] = +2.128e-01-1.275e-01i, |S[2][1]| = -1.211e+01, arg(S[2][1]) = -3.093e+01
It 74/300: ω/2π = 2.517e+01 GHz (total elapsed time = 1.72e+02 s)
Calculating boundary modes at wave ports for ω/2π = 2.517e+01 GHz (4.220e-01)
Port 1, mode 1: kₙ = 1.773e+03-8.154e-02i m⁻¹
Port 2, mode 1: kₙ = 1.773e+03-8.153e-02i m⁻¹
Sol. ||E|| = 1.441881e+01
Field energy E (4.367e-04 J) + H (5.681e-04 J) = 1.005e-03 J
S[1][1] = -6.826e-01+3.138e-02i, |S[1][1]| = -3.308e+00, arg(S[1][1]) = +1.774e+02
S[2][1] = +2.112e-01-1.288e-01i, |S[2][1]| = -1.213e+01, arg(S[2][1]) = -3.138e+01
It 75/300: ω/2π = 2.550e+01 GHz (total elapsed time = 1.73e+02 s)
Calculating boundary modes at wave ports for ω/2π = 2.550e+01 GHz (4.276e-01)
Port 1, mode 1: kₙ = 1.796e+03-8.261e-02i m⁻¹
Port 2, mode 1: kₙ = 1.796e+03-8.260e-02i m⁻¹
Sol. ||E|| = 1.441490e+01
Field energy E (4.364e-04 J) + H (5.678e-04 J) = 1.004e-03 J
S[1][1] = -6.819e-01+3.172e-02i, |S[1][1]| = -3.316e+00, arg(S[1][1]) = +1.773e+02
S[2][1] = +2.096e-01-1.301e-01i, |S[2][1]| = -1.216e+01, arg(S[2][1]) = -3.183e+01
It 76/300: ω/2π = 2.583e+01 GHz (total elapsed time = 1.73e+02 s)
Calculating boundary modes at wave ports for ω/2π = 2.583e+01 GHz (4.331e-01)
Port 1, mode 1: kₙ = 1.819e+03-8.368e-02i m⁻¹
Port 2, mode 1: kₙ = 1.819e+03-8.368e-02i m⁻¹
Sol. ||E|| = 1.441099e+01
Field energy E (4.362e-04 J) + H (5.674e-04 J) = 1.004e-03 J
S[1][1] = -6.812e-01+3.206e-02i, |S[1][1]| = -3.325e+00, arg(S[1][1]) = +1.773e+02
S[2][1] = +2.080e-01-1.314e-01i, |S[2][1]| = -1.218e+01, arg(S[2][1]) = -3.228e+01
It 77/300: ω/2π = 2.616e+01 GHz (total elapsed time = 1.73e+02 s)
Calculating boundary modes at wave ports for ω/2π = 2.616e+01 GHz (4.387e-01)
Port 1, mode 1: kₙ = 1.843e+03-8.476e-02i m⁻¹
Port 2, mode 1: kₙ = 1.843e+03-8.475e-02i m⁻¹
Sol. ||E|| = 1.440710e+01
Field energy E (4.359e-04 J) + H (5.671e-04 J) = 1.003e-03 J
S[1][1] = -6.805e-01+3.240e-02i, |S[1][1]| = -3.334e+00, arg(S[1][1]) = +1.773e+02
S[2][1] = +2.064e-01-1.327e-01i, |S[2][1]| = -1.220e+01, arg(S[2][1]) = -3.273e+01
It 78/300: ω/2π = 2.649e+01 GHz (total elapsed time = 1.74e+02 s)
Calculating boundary modes at wave ports for ω/2π = 2.649e+01 GHz (4.442e-01)
Port 1, mode 1: kₙ = 1.866e+03-8.583e-02i m⁻¹
Port 2, mode 1: kₙ = 1.866e+03-8.582e-02i m⁻¹
Sol. ||E|| = 1.440322e+01
Field energy E (4.357e-04 J) + H (5.667e-04 J) = 1.002e-03 J
S[1][1] = -6.798e-01+3.273e-02i, |S[1][1]| = -3.343e+00, arg(S[1][1]) = +1.772e+02
S[2][1] = +2.048e-01-1.340e-01i, |S[2][1]| = -1.223e+01, arg(S[2][1]) = -3.319e+01
It 79/300: ω/2π = 2.683e+01 GHz (total elapsed time = 1.74e+02 s)
Calculating boundary modes at wave ports for ω/2π = 2.683e+01 GHz (4.498e-01)
Port 1, mode 1: kₙ = 1.889e+03-8.690e-02i m⁻¹
Port 2, mode 1: kₙ = 1.889e+03-8.689e-02i m⁻¹
Sol. ||E|| = 1.439935e+01
Field energy E (4.355e-04 J) + H (5.664e-04 J) = 1.002e-03 J
S[1][1] = -6.790e-01+3.307e-02i, |S[1][1]| = -3.352e+00, arg(S[1][1]) = +1.772e+02
S[2][1] = +2.032e-01-1.352e-01i, |S[2][1]| = -1.225e+01, arg(S[2][1]) = -3.364e+01
It 80/300: ω/2π = 2.716e+01 GHz (total elapsed time = 1.74e+02 s)
Calculating boundary modes at wave ports for ω/2π = 2.716e+01 GHz (4.553e-01)
Port 1, mode 1: kₙ = 1.913e+03-8.797e-02i m⁻¹
Port 2, mode 1: kₙ = 1.913e+03-8.797e-02i m⁻¹
Sol. ||E|| = 1.439550e+01
Field energy E (4.352e-04 J) + H (5.661e-04 J) = 1.001e-03 J
S[1][1] = -6.783e-01+3.341e-02i, |S[1][1]| = -3.361e+00, arg(S[1][1]) = +1.772e+02
S[2][1] = +2.016e-01-1.365e-01i, |S[2][1]| = -1.227e+01, arg(S[2][1]) = -3.410e+01
It 81/300: ω/2π = 2.749e+01 GHz (total elapsed time = 1.74e+02 s)
Calculating boundary modes at wave ports for ω/2π = 2.749e+01 GHz (4.609e-01)
Port 1, mode 1: kₙ = 1.936e+03-8.905e-02i m⁻¹
Port 2, mode 1: kₙ = 1.936e+03-8.904e-02i m⁻¹
Sol. ||E|| = 1.439166e+01
Field energy E (4.350e-04 J) + H (5.657e-04 J) = 1.001e-03 J
S[1][1] = -6.776e-01+3.375e-02i, |S[1][1]| = -3.370e+00, arg(S[1][1]) = +1.771e+02
S[2][1] = +1.999e-01-1.377e-01i, |S[2][1]| = -1.230e+01, arg(S[2][1]) = -3.456e+01
It 82/300: ω/2π = 2.782e+01 GHz (total elapsed time = 1.75e+02 s)
Calculating boundary modes at wave ports for ω/2π = 2.782e+01 GHz (4.664e-01)
Port 1, mode 1: kₙ = 1.959e+03-9.012e-02i m⁻¹
Port 2, mode 1: kₙ = 1.959e+03-9.011e-02i m⁻¹
Sol. ||E|| = 1.438784e+01
Field energy E (4.348e-04 J) + H (5.654e-04 J) = 1.000e-03 J
S[1][1] = -6.769e-01+3.409e-02i, |S[1][1]| = -3.379e+00, arg(S[1][1]) = +1.771e+02
S[2][1] = +1.983e-01-1.389e-01i, |S[2][1]| = -1.232e+01, arg(S[2][1]) = -3.502e+01
It 83/300: ω/2π = 2.815e+01 GHz (total elapsed time = 1.75e+02 s)
Calculating boundary modes at wave ports for ω/2π = 2.815e+01 GHz (4.720e-01)
Port 1, mode 1: kₙ = 1.982e+03-9.119e-02i m⁻¹
Port 2, mode 1: kₙ = 1.982e+03-9.118e-02i m⁻¹
Sol. ||E|| = 1.438404e+01
Field energy E (4.345e-04 J) + H (5.651e-04 J) = 9.997e-04 J
S[1][1] = -6.761e-01+3.442e-02i, |S[1][1]| = -3.388e+00, arg(S[1][1]) = +1.771e+02
S[2][1] = +1.966e-01-1.401e-01i, |S[2][1]| = -1.234e+01, arg(S[2][1]) = -3.548e+01
It 84/300: ω/2π = 2.848e+01 GHz (total elapsed time = 1.75e+02 s)
Calculating boundary modes at wave ports for ω/2π = 2.848e+01 GHz (4.775e-01)
Port 1, mode 1: kₙ = 2.006e+03-9.226e-02i m⁻¹
Port 2, mode 1: kₙ = 2.006e+03-9.226e-02i m⁻¹
Sol. ||E|| = 1.438026e+01
Field energy E (4.343e-04 J) + H (5.648e-04 J) = 9.991e-04 J
S[1][1] = -6.754e-01+3.476e-02i, |S[1][1]| = -3.397e+00, arg(S[1][1]) = +1.771e+02
S[2][1] = +1.949e-01-1.413e-01i, |S[2][1]| = -1.237e+01, arg(S[2][1]) = -3.595e+01
It 85/300: ω/2π = 2.881e+01 GHz (total elapsed time = 1.75e+02 s)
Calculating boundary modes at wave ports for ω/2π = 2.881e+01 GHz (4.831e-01)
Port 1, mode 1: kₙ = 2.029e+03-9.334e-02i m⁻¹
Port 2, mode 1: kₙ = 2.029e+03-9.333e-02i m⁻¹
Sol. ||E|| = 1.437650e+01
Field energy E (4.341e-04 J) + H (5.645e-04 J) = 9.986e-04 J
S[1][1] = -6.747e-01+3.510e-02i, |S[1][1]| = -3.407e+00, arg(S[1][1]) = +1.770e+02
S[2][1] = +1.932e-01-1.425e-01i, |S[2][1]| = -1.239e+01, arg(S[2][1]) = -3.641e+01
It 86/300: ω/2π = 2.914e+01 GHz (total elapsed time = 1.76e+02 s)
Calculating boundary modes at wave ports for ω/2π = 2.914e+01 GHz (4.886e-01)
Port 1, mode 1: kₙ = 2.052e+03-9.441e-02i m⁻¹
Port 2, mode 1: kₙ = 2.052e+03-9.440e-02i m⁻¹
Sol. ||E|| = 1.437276e+01
Field energy E (4.338e-04 J) + H (5.642e-04 J) = 9.981e-04 J
S[1][1] = -6.739e-01+3.543e-02i, |S[1][1]| = -3.416e+00, arg(S[1][1]) = +1.770e+02
S[2][1] = +1.915e-01-1.437e-01i, |S[2][1]| = -1.242e+01, arg(S[2][1]) = -3.688e+01
It 87/300: ω/2π = 2.947e+01 GHz (total elapsed time = 1.76e+02 s)
Calculating boundary modes at wave ports for ω/2π = 2.947e+01 GHz (4.942e-01)
Port 1, mode 1: kₙ = 2.076e+03-9.548e-02i m⁻¹
Port 2, mode 1: kₙ = 2.076e+03-9.547e-02i m⁻¹
Sol. ||E|| = 1.436904e+01
Field energy E (4.336e-04 J) + H (5.640e-04 J) = 9.976e-04 J
S[1][1] = -6.732e-01+3.577e-02i, |S[1][1]| = -3.425e+00, arg(S[1][1]) = +1.770e+02
S[2][1] = +1.898e-01-1.448e-01i, |S[2][1]| = -1.244e+01, arg(S[2][1]) = -3.735e+01
It 88/300: ω/2π = 2.981e+01 GHz (total elapsed time = 1.76e+02 s)
Calculating boundary modes at wave ports for ω/2π = 2.981e+01 GHz (4.998e-01)
Port 1, mode 1: kₙ = 2.099e+03-9.655e-02i m⁻¹
Port 2, mode 1: kₙ = 2.099e+03-9.655e-02i m⁻¹
Sol. ||E|| = 1.436536e+01
Field energy E (4.334e-04 J) + H (5.637e-04 J) = 9.971e-04 J
S[1][1] = -6.724e-01+3.610e-02i, |S[1][1]| = -3.434e+00, arg(S[1][1]) = +1.769e+02
S[2][1] = +1.881e-01-1.460e-01i, |S[2][1]| = -1.247e+01, arg(S[2][1]) = -3.782e+01
It 89/300: ω/2π = 3.014e+01 GHz (total elapsed time = 1.77e+02 s)
Calculating boundary modes at wave ports for ω/2π = 3.014e+01 GHz (5.053e-01)
Port 1, mode 1: kₙ = 2.122e+03-9.763e-02i m⁻¹
Port 2, mode 1: kₙ = 2.122e+03-9.762e-02i m⁻¹
Sol. ||E|| = 1.436169e+01
Field energy E (4.332e-04 J) + H (5.634e-04 J) = 9.966e-04 J
S[1][1] = -6.717e-01+3.644e-02i, |S[1][1]| = -3.444e+00, arg(S[1][1]) = +1.769e+02
S[2][1] = +1.863e-01-1.471e-01i, |S[2][1]| = -1.249e+01, arg(S[2][1]) = -3.829e+01
It 90/300: ω/2π = 3.047e+01 GHz (total elapsed time = 1.77e+02 s)
Calculating boundary modes at wave ports for ω/2π = 3.047e+01 GHz (5.109e-01)
Port 1, mode 1: kₙ = 2.146e+03-9.870e-02i m⁻¹
Port 2, mode 1: kₙ = 2.146e+03-9.869e-02i m⁻¹
Sol. ||E|| = 1.435806e+01
Field energy E (4.329e-04 J) + H (5.632e-04 J) = 9.961e-04 J
S[1][1] = -6.709e-01+3.677e-02i, |S[1][1]| = -3.453e+00, arg(S[1][1]) = +1.769e+02
S[2][1] = +1.846e-01-1.482e-01i, |S[2][1]| = -1.252e+01, arg(S[2][1]) = -3.877e+01
It 91/300: ω/2π = 3.080e+01 GHz (total elapsed time = 1.78e+02 s)
Calculating boundary modes at wave ports for ω/2π = 3.080e+01 GHz (5.164e-01)
Port 1, mode 1: kₙ = 2.169e+03-9.977e-02i m⁻¹
Port 2, mode 1: kₙ = 2.169e+03-9.976e-02i m⁻¹
Sol. ||E|| = 1.435445e+01
Field energy E (4.327e-04 J) + H (5.629e-04 J) = 9.956e-04 J
S[1][1] = -6.702e-01+3.710e-02i, |S[1][1]| = -3.463e+00, arg(S[1][1]) = +1.768e+02
S[2][1] = +1.828e-01-1.493e-01i, |S[2][1]| = -1.254e+01, arg(S[2][1]) = -3.924e+01
It 92/300: ω/2π = 3.113e+01 GHz (total elapsed time = 1.78e+02 s)
Calculating boundary modes at wave ports for ω/2π = 3.113e+01 GHz (5.220e-01)
Port 1, mode 1: kₙ = 2.192e+03-1.008e-01i m⁻¹
Port 2, mode 1: kₙ = 2.192e+03-1.008e-01i m⁻¹
Sol. ||E|| = 1.435087e+01
Field energy E (4.325e-04 J) + H (5.626e-04 J) = 9.951e-04 J
S[1][1] = -6.694e-01+3.743e-02i, |S[1][1]| = -3.472e+00, arg(S[1][1]) = +1.768e+02
S[2][1] = +1.811e-01-1.504e-01i, |S[2][1]| = -1.256e+01, arg(S[2][1]) = -3.972e+01
It 93/300: ω/2π = 3.146e+01 GHz (total elapsed time = 1.79e+02 s)
Calculating boundary modes at wave ports for ω/2π = 3.146e+01 GHz (5.275e-01)
Port 1, mode 1: kₙ = 2.216e+03-1.019e-01i m⁻¹
Port 2, mode 1: kₙ = 2.216e+03-1.019e-01i m⁻¹
Sol. ||E|| = 1.434732e+01
Field energy E (4.323e-04 J) + H (5.624e-04 J) = 9.947e-04 J
S[1][1] = -6.687e-01+3.777e-02i, |S[1][1]| = -3.482e+00, arg(S[1][1]) = +1.768e+02
S[2][1] = +1.793e-01-1.515e-01i, |S[2][1]| = -1.259e+01, arg(S[2][1]) = -4.020e+01
It 94/300: ω/2π = 3.179e+01 GHz (total elapsed time = 1.79e+02 s)
Calculating boundary modes at wave ports for ω/2π = 3.179e+01 GHz (5.331e-01)
Port 1, mode 1: kₙ = 2.239e+03-1.030e-01i m⁻¹
Port 2, mode 1: kₙ = 2.239e+03-1.030e-01i m⁻¹
Sol. ||E|| = 1.434381e+01
Field energy E (4.321e-04 J) + H (5.621e-04 J) = 9.942e-04 J
S[1][1] = -6.679e-01+3.810e-02i, |S[1][1]| = -3.492e+00, arg(S[1][1]) = +1.767e+02
S[2][1] = +1.775e-01-1.525e-01i, |S[2][1]| = -1.261e+01, arg(S[2][1]) = -4.068e+01
It 95/300: ω/2π = 3.212e+01 GHz (total elapsed time = 1.79e+02 s)
Calculating boundary modes at wave ports for ω/2π = 3.212e+01 GHz (5.386e-01)
Port 1, mode 1: kₙ = 2.262e+03-1.041e-01i m⁻¹
Port 2, mode 1: kₙ = 2.262e+03-1.041e-01i m⁻¹
Sol. ||E|| = 1.434032e+01
Field energy E (4.318e-04 J) + H (5.619e-04 J) = 9.937e-04 J
S[1][1] = -6.671e-01+3.843e-02i, |S[1][1]| = -3.501e+00, arg(S[1][1]) = +1.767e+02
S[2][1] = +1.757e-01-1.536e-01i, |S[2][1]| = -1.264e+01, arg(S[2][1]) = -4.116e+01
It 96/300: ω/2π = 3.245e+01 GHz (total elapsed time = 1.79e+02 s)
Calculating boundary modes at wave ports for ω/2π = 3.245e+01 GHz (5.442e-01)
Port 1, mode 1: kₙ = 2.286e+03-1.051e-01i m⁻¹
Port 2, mode 1: kₙ = 2.286e+03-1.051e-01i m⁻¹
Sol. ||E|| = 1.433687e+01
Field energy E (4.316e-04 J) + H (5.617e-04 J) = 9.933e-04 J
S[1][1] = -6.664e-01+3.876e-02i, |S[1][1]| = -3.511e+00, arg(S[1][1]) = +1.767e+02
S[2][1] = +1.739e-01-1.546e-01i, |S[2][1]| = -1.266e+01, arg(S[2][1]) = -4.164e+01
It 97/300: ω/2π = 3.279e+01 GHz (total elapsed time = 1.80e+02 s)
Calculating boundary modes at wave ports for ω/2π = 3.279e+01 GHz (5.497e-01)
Port 1, mode 1: kₙ = 2.309e+03-1.062e-01i m⁻¹
Port 2, mode 1: kₙ = 2.309e+03-1.062e-01i m⁻¹
Sol. ||E|| = 1.433346e+01
Field energy E (4.314e-04 J) + H (5.614e-04 J) = 9.929e-04 J
S[1][1] = -6.656e-01+3.909e-02i, |S[1][1]| = -3.521e+00, arg(S[1][1]) = +1.766e+02
S[2][1] = +1.721e-01-1.556e-01i, |S[2][1]| = -1.269e+01, arg(S[2][1]) = -4.213e+01
It 98/300: ω/2π = 3.312e+01 GHz (total elapsed time = 1.80e+02 s)
Calculating boundary modes at wave ports for ω/2π = 3.312e+01 GHz (5.553e-01)
Port 1, mode 1: kₙ = 2.332e+03-1.073e-01i m⁻¹
Port 2, mode 1: kₙ = 2.332e+03-1.073e-01i m⁻¹
Sol. ||E|| = 1.433008e+01
Field energy E (4.312e-04 J) + H (5.612e-04 J) = 9.924e-04 J
S[1][1] = -6.648e-01+3.942e-02i, |S[1][1]| = -3.530e+00, arg(S[1][1]) = +1.766e+02
S[2][1] = +1.702e-01-1.566e-01i, |S[2][1]| = -1.272e+01, arg(S[2][1]) = -4.261e+01
It 99/300: ω/2π = 3.345e+01 GHz (total elapsed time = 1.80e+02 s)
Calculating boundary modes at wave ports for ω/2π = 3.345e+01 GHz (5.608e-01)
Port 1, mode 1: kₙ = 2.356e+03-1.084e-01i m⁻¹
Port 2, mode 1: kₙ = 2.356e+03-1.083e-01i m⁻¹
Sol. ||E|| = 1.432674e+01
Field energy E (4.310e-04 J) + H (5.610e-04 J) = 9.920e-04 J
S[1][1] = -6.641e-01+3.975e-02i, |S[1][1]| = -3.540e+00, arg(S[1][1]) = +1.766e+02
S[2][1] = +1.684e-01-1.576e-01i, |S[2][1]| = -1.274e+01, arg(S[2][1]) = -4.310e+01
It 100/300: ω/2π = 3.378e+01 GHz (total elapsed time = 1.81e+02 s)
Calculating boundary modes at wave ports for ω/2π = 3.378e+01 GHz (5.664e-01)
Port 1, mode 1: kₙ = 2.379e+03-1.094e-01i m⁻¹
Port 2, mode 1: kₙ = 2.379e+03-1.094e-01i m⁻¹
Sol. ||E|| = 1.432343e+01
Field energy E (4.308e-04 J) + H (5.608e-04 J) = 9.916e-04 J
S[1][1] = -6.633e-01+4.007e-02i, |S[1][1]| = -3.550e+00, arg(S[1][1]) = +1.765e+02
S[2][1] = +1.666e-01-1.586e-01i, |S[2][1]| = -1.277e+01, arg(S[2][1]) = -4.359e+01
It 101/300: ω/2π = 3.411e+01 GHz (total elapsed time = 1.81e+02 s)
Calculating boundary modes at wave ports for ω/2π = 3.411e+01 GHz (5.719e-01)
Port 1, mode 1: kₙ = 2.402e+03-1.105e-01i m⁻¹
Port 2, mode 1: kₙ = 2.402e+03-1.105e-01i m⁻¹
Sol. ||E|| = 1.432016e+01
Field energy E (4.306e-04 J) + H (5.606e-04 J) = 9.912e-04 J
S[1][1] = -6.625e-01+4.040e-02i, |S[1][1]| = -3.560e+00, arg(S[1][1]) = +1.765e+02
S[2][1] = +1.647e-01-1.595e-01i, |S[2][1]| = -1.279e+01, arg(S[2][1]) = -4.408e+01
It 102/300: ω/2π = 3.444e+01 GHz (total elapsed time = 1.81e+02 s)
Calculating boundary modes at wave ports for ω/2π = 3.444e+01 GHz (5.775e-01)
Port 1, mode 1: kₙ = 2.426e+03-1.116e-01i m⁻¹
Port 2, mode 1: kₙ = 2.426e+03-1.116e-01i m⁻¹
Sol. ||E|| = 1.431694e+01
Field energy E (4.304e-04 J) + H (5.603e-04 J) = 9.907e-04 J
S[1][1] = -6.618e-01+4.073e-02i, |S[1][1]| = -3.570e+00, arg(S[1][1]) = +1.765e+02
S[2][1] = +1.629e-01-1.605e-01i, |S[2][1]| = -1.282e+01, arg(S[2][1]) = -4.458e+01
It 103/300: ω/2π = 3.477e+01 GHz (total elapsed time = 1.81e+02 s)
Calculating boundary modes at wave ports for ω/2π = 3.477e+01 GHz (5.830e-01)
Port 1, mode 1: kₙ = 2.449e+03-1.126e-01i m⁻¹
Port 2, mode 1: kₙ = 2.449e+03-1.126e-01i m⁻¹
Sol. ||E|| = 1.431375e+01
Field energy E (4.302e-04 J) + H (5.601e-04 J) = 9.903e-04 J
S[1][1] = -6.610e-01+4.105e-02i, |S[1][1]| = -3.580e+00, arg(S[1][1]) = +1.764e+02
S[2][1] = +1.610e-01-1.614e-01i, |S[2][1]| = -1.284e+01, arg(S[2][1]) = -4.507e+01
It 104/300: ω/2π = 3.510e+01 GHz (total elapsed time = 1.82e+02 s)
Calculating boundary modes at wave ports for ω/2π = 3.510e+01 GHz (5.886e-01)
Port 1, mode 1: kₙ = 2.472e+03-1.137e-01i m⁻¹
Port 2, mode 1: kₙ = 2.472e+03-1.137e-01i m⁻¹
Sol. ||E|| = 1.431061e+01
Field energy E (4.300e-04 J) + H (5.599e-04 J) = 9.899e-04 J
S[1][1] = -6.602e-01+4.138e-02i, |S[1][1]| = -3.590e+00, arg(S[1][1]) = +1.764e+02
S[2][1] = +1.591e-01-1.623e-01i, |S[2][1]| = -1.287e+01, arg(S[2][1]) = -4.557e+01
It 105/300: ω/2π = 3.543e+01 GHz (total elapsed time = 1.82e+02 s)
Calculating boundary modes at wave ports for ω/2π = 3.543e+01 GHz (5.941e-01)
Port 1, mode 1: kₙ = 2.495e+03-1.148e-01i m⁻¹
Port 2, mode 1: kₙ = 2.495e+03-1.148e-01i m⁻¹
Sol. ||E|| = 1.430750e+01
Field energy E (4.298e-04 J) + H (5.597e-04 J) = 9.895e-04 J
S[1][1] = -6.594e-01+4.170e-02i, |S[1][1]| = -3.600e+00, arg(S[1][1]) = +1.764e+02
S[2][1] = +1.572e-01-1.632e-01i, |S[2][1]| = -1.289e+01, arg(S[2][1]) = -4.607e+01
It 106/300: ω/2π = 3.577e+01 GHz (total elapsed time = 1.82e+02 s)
Calculating boundary modes at wave ports for ω/2π = 3.577e+01 GHz (5.997e-01)
Port 1, mode 1: kₙ = 2.519e+03-1.159e-01i m⁻¹
Port 2, mode 1: kₙ = 2.519e+03-1.159e-01i m⁻¹
Sol. ||E|| = 1.430444e+01
Field energy E (4.296e-04 J) + H (5.595e-04 J) = 9.892e-04 J
S[1][1] = -6.586e-01+4.202e-02i, |S[1][1]| = -3.610e+00, arg(S[1][1]) = +1.763e+02
S[2][1] = +1.553e-01-1.641e-01i, |S[2][1]| = -1.292e+01, arg(S[2][1]) = -4.657e+01
It 107/300: ω/2π = 3.610e+01 GHz (total elapsed time = 1.83e+02 s)
Calculating boundary modes at wave ports for ω/2π = 3.610e+01 GHz (6.052e-01)
Port 1, mode 1: kₙ = 2.542e+03-1.169e-01i m⁻¹
Port 2, mode 1: kₙ = 2.542e+03-1.169e-01i m⁻¹
Sol. ||E|| = 1.430143e+01
Field energy E (4.294e-04 J) + H (5.593e-04 J) = 9.888e-04 J
S[1][1] = -6.578e-01+4.235e-02i, |S[1][1]| = -3.620e+00, arg(S[1][1]) = +1.763e+02
S[2][1] = +1.535e-01-1.650e-01i, |S[2][1]| = -1.294e+01, arg(S[2][1]) = -4.707e+01
It 108/300: ω/2π = 3.643e+01 GHz (total elapsed time = 1.83e+02 s)
Calculating boundary modes at wave ports for ω/2π = 3.643e+01 GHz (6.108e-01)
Port 1, mode 1: kₙ = 2.565e+03-1.180e-01i m⁻¹
Port 2, mode 1: kₙ = 2.565e+03-1.180e-01i m⁻¹
Sol. ||E|| = 1.429846e+01
Field energy E (4.293e-04 J) + H (5.591e-04 J) = 9.884e-04 J
S[1][1] = -6.571e-01+4.267e-02i, |S[1][1]| = -3.630e+00, arg(S[1][1]) = +1.763e+02
S[2][1] = +1.515e-01-1.658e-01i, |S[2][1]| = -1.297e+01, arg(S[2][1]) = -4.757e+01
It 109/300: ω/2π = 3.676e+01 GHz (total elapsed time = 1.84e+02 s)
Calculating boundary modes at wave ports for ω/2π = 3.676e+01 GHz (6.163e-01)
Port 1, mode 1: kₙ = 2.589e+03-1.191e-01i m⁻¹
Port 2, mode 1: kₙ = 2.589e+03-1.191e-01i m⁻¹
Sol. ||E|| = 1.429553e+01
Field energy E (4.291e-04 J) + H (5.590e-04 J) = 9.880e-04 J
S[1][1] = -6.563e-01+4.299e-02i, |S[1][1]| = -3.640e+00, arg(S[1][1]) = +1.763e+02
S[2][1] = +1.496e-01-1.666e-01i, |S[2][1]| = -1.300e+01, arg(S[2][1]) = -4.808e+01
It 110/300: ω/2π = 3.709e+01 GHz (total elapsed time = 1.84e+02 s)
Calculating boundary modes at wave ports for ω/2π = 3.709e+01 GHz (6.219e-01)
Port 1, mode 1: kₙ = 2.612e+03-1.201e-01i m⁻¹
Port 2, mode 1: kₙ = 2.612e+03-1.201e-01i m⁻¹
Sol. ||E|| = 1.429265e+01
Field energy E (4.289e-04 J) + H (5.588e-04 J) = 9.877e-04 J
S[1][1] = -6.555e-01+4.331e-02i, |S[1][1]| = -3.650e+00, arg(S[1][1]) = +1.762e+02
S[2][1] = +1.477e-01-1.675e-01i, |S[2][1]| = -1.302e+01, arg(S[2][1]) = -4.858e+01
It 111/300: ω/2π = 3.742e+01 GHz (total elapsed time = 1.85e+02 s)
Calculating boundary modes at wave ports for ω/2π = 3.742e+01 GHz (6.274e-01)
Port 1, mode 1: kₙ = 2.635e+03-1.212e-01i m⁻¹
Port 2, mode 1: kₙ = 2.635e+03-1.212e-01i m⁻¹
Sol. ||E|| = 1.428982e+01
Field energy E (4.287e-04 J) + H (5.586e-04 J) = 9.873e-04 J
S[1][1] = -6.547e-01+4.363e-02i, |S[1][1]| = -3.660e+00, arg(S[1][1]) = +1.762e+02
S[2][1] = +1.458e-01-1.683e-01i, |S[2][1]| = -1.305e+01, arg(S[2][1]) = -4.909e+01
It 112/300: ω/2π = 3.775e+01 GHz (total elapsed time = 1.85e+02 s)
Calculating boundary modes at wave ports for ω/2π = 3.775e+01 GHz (6.330e-01)
Port 1, mode 1: kₙ = 2.659e+03-1.223e-01i m⁻¹
Port 2, mode 1: kₙ = 2.659e+03-1.223e-01i m⁻¹
Sol. ||E|| = 1.428703e+01
Field energy E (4.285e-04 J) + H (5.584e-04 J) = 9.870e-04 J
S[1][1] = -6.539e-01+4.394e-02i, |S[1][1]| = -3.670e+00, arg(S[1][1]) = +1.762e+02
S[2][1] = +1.439e-01-1.691e-01i, |S[2][1]| = -1.307e+01, arg(S[2][1]) = -4.960e+01
It 113/300: ω/2π = 3.808e+01 GHz (total elapsed time = 1.86e+02 s)
Calculating boundary modes at wave ports for ω/2π = 3.808e+01 GHz (6.385e-01)
Port 1, mode 1: kₙ = 2.682e+03-1.234e-01i m⁻¹
Port 2, mode 1: kₙ = 2.682e+03-1.234e-01i m⁻¹
Sol. ||E|| = 1.428429e+01
Field energy E (4.284e-04 J) + H (5.582e-04 J) = 9.866e-04 J
S[1][1] = -6.531e-01+4.426e-02i, |S[1][1]| = -3.680e+00, arg(S[1][1]) = +1.761e+02
S[2][1] = +1.419e-01-1.698e-01i, |S[2][1]| = -1.310e+01, arg(S[2][1]) = -5.011e+01
It 114/300: ω/2π = 3.841e+01 GHz (total elapsed time = 1.87e+02 s)
Calculating boundary modes at wave ports for ω/2π = 3.841e+01 GHz (6.441e-01)
Port 1, mode 1: kₙ = 2.705e+03-1.244e-01i m⁻¹
Port 2, mode 1: kₙ = 2.705e+03-1.244e-01i m⁻¹
Sol. ||E|| = 1.428161e+01
Field energy E (4.282e-04 J) + H (5.580e-04 J) = 9.863e-04 J
S[1][1] = -6.523e-01+4.458e-02i, |S[1][1]| = -3.691e+00, arg(S[1][1]) = +1.761e+02
S[2][1] = +1.400e-01-1.706e-01i, |S[2][1]| = -1.313e+01, arg(S[2][1]) = -5.063e+01
It 115/300: ω/2π = 3.875e+01 GHz (total elapsed time = 1.87e+02 s)
Calculating boundary modes at wave ports for ω/2π = 3.875e+01 GHz (6.496e-01)
Port 1, mode 1: kₙ = 2.729e+03-1.255e-01i m⁻¹
Port 2, mode 1: kₙ = 2.729e+03-1.255e-01i m⁻¹
Sol. ||E|| = 1.427897e+01
Field energy E (4.280e-04 J) + H (5.579e-04 J) = 9.859e-04 J
S[1][1] = -6.515e-01+4.489e-02i, |S[1][1]| = -3.701e+00, arg(S[1][1]) = +1.761e+02
S[2][1] = +1.380e-01-1.713e-01i, |S[2][1]| = -1.315e+01, arg(S[2][1]) = -5.114e+01
It 116/300: ω/2π = 3.908e+01 GHz (total elapsed time = 1.87e+02 s)
Calculating boundary modes at wave ports for ω/2π = 3.908e+01 GHz (6.552e-01)
Port 1, mode 1: kₙ = 2.752e+03-1.266e-01i m⁻¹
Port 2, mode 1: kₙ = 2.752e+03-1.266e-01i m⁻¹
Sol. ||E|| = 1.427638e+01
Field energy E (4.279e-04 J) + H (5.577e-04 J) = 9.856e-04 J
S[1][1] = -6.507e-01+4.520e-02i, |S[1][1]| = -3.711e+00, arg(S[1][1]) = +1.760e+02
S[2][1] = +1.361e-01-1.720e-01i, |S[2][1]| = -1.318e+01, arg(S[2][1]) = -5.166e+01
It 117/300: ω/2π = 3.941e+01 GHz (total elapsed time = 1.88e+02 s)
Calculating boundary modes at wave ports for ω/2π = 3.941e+01 GHz (6.607e-01)
Port 1, mode 1: kₙ = 2.775e+03-1.277e-01i m⁻¹
Port 2, mode 1: kₙ = 2.775e+03-1.276e-01i m⁻¹
Sol. ||E|| = 1.427384e+01
Field energy E (4.277e-04 J) + H (5.575e-04 J) = 9.853e-04 J
S[1][1] = -6.499e-01+4.552e-02i, |S[1][1]| = -3.721e+00, arg(S[1][1]) = +1.760e+02
S[2][1] = +1.341e-01-1.727e-01i, |S[2][1]| = -1.320e+01, arg(S[2][1]) = -5.217e+01
It 118/300: ω/2π = 3.974e+01 GHz (total elapsed time = 1.88e+02 s)
Calculating boundary modes at wave ports for ω/2π = 3.974e+01 GHz (6.663e-01)
Port 1, mode 1: kₙ = 2.799e+03-1.287e-01i m⁻¹
Port 2, mode 1: kₙ = 2.799e+03-1.287e-01i m⁻¹
Sol. ||E|| = 1.427135e+01
Field energy E (4.276e-04 J) + H (5.574e-04 J) = 9.849e-04 J
S[1][1] = -6.491e-01+4.583e-02i, |S[1][1]| = -3.732e+00, arg(S[1][1]) = +1.760e+02
S[2][1] = +1.322e-01-1.734e-01i, |S[2][1]| = -1.323e+01, arg(S[2][1]) = -5.269e+01
It 119/300: ω/2π = 4.007e+01 GHz (total elapsed time = 1.88e+02 s)
Calculating boundary modes at wave ports for ω/2π = 4.007e+01 GHz (6.718e-01)
Port 1, mode 1: kₙ = 2.822e+03-1.298e-01i m⁻¹
Port 2, mode 1: kₙ = 2.822e+03-1.298e-01i m⁻¹
Sol. ||E|| = 1.426891e+01
Field energy E (4.274e-04 J) + H (5.572e-04 J) = 9.846e-04 J
S[1][1] = -6.483e-01+4.614e-02i, |S[1][1]| = -3.742e+00, arg(S[1][1]) = +1.759e+02
S[2][1] = +1.302e-01-1.741e-01i, |S[2][1]| = -1.325e+01, arg(S[2][1]) = -5.321e+01
It 120/300: ω/2π = 4.040e+01 GHz (total elapsed time = 1.88e+02 s)
Calculating boundary modes at wave ports for ω/2π = 4.040e+01 GHz (6.774e-01)
Port 1, mode 1: kₙ = 2.845e+03-1.309e-01i m⁻¹
Port 2, mode 1: kₙ = 2.845e+03-1.309e-01i m⁻¹
Sol. ||E|| = 1.426653e+01
Field energy E (4.273e-04 J) + H (5.570e-04 J) = 9.843e-04 J
S[1][1] = -6.475e-01+4.645e-02i, |S[1][1]| = -3.752e+00, arg(S[1][1]) = +1.759e+02
S[2][1] = +1.282e-01-1.748e-01i, |S[2][1]| = -1.328e+01, arg(S[2][1]) = -5.374e+01
It 121/300: ω/2π = 4.073e+01 GHz (total elapsed time = 1.89e+02 s)
Calculating boundary modes at wave ports for ω/2π = 4.073e+01 GHz (6.830e-01)
Port 1, mode 1: kₙ = 2.869e+03-1.319e-01i m⁻¹
Port 2, mode 1: kₙ = 2.869e+03-1.319e-01i m⁻¹
Sol. ||E|| = 1.426420e+01
Field energy E (4.271e-04 J) + H (5.569e-04 J) = 9.840e-04 J
S[1][1] = -6.467e-01+4.675e-02i, |S[1][1]| = -3.763e+00, arg(S[1][1]) = +1.759e+02
S[2][1] = +1.262e-01-1.754e-01i, |S[2][1]| = -1.331e+01, arg(S[2][1]) = -5.426e+01
It 122/300: ω/2π = 4.106e+01 GHz (total elapsed time = 1.89e+02 s)
Calculating boundary modes at wave ports for ω/2π = 4.106e+01 GHz (6.885e-01)
Port 1, mode 1: kₙ = 2.892e+03-1.330e-01i m⁻¹
Port 2, mode 1: kₙ = 2.892e+03-1.330e-01i m⁻¹
Sol. ||E|| = 1.426192e+01
Field energy E (4.270e-04 J) + H (5.567e-04 J) = 9.837e-04 J
S[1][1] = -6.459e-01+4.706e-02i, |S[1][1]| = -3.773e+00, arg(S[1][1]) = +1.758e+02
S[2][1] = +1.243e-01-1.760e-01i, |S[2][1]| = -1.333e+01, arg(S[2][1]) = -5.478e+01
It 123/300: ω/2π = 4.139e+01 GHz (total elapsed time = 1.89e+02 s)
Calculating boundary modes at wave ports for ω/2π = 4.139e+01 GHz (6.941e-01)
Port 1, mode 1: kₙ = 2.915e+03-1.341e-01i m⁻¹
Port 2, mode 1: kₙ = 2.915e+03-1.341e-01i m⁻¹
Sol. ||E|| = 1.425969e+01
Field energy E (4.268e-04 J) + H (5.566e-04 J) = 9.834e-04 J
S[1][1] = -6.451e-01+4.737e-02i, |S[1][1]| = -3.783e+00, arg(S[1][1]) = +1.758e+02
S[2][1] = +1.223e-01-1.767e-01i, |S[2][1]| = -1.336e+01, arg(S[2][1]) = -5.531e+01
It 124/300: ω/2π = 4.173e+01 GHz (total elapsed time = 1.90e+02 s)
Calculating boundary modes at wave ports for ω/2π = 4.173e+01 GHz (6.996e-01)
Port 1, mode 1: kₙ = 2.939e+03-1.352e-01i m⁻¹
Port 2, mode 1: kₙ = 2.939e+03-1.352e-01i m⁻¹
Sol. ||E|| = 1.425752e+01
Field energy E (4.267e-04 J) + H (5.564e-04 J) = 9.831e-04 J
S[1][1] = -6.443e-01+4.767e-02i, |S[1][1]| = -3.794e+00, arg(S[1][1]) = +1.758e+02
S[2][1] = +1.203e-01-1.772e-01i, |S[2][1]| = -1.338e+01, arg(S[2][1]) = -5.584e+01
It 125/300: ω/2π = 4.206e+01 GHz (total elapsed time = 1.90e+02 s)
Calculating boundary modes at wave ports for ω/2π = 4.206e+01 GHz (7.052e-01)
Port 1, mode 1: kₙ = 2.962e+03-1.362e-01i m⁻¹
Port 2, mode 1: kₙ = 2.962e+03-1.362e-01i m⁻¹
Sol. ||E|| = 1.425540e+01
Field energy E (4.266e-04 J) + H (5.563e-04 J) = 9.828e-04 J
S[1][1] = -6.435e-01+4.797e-02i, |S[1][1]| = -3.804e+00, arg(S[1][1]) = +1.757e+02
S[2][1] = +1.183e-01-1.778e-01i, |S[2][1]| = -1.341e+01, arg(S[2][1]) = -5.637e+01
It 126/300: ω/2π = 4.239e+01 GHz (total elapsed time = 1.90e+02 s)
Calculating boundary modes at wave ports for ω/2π = 4.239e+01 GHz (7.107e-01)
Port 1, mode 1: kₙ = 2.985e+03-1.373e-01i m⁻¹
Port 2, mode 1: kₙ = 2.985e+03-1.373e-01i m⁻¹
Sol. ||E|| = 1.425334e+01
Field energy E (4.264e-04 J) + H (5.561e-04 J) = 9.825e-04 J
S[1][1] = -6.427e-01+4.827e-02i, |S[1][1]| = -3.815e+00, arg(S[1][1]) = +1.757e+02
S[2][1] = +1.163e-01-1.784e-01i, |S[2][1]| = -1.344e+01, arg(S[2][1]) = -5.690e+01
It 127/300: ω/2π = 4.272e+01 GHz (total elapsed time = 1.91e+02 s)
Calculating boundary modes at wave ports for ω/2π = 4.272e+01 GHz (7.163e-01)
Port 1, mode 1: kₙ = 3.008e+03-1.384e-01i m⁻¹
Port 2, mode 1: kₙ = 3.008e+03-1.384e-01i m⁻¹
Sol. ||E|| = 1.425133e+01
Field energy E (4.263e-04 J) + H (5.560e-04 J) = 9.823e-04 J
S[1][1] = -6.419e-01+4.857e-02i, |S[1][1]| = -3.825e+00, arg(S[1][1]) = +1.757e+02
S[2][1] = +1.143e-01-1.789e-01i, |S[2][1]| = -1.346e+01, arg(S[2][1]) = -5.743e+01
It 128/300: ω/2π = 4.305e+01 GHz (total elapsed time = 1.91e+02 s)
Calculating boundary modes at wave ports for ω/2π = 4.305e+01 GHz (7.218e-01)
Port 1, mode 1: kₙ = 3.032e+03-1.395e-01i m⁻¹
Port 2, mode 1: kₙ = 3.032e+03-1.394e-01i m⁻¹
Sol. ||E|| = 1.424938e+01
Field energy E (4.262e-04 J) + H (5.558e-04 J) = 9.820e-04 J
S[1][1] = -6.411e-01+4.887e-02i, |S[1][1]| = -3.836e+00, arg(S[1][1]) = +1.756e+02
S[2][1] = +1.123e-01-1.794e-01i, |S[2][1]| = -1.349e+01, arg(S[2][1]) = -5.797e+01
It 129/300: ω/2π = 4.338e+01 GHz (total elapsed time = 1.91e+02 s)
Calculating boundary modes at wave ports for ω/2π = 4.338e+01 GHz (7.274e-01)
Port 1, mode 1: kₙ = 3.055e+03-1.405e-01i m⁻¹
Port 2, mode 1: kₙ = 3.055e+03-1.405e-01i m⁻¹
Sol. ||E|| = 1.424749e+01
Field energy E (4.261e-04 J) + H (5.557e-04 J) = 9.817e-04 J
S[1][1] = -6.403e-01+4.917e-02i, |S[1][1]| = -3.846e+00, arg(S[1][1]) = +1.756e+02
S[2][1] = +1.103e-01-1.800e-01i, |S[2][1]| = -1.351e+01, arg(S[2][1]) = -5.850e+01
It 130/300: ω/2π = 4.371e+01 GHz (total elapsed time = 1.92e+02 s)
Calculating boundary modes at wave ports for ω/2π = 4.371e+01 GHz (7.329e-01)
Port 1, mode 1: kₙ = 3.078e+03-1.416e-01i m⁻¹
Port 2, mode 1: kₙ = 3.078e+03-1.416e-01i m⁻¹
Sol. ||E|| = 1.424565e+01
Field energy E (4.259e-04 J) + H (5.555e-04 J) = 9.815e-04 J
S[1][1] = -6.395e-01+4.947e-02i, |S[1][1]| = -3.857e+00, arg(S[1][1]) = +1.756e+02
S[2][1] = +1.082e-01-1.804e-01i, |S[2][1]| = -1.354e+01, arg(S[2][1]) = -5.904e+01
It 131/300: ω/2π = 4.404e+01 GHz (total elapsed time = 1.92e+02 s)
Calculating boundary modes at wave ports for ω/2π = 4.404e+01 GHz (7.385e-01)
Port 1, mode 1: kₙ = 3.102e+03-1.427e-01i m⁻¹
Port 2, mode 1: kₙ = 3.102e+03-1.427e-01i m⁻¹
Sol. ||E|| = 1.424386e+01
Field energy E (4.258e-04 J) + H (5.554e-04 J) = 9.812e-04 J
S[1][1] = -6.387e-01+4.976e-02i, |S[1][1]| = -3.867e+00, arg(S[1][1]) = +1.755e+02
S[2][1] = +1.062e-01-1.809e-01i, |S[2][1]| = -1.356e+01, arg(S[2][1]) = -5.958e+01
It 132/300: ω/2π = 4.437e+01 GHz (total elapsed time = 1.92e+02 s)
Calculating boundary modes at wave ports for ω/2π = 4.437e+01 GHz (7.440e-01)
Port 1, mode 1: kₙ = 3.125e+03-1.437e-01i m⁻¹
Port 2, mode 1: kₙ = 3.125e+03-1.437e-01i m⁻¹
Sol. ||E|| = 1.424214e+01
Field energy E (4.257e-04 J) + H (5.552e-04 J) = 9.809e-04 J
S[1][1] = -6.379e-01+5.005e-02i, |S[1][1]| = -3.878e+00, arg(S[1][1]) = +1.755e+02
S[2][1] = +1.042e-01-1.814e-01i, |S[2][1]| = -1.359e+01, arg(S[2][1]) = -6.012e+01
It 133/300: ω/2π = 4.471e+01 GHz (total elapsed time = 1.93e+02 s)
Calculating boundary modes at wave ports for ω/2π = 4.471e+01 GHz (7.496e-01)
Port 1, mode 1: kₙ = 3.148e+03-1.448e-01i m⁻¹
Port 2, mode 1: kₙ = 3.148e+03-1.448e-01i m⁻¹
Sol. ||E|| = 1.424047e+01
Field energy E (4.256e-04 J) + H (5.551e-04 J) = 9.807e-04 J
S[1][1] = -6.371e-01+5.034e-02i, |S[1][1]| = -3.888e+00, arg(S[1][1]) = +1.755e+02
S[2][1] = +1.022e-01-1.818e-01i, |S[2][1]| = -1.362e+01, arg(S[2][1]) = -6.066e+01
It 134/300: ω/2π = 4.504e+01 GHz (total elapsed time = 1.93e+02 s)
Calculating boundary modes at wave ports for ω/2π = 4.504e+01 GHz (7.551e-01)
Port 1, mode 1: kₙ = 3.172e+03-1.459e-01i m⁻¹
Port 2, mode 1: kₙ = 3.172e+03-1.459e-01i m⁻¹
Sol. ||E|| = 1.423885e+01
Field energy E (4.255e-04 J) + H (5.549e-04 J) = 9.804e-04 J
S[1][1] = -6.363e-01+5.063e-02i, |S[1][1]| = -3.899e+00, arg(S[1][1]) = +1.755e+02
S[2][1] = +1.002e-01-1.822e-01i, |S[2][1]| = -1.364e+01, arg(S[2][1]) = -6.120e+01
It 135/300: ω/2π = 4.537e+01 GHz (total elapsed time = 1.93e+02 s)
Calculating boundary modes at wave ports for ω/2π = 4.537e+01 GHz (7.607e-01)
Port 1, mode 1: kₙ = 3.195e+03-1.470e-01i m⁻¹
Port 2, mode 1: kₙ = 3.195e+03-1.469e-01i m⁻¹
Sol. ||E|| = 1.423730e+01
Field energy E (4.254e-04 J) + H (5.548e-04 J) = 9.802e-04 J
S[1][1] = -6.355e-01+5.092e-02i, |S[1][1]| = -3.909e+00, arg(S[1][1]) = +1.754e+02
S[2][1] = +9.814e-02-1.826e-01i, |S[2][1]| = -1.367e+01, arg(S[2][1]) = -6.175e+01
It 136/300: ω/2π = 4.570e+01 GHz (total elapsed time = 1.94e+02 s)
Calculating boundary modes at wave ports for ω/2π = 4.570e+01 GHz (7.662e-01)
Port 1, mode 1: kₙ = 3.218e+03-1.480e-01i m⁻¹
Port 2, mode 1: kₙ = 3.218e+03-1.480e-01i m⁻¹
Sol. ||E|| = 1.423580e+01
Field energy E (4.253e-04 J) + H (5.546e-04 J) = 9.800e-04 J
S[1][1] = -6.347e-01+5.121e-02i, |S[1][1]| = -3.920e+00, arg(S[1][1]) = +1.754e+02
S[2][1] = +9.612e-02-1.830e-01i, |S[2][1]| = -1.369e+01, arg(S[2][1]) = -6.229e+01
It 137/300: ω/2π = 4.603e+01 GHz (total elapsed time = 1.94e+02 s)
Calculating boundary modes at wave ports for ω/2π = 4.603e+01 GHz (7.718e-01)
Port 1, mode 1: kₙ = 3.242e+03-1.491e-01i m⁻¹
Port 2, mode 1: kₙ = 3.242e+03-1.491e-01i m⁻¹
Sol. ||E|| = 1.423436e+01
Field energy E (4.252e-04 J) + H (5.545e-04 J) = 9.797e-04 J
S[1][1] = -6.339e-01+5.149e-02i, |S[1][1]| = -3.931e+00, arg(S[1][1]) = +1.754e+02
S[2][1] = +9.409e-02-1.834e-01i, |S[2][1]| = -1.372e+01, arg(S[2][1]) = -6.284e+01
It 138/300: ω/2π = 4.636e+01 GHz (total elapsed time = 1.94e+02 s)
Calculating boundary modes at wave ports for ω/2π = 4.636e+01 GHz (7.773e-01)
Port 1, mode 1: kₙ = 3.265e+03-1.502e-01i m⁻¹
Port 2, mode 1: kₙ = 3.265e+03-1.502e-01i m⁻¹
Sol. ||E|| = 1.423297e+01
Field energy E (4.251e-04 J) + H (5.544e-04 J) = 9.795e-04 J
S[1][1] = -6.331e-01+5.178e-02i, |S[1][1]| = -3.941e+00, arg(S[1][1]) = +1.753e+02
S[2][1] = +9.206e-02-1.838e-01i, |S[2][1]| = -1.374e+01, arg(S[2][1]) = -6.339e+01
It 139/300: ω/2π = 4.669e+01 GHz (total elapsed time = 1.95e+02 s)
Calculating boundary modes at wave ports for ω/2π = 4.669e+01 GHz (7.829e-01)
Port 1, mode 1: kₙ = 3.288e+03-1.513e-01i m⁻¹
Port 2, mode 1: kₙ = 3.288e+03-1.512e-01i m⁻¹
Sol. ||E|| = 1.423165e+01
Field energy E (4.250e-04 J) + H (5.542e-04 J) = 9.793e-04 J
S[1][1] = -6.323e-01+5.206e-02i, |S[1][1]| = -3.952e+00, arg(S[1][1]) = +1.753e+02
S[2][1] = +9.002e-02-1.841e-01i, |S[2][1]| = -1.377e+01, arg(S[2][1]) = -6.394e+01
It 140/300: ω/2π = 4.702e+01 GHz (total elapsed time = 1.95e+02 s)
Calculating boundary modes at wave ports for ω/2π = 4.702e+01 GHz (7.884e-01)
Port 1, mode 1: kₙ = 3.312e+03-1.523e-01i m⁻¹
Port 2, mode 1: kₙ = 3.312e+03-1.523e-01i m⁻¹
Sol. ||E|| = 1.423038e+01
Field energy E (4.250e-04 J) + H (5.541e-04 J) = 9.791e-04 J
S[1][1] = -6.315e-01+5.234e-02i, |S[1][1]| = -3.962e+00, arg(S[1][1]) = +1.753e+02
S[2][1] = +8.799e-02-1.844e-01i, |S[2][1]| = -1.379e+01, arg(S[2][1]) = -6.449e+01
It 141/300: ω/2π = 4.735e+01 GHz (total elapsed time = 1.95e+02 s)
Calculating boundary modes at wave ports for ω/2π = 4.735e+01 GHz (7.940e-01)
Port 1, mode 1: kₙ = 3.335e+03-1.534e-01i m⁻¹
Port 2, mode 1: kₙ = 3.335e+03-1.534e-01i m⁻¹
Sol. ||E|| = 1.422917e+01
Field energy E (4.249e-04 J) + H (5.540e-04 J) = 9.788e-04 J
S[1][1] = -6.307e-01+5.262e-02i, |S[1][1]| = -3.973e+00, arg(S[1][1]) = +1.752e+02
S[2][1] = +8.596e-02-1.847e-01i, |S[2][1]| = -1.382e+01, arg(S[2][1]) = -6.505e+01
It 142/300: ω/2π = 4.769e+01 GHz (total elapsed time = 1.96e+02 s)
Calculating boundary modes at wave ports for ω/2π = 4.769e+01 GHz (7.995e-01)
Port 1, mode 1: kₙ = 3.358e+03-1.545e-01i m⁻¹
Port 2, mode 1: kₙ = 3.358e+03-1.545e-01i m⁻¹
Sol. ||E|| = 1.422802e+01
Field energy E (4.248e-04 J) + H (5.538e-04 J) = 9.786e-04 J
S[1][1] = -6.299e-01+5.289e-02i, |S[1][1]| = -3.984e+00, arg(S[1][1]) = +1.752e+02
S[2][1] = +8.392e-02-1.850e-01i, |S[2][1]| = -1.384e+01, arg(S[2][1]) = -6.560e+01
It 143/300: ω/2π = 4.802e+01 GHz (total elapsed time = 1.96e+02 s)
Calculating boundary modes at wave ports for ω/2π = 4.802e+01 GHz (8.051e-01)
Port 1, mode 1: kₙ = 3.382e+03-1.555e-01i m⁻¹
Port 2, mode 1: kₙ = 3.382e+03-1.555e-01i m⁻¹
Sol. ||E|| = 1.422692e+01
Field energy E (4.247e-04 J) + H (5.537e-04 J) = 9.784e-04 J
S[1][1] = -6.291e-01+5.317e-02i, |S[1][1]| = -3.994e+00, arg(S[1][1]) = +1.752e+02
S[2][1] = +8.189e-02-1.853e-01i, |S[2][1]| = -1.387e+01, arg(S[2][1]) = -6.616e+01
It 144/300: ω/2π = 4.835e+01 GHz (total elapsed time = 1.96e+02 s)
Calculating boundary modes at wave ports for ω/2π = 4.835e+01 GHz (8.106e-01)
Port 1, mode 1: kₙ = 3.405e+03-1.566e-01i m⁻¹
Port 2, mode 1: kₙ = 3.405e+03-1.566e-01i m⁻¹
Sol. ||E|| = 1.422589e+01
Field energy E (4.247e-04 J) + H (5.535e-04 J) = 9.782e-04 J
S[1][1] = -6.283e-01+5.344e-02i, |S[1][1]| = -4.005e+00, arg(S[1][1]) = +1.751e+02
S[2][1] = +7.985e-02-1.855e-01i, |S[2][1]| = -1.389e+01, arg(S[2][1]) = -6.671e+01
It 145/300: ω/2π = 4.868e+01 GHz (total elapsed time = 1.96e+02 s)
Calculating boundary modes at wave ports for ω/2π = 4.868e+01 GHz (8.162e-01)
Port 1, mode 1: kₙ = 3.428e+03-1.577e-01i m⁻¹
Port 2, mode 1: kₙ = 3.428e+03-1.577e-01i m⁻¹
Sol. ||E|| = 1.422491e+01
Field energy E (4.246e-04 J) + H (5.534e-04 J) = 9.780e-04 J
S[1][1] = -6.275e-01+5.371e-02i, |S[1][1]| = -4.015e+00, arg(S[1][1]) = +1.751e+02
S[2][1] = +7.781e-02-1.858e-01i, |S[2][1]| = -1.392e+01, arg(S[2][1]) = -6.727e+01
It 146/300: ω/2π = 4.901e+01 GHz (total elapsed time = 1.97e+02 s)
Calculating boundary modes at wave ports for ω/2π = 4.901e+01 GHz (8.217e-01)
Port 1, mode 1: kₙ = 3.452e+03-1.588e-01i m⁻¹
Port 2, mode 1: kₙ = 3.452e+03-1.587e-01i m⁻¹
Sol. ||E|| = 1.422399e+01
Field energy E (4.245e-04 J) + H (5.533e-04 J) = 9.778e-04 J
S[1][1] = -6.267e-01+5.398e-02i, |S[1][1]| = -4.026e+00, arg(S[1][1]) = +1.751e+02
S[2][1] = +7.578e-02-1.860e-01i, |S[2][1]| = -1.394e+01, arg(S[2][1]) = -6.783e+01
It 147/300: ω/2π = 4.934e+01 GHz (total elapsed time = 1.97e+02 s)
Calculating boundary modes at wave ports for ω/2π = 4.934e+01 GHz (8.273e-01)
Port 1, mode 1: kₙ = 3.475e+03-1.598e-01i m⁻¹
Port 2, mode 1: kₙ = 3.475e+03-1.598e-01i m⁻¹
Sol. ||E|| = 1.422313e+01
Field energy E (4.245e-04 J) + H (5.531e-04 J) = 9.776e-04 J
S[1][1] = -6.259e-01+5.425e-02i, |S[1][1]| = -4.037e+00, arg(S[1][1]) = +1.750e+02
S[2][1] = +7.374e-02-1.862e-01i, |S[2][1]| = -1.397e+01, arg(S[2][1]) = -6.839e+01
It 148/300: ω/2π = 4.967e+01 GHz (total elapsed time = 1.97e+02 s)
Calculating boundary modes at wave ports for ω/2π = 4.967e+01 GHz (8.328e-01)
Port 1, mode 1: kₙ = 3.498e+03-1.609e-01i m⁻¹
Port 2, mode 1: kₙ = 3.498e+03-1.609e-01i m⁻¹
Sol. ||E|| = 1.422233e+01
Field energy E (4.244e-04 J) + H (5.530e-04 J) = 9.774e-04 J
S[1][1] = -6.251e-01+5.451e-02i, |S[1][1]| = -4.047e+00, arg(S[1][1]) = +1.750e+02
S[2][1] = +7.170e-02-1.863e-01i, |S[2][1]| = -1.399e+01, arg(S[2][1]) = -6.895e+01
It 149/300: ω/2π = 5.000e+01 GHz (total elapsed time = 1.98e+02 s)
Calculating boundary modes at wave ports for ω/2π = 5.000e+01 GHz (8.384e-01)
Port 1, mode 1: kₙ = 3.521e+03-1.620e-01i m⁻¹
Port 2, mode 1: kₙ = 3.521e+03-1.620e-01i m⁻¹
Sol. ||E|| = 1.422158e+01
Field energy E (4.244e-04 J) + H (5.529e-04 J) = 9.772e-04 J
S[1][1] = -6.244e-01+5.477e-02i, |S[1][1]| = -4.058e+00, arg(S[1][1]) = +1.750e+02
S[2][1] = +6.967e-02-1.865e-01i, |S[2][1]| = -1.402e+01, arg(S[2][1]) = -6.952e+01
It 150/300: ω/2π = 5.033e+01 GHz (total elapsed time = 1.98e+02 s)
Calculating boundary modes at wave ports for ω/2π = 5.033e+01 GHz (8.439e-01)
Port 1, mode 1: kₙ = 3.545e+03-1.630e-01i m⁻¹
Port 2, mode 1: kₙ = 3.545e+03-1.630e-01i m⁻¹
Sol. ||E|| = 1.422090e+01
Field energy E (4.243e-04 J) + H (5.527e-04 J) = 9.770e-04 J
S[1][1] = -6.236e-01+5.504e-02i, |S[1][1]| = -4.069e+00, arg(S[1][1]) = +1.750e+02
S[2][1] = +6.763e-02-1.866e-01i, |S[2][1]| = -1.404e+01, arg(S[2][1]) = -7.008e+01
It 151/300: ω/2π = 5.067e+01 GHz (total elapsed time = 1.98e+02 s)
Calculating boundary modes at wave ports for ω/2π = 5.067e+01 GHz (8.495e-01)
Port 1, mode 1: kₙ = 3.568e+03-1.641e-01i m⁻¹
Port 2, mode 1: kₙ = 3.568e+03-1.641e-01i m⁻¹
Sol. ||E|| = 1.422027e+01
Field energy E (4.243e-04 J) + H (5.526e-04 J) = 9.769e-04 J
S[1][1] = -6.228e-01+5.530e-02i, |S[1][1]| = -4.079e+00, arg(S[1][1]) = +1.749e+02
S[2][1] = +6.560e-02-1.868e-01i, |S[2][1]| = -1.407e+01, arg(S[2][1]) = -7.065e+01
It 152/300: ω/2π = 5.100e+01 GHz (total elapsed time = 1.99e+02 s)
Calculating boundary modes at wave ports for ω/2π = 5.100e+01 GHz (8.550e-01)
Port 1, mode 1: kₙ = 3.591e+03-1.652e-01i m⁻¹
Port 2, mode 1: kₙ = 3.591e+03-1.652e-01i m⁻¹
Sol. ||E|| = 1.421970e+01
Field energy E (4.242e-04 J) + H (5.525e-04 J) = 9.767e-04 J
S[1][1] = -6.220e-01+5.555e-02i, |S[1][1]| = -4.090e+00, arg(S[1][1]) = +1.749e+02
S[2][1] = +6.357e-02-1.869e-01i, |S[2][1]| = -1.409e+01, arg(S[2][1]) = -7.121e+01
It 153/300: ω/2π = 5.133e+01 GHz (total elapsed time = 1.99e+02 s)
Calculating boundary modes at wave ports for ω/2π = 5.133e+01 GHz (8.606e-01)
Port 1, mode 1: kₙ = 3.615e+03-1.663e-01i m⁻¹
Port 2, mode 1: kₙ = 3.615e+03-1.663e-01i m⁻¹
Sol. ||E|| = 1.421918e+01
Field energy E (4.242e-04 J) + H (5.523e-04 J) = 9.765e-04 J
S[1][1] = -6.212e-01+5.581e-02i, |S[1][1]| = -4.101e+00, arg(S[1][1]) = +1.749e+02
S[2][1] = +6.153e-02-1.870e-01i, |S[2][1]| = -1.412e+01, arg(S[2][1]) = -7.178e+01
It 154/300: ω/2π = 5.166e+01 GHz (total elapsed time = 1.99e+02 s)
Calculating boundary modes at wave ports for ω/2π = 5.166e+01 GHz (8.662e-01)
Port 1, mode 1: kₙ = 3.638e+03-1.673e-01i m⁻¹
Port 2, mode 1: kₙ = 3.638e+03-1.673e-01i m⁻¹
Sol. ||E|| = 1.421873e+01
Field energy E (4.242e-04 J) + H (5.522e-04 J) = 9.763e-04 J
S[1][1] = -6.204e-01+5.606e-02i, |S[1][1]| = -4.111e+00, arg(S[1][1]) = +1.748e+02
S[2][1] = +5.950e-02-1.870e-01i, |S[2][1]| = -1.414e+01, arg(S[2][1]) = -7.235e+01
It 155/300: ω/2π = 5.199e+01 GHz (total elapsed time = 2.00e+02 s)
Calculating boundary modes at wave ports for ω/2π = 5.199e+01 GHz (8.717e-01)
Port 1, mode 1: kₙ = 3.661e+03-1.684e-01i m⁻¹
Port 2, mode 1: kₙ = 3.661e+03-1.684e-01i m⁻¹
Sol. ||E|| = 1.421833e+01
Field energy E (4.241e-04 J) + H (5.521e-04 J) = 9.762e-04 J
S[1][1] = -6.196e-01+5.631e-02i, |S[1][1]| = -4.122e+00, arg(S[1][1]) = +1.748e+02
S[2][1] = +5.747e-02-1.871e-01i, |S[2][1]| = -1.417e+01, arg(S[2][1]) = -7.292e+01
It 156/300: ω/2π = 5.232e+01 GHz (total elapsed time = 2.00e+02 s)
Calculating boundary modes at wave ports for ω/2π = 5.232e+01 GHz (8.773e-01)
Port 1, mode 1: kₙ = 3.685e+03-1.695e-01i m⁻¹
Port 2, mode 1: kₙ = 3.685e+03-1.695e-01i m⁻¹
Sol. ||E|| = 1.421799e+01
Field energy E (4.241e-04 J) + H (5.519e-04 J) = 9.760e-04 J
S[1][1] = -6.188e-01+5.656e-02i, |S[1][1]| = -4.133e+00, arg(S[1][1]) = +1.748e+02
S[2][1] = +5.545e-02-1.871e-01i, |S[2][1]| = -1.419e+01, arg(S[2][1]) = -7.350e+01
It 157/300: ω/2π = 5.265e+01 GHz (total elapsed time = 2.00e+02 s)
Calculating boundary modes at wave ports for ω/2π = 5.265e+01 GHz (8.828e-01)
Port 1, mode 1: kₙ = 3.708e+03-1.706e-01i m⁻¹
Port 2, mode 1: kₙ = 3.708e+03-1.705e-01i m⁻¹
Sol. ||E|| = 1.421770e+01
Field energy E (4.241e-04 J) + H (5.518e-04 J) = 9.759e-04 J
S[1][1] = -6.180e-01+5.681e-02i, |S[1][1]| = -4.143e+00, arg(S[1][1]) = +1.747e+02
S[2][1] = +5.342e-02-1.872e-01i, |S[2][1]| = -1.422e+01, arg(S[2][1]) = -7.407e+01
It 158/300: ω/2π = 5.298e+01 GHz (total elapsed time = 2.01e+02 s)
Calculating boundary modes at wave ports for ω/2π = 5.298e+01 GHz (8.884e-01)
Port 1, mode 1: kₙ = 3.731e+03-1.716e-01i m⁻¹
Port 2, mode 1: kₙ = 3.731e+03-1.716e-01i m⁻¹
Sol. ||E|| = 1.421748e+01
Field energy E (4.241e-04 J) + H (5.517e-04 J) = 9.757e-04 J
S[1][1] = -6.172e-01+5.705e-02i, |S[1][1]| = -4.154e+00, arg(S[1][1]) = +1.747e+02
S[2][1] = +5.140e-02-1.872e-01i, |S[2][1]| = -1.424e+01, arg(S[2][1]) = -7.464e+01
It 159/300: ω/2π = 5.331e+01 GHz (total elapsed time = 2.01e+02 s)
Calculating boundary modes at wave ports for ω/2π = 5.331e+01 GHz (8.939e-01)
Port 1, mode 1: kₙ = 3.755e+03-1.727e-01i m⁻¹
Port 2, mode 1: kₙ = 3.755e+03-1.727e-01i m⁻¹
Sol. ||E|| = 1.421731e+01
Field energy E (4.240e-04 J) + H (5.515e-04 J) = 9.756e-04 J
S[1][1] = -6.165e-01+5.730e-02i, |S[1][1]| = -4.165e+00, arg(S[1][1]) = +1.747e+02
S[2][1] = +4.938e-02-1.872e-01i, |S[2][1]| = -1.426e+01, arg(S[2][1]) = -7.522e+01
It 160/300: ω/2π = 5.365e+01 GHz (total elapsed time = 2.01e+02 s)
Calculating boundary modes at wave ports for ω/2π = 5.365e+01 GHz (8.995e-01)
Port 1, mode 1: kₙ = 3.778e+03-1.738e-01i m⁻¹
Port 2, mode 1: kₙ = 3.778e+03-1.738e-01i m⁻¹
Sol. ||E|| = 1.421719e+01
Field energy E (4.240e-04 J) + H (5.514e-04 J) = 9.754e-04 J
S[1][1] = -6.157e-01+5.754e-02i, |S[1][1]| = -4.175e+00, arg(S[1][1]) = +1.747e+02
S[2][1] = +4.736e-02-1.871e-01i, |S[2][1]| = -1.429e+01, arg(S[2][1]) = -7.580e+01
It 161/300: ω/2π = 5.398e+01 GHz (total elapsed time = 2.02e+02 s)
Calculating boundary modes at wave ports for ω/2π = 5.398e+01 GHz (9.050e-01)
Port 1, mode 1: kₙ = 3.801e+03-1.748e-01i m⁻¹
Port 2, mode 1: kₙ = 3.801e+03-1.748e-01i m⁻¹
Sol. ||E|| = 1.421714e+01
Field energy E (4.240e-04 J) + H (5.513e-04 J) = 9.753e-04 J
S[1][1] = -6.149e-01+5.778e-02i, |S[1][1]| = -4.186e+00, arg(S[1][1]) = +1.746e+02
S[2][1] = +4.534e-02-1.871e-01i, |S[2][1]| = -1.431e+01, arg(S[2][1]) = -7.638e+01
It 162/300: ω/2π = 5.431e+01 GHz (total elapsed time = 2.02e+02 s)
Calculating boundary modes at wave ports for ω/2π = 5.431e+01 GHz (9.106e-01)
Port 1, mode 1: kₙ = 3.825e+03-1.759e-01i m⁻¹
Port 2, mode 1: kₙ = 3.825e+03-1.759e-01i m⁻¹
Sol. ||E|| = 1.421714e+01
Field energy E (4.240e-04 J) + H (5.511e-04 J) = 9.751e-04 J
S[1][1] = -6.141e-01+5.801e-02i, |S[1][1]| = -4.197e+00, arg(S[1][1]) = +1.746e+02
S[2][1] = +4.333e-02-1.870e-01i, |S[2][1]| = -1.434e+01, arg(S[2][1]) = -7.696e+01
It 163/300: ω/2π = 5.464e+01 GHz (total elapsed time = 2.02e+02 s)
Calculating boundary modes at wave ports for ω/2π = 5.464e+01 GHz (9.161e-01)
Port 1, mode 1: kₙ = 3.848e+03-1.770e-01i m⁻¹
Port 2, mode 1: kₙ = 3.848e+03-1.770e-01i m⁻¹
Sol. ||E|| = 1.421719e+01
Field energy E (4.240e-04 J) + H (5.510e-04 J) = 9.750e-04 J
S[1][1] = -6.133e-01+5.825e-02i, |S[1][1]| = -4.207e+00, arg(S[1][1]) = +1.746e+02
S[2][1] = +4.132e-02-1.869e-01i, |S[2][1]| = -1.436e+01, arg(S[2][1]) = -7.754e+01
It 164/300: ω/2π = 5.497e+01 GHz (total elapsed time = 2.02e+02 s)
Calculating boundary modes at wave ports for ω/2π = 5.497e+01 GHz (9.217e-01)
Port 1, mode 1: kₙ = 3.871e+03-1.781e-01i m⁻¹
Port 2, mode 1: kₙ = 3.871e+03-1.780e-01i m⁻¹
Sol. ||E|| = 1.421730e+01
Field energy E (4.240e-04 J) + H (5.508e-04 J) = 9.748e-04 J
S[1][1] = -6.126e-01+5.848e-02i, |S[1][1]| = -4.218e+00, arg(S[1][1]) = +1.745e+02
S[2][1] = +3.931e-02-1.868e-01i, |S[2][1]| = -1.438e+01, arg(S[2][1]) = -7.812e+01
It 165/300: ω/2π = 5.530e+01 GHz (total elapsed time = 2.03e+02 s)
Calculating boundary modes at wave ports for ω/2π = 5.530e+01 GHz (9.272e-01)
Port 1, mode 1: kₙ = 3.895e+03-1.791e-01i m⁻¹
Port 2, mode 1: kₙ = 3.895e+03-1.791e-01i m⁻¹
Sol. ||E|| = 1.421747e+01
Field energy E (4.240e-04 J) + H (5.507e-04 J) = 9.747e-04 J
S[1][1] = -6.118e-01+5.871e-02i, |S[1][1]| = -4.228e+00, arg(S[1][1]) = +1.745e+02
S[2][1] = +3.731e-02-1.867e-01i, |S[2][1]| = -1.441e+01, arg(S[2][1]) = -7.870e+01
It 166/300: ω/2π = 5.563e+01 GHz (total elapsed time = 2.03e+02 s)
Calculating boundary modes at wave ports for ω/2π = 5.563e+01 GHz (9.328e-01)
Port 1, mode 1: kₙ = 3.918e+03-1.802e-01i m⁻¹
Port 2, mode 1: kₙ = 3.918e+03-1.802e-01i m⁻¹
Sol. ||E|| = 1.421769e+01
Field energy E (4.240e-04 J) + H (5.506e-04 J) = 9.746e-04 J
S[1][1] = -6.110e-01+5.894e-02i, |S[1][1]| = -4.239e+00, arg(S[1][1]) = +1.745e+02
S[2][1] = +3.530e-02-1.866e-01i, |S[2][1]| = -1.443e+01, arg(S[2][1]) = -7.928e+01
It 167/300: ω/2π = 5.596e+01 GHz (total elapsed time = 2.03e+02 s)
Calculating boundary modes at wave ports for ω/2π = 5.596e+01 GHz (9.383e-01)
Port 1, mode 1: kₙ = 3.941e+03-1.813e-01i m⁻¹
Port 2, mode 1: kₙ = 3.941e+03-1.813e-01i m⁻¹
Sol. ||E|| = 1.421797e+01
Field energy E (4.240e-04 J) + H (5.504e-04 J) = 9.745e-04 J
S[1][1] = -6.102e-01+5.916e-02i, |S[1][1]| = -4.250e+00, arg(S[1][1]) = +1.745e+02
S[2][1] = +3.331e-02-1.864e-01i, |S[2][1]| = -1.445e+01, arg(S[2][1]) = -7.987e+01
It 168/300: ω/2π = 5.629e+01 GHz (total elapsed time = 2.04e+02 s)
Calculating boundary modes at wave ports for ω/2π = 5.629e+01 GHz (9.439e-01)
Port 1, mode 1: kₙ = 3.965e+03-1.823e-01i m⁻¹
Port 2, mode 1: kₙ = 3.965e+03-1.823e-01i m⁻¹
Sol. ||E|| = 1.421830e+01
Field energy E (4.240e-04 J) + H (5.503e-04 J) = 9.743e-04 J
S[1][1] = -6.095e-01+5.939e-02i, |S[1][1]| = -4.260e+00, arg(S[1][1]) = +1.744e+02
S[2][1] = +3.132e-02-1.862e-01i, |S[2][1]| = -1.448e+01, arg(S[2][1]) = -8.045e+01
It 169/300: ω/2π = 5.663e+01 GHz (total elapsed time = 2.04e+02 s)
Calculating boundary modes at wave ports for ω/2π = 5.663e+01 GHz (9.494e-01)
Port 1, mode 1: kₙ = 3.988e+03-1.834e-01i m⁻¹
Port 2, mode 1: kₙ = 3.988e+03-1.834e-01i m⁻¹
Sol. ||E|| = 1.421868e+01
Field energy E (4.240e-04 J) + H (5.502e-04 J) = 9.742e-04 J
S[1][1] = -6.087e-01+5.961e-02i, |S[1][1]| = -4.271e+00, arg(S[1][1]) = +1.744e+02
S[2][1] = +2.933e-02-1.860e-01i, |S[2][1]| = -1.450e+01, arg(S[2][1]) = -8.104e+01
It 170/300: ω/2π = 5.696e+01 GHz (total elapsed time = 2.04e+02 s)
Calculating boundary modes at wave ports for ω/2π = 5.696e+01 GHz (9.550e-01)
Port 1, mode 1: kₙ = 4.011e+03-1.845e-01i m⁻¹
Port 2, mode 1: kₙ = 4.011e+03-1.845e-01i m⁻¹
Sol. ||E|| = 1.421912e+01
Field energy E (4.241e-04 J) + H (5.500e-04 J) = 9.741e-04 J
S[1][1] = -6.079e-01+5.983e-02i, |S[1][1]| = -4.281e+00, arg(S[1][1]) = +1.744e+02
S[2][1] = +2.734e-02-1.858e-01i, |S[2][1]| = -1.452e+01, arg(S[2][1]) = -8.163e+01
It 171/300: ω/2π = 5.729e+01 GHz (total elapsed time = 2.05e+02 s)
Calculating boundary modes at wave ports for ω/2π = 5.729e+01 GHz (9.605e-01)
Port 1, mode 1: kₙ = 4.034e+03-1.856e-01i m⁻¹
Port 2, mode 1: kₙ = 4.034e+03-1.856e-01i m⁻¹
Sol. ||E|| = 1.421961e+01
Field energy E (4.241e-04 J) + H (5.499e-04 J) = 9.740e-04 J
S[1][1] = -6.071e-01+6.004e-02i, |S[1][1]| = -4.292e+00, arg(S[1][1]) = +1.744e+02
S[2][1] = +2.536e-02-1.856e-01i, |S[2][1]| = -1.455e+01, arg(S[2][1]) = -8.222e+01
It 172/300: ω/2π = 5.762e+01 GHz (total elapsed time = 2.05e+02 s)
Calculating boundary modes at wave ports for ω/2π = 5.762e+01 GHz (9.661e-01)
Port 1, mode 1: kₙ = 4.058e+03-1.866e-01i m⁻¹
Port 2, mode 1: kₙ = 4.058e+03-1.866e-01i m⁻¹
Sol. ||E|| = 1.422016e+01
Field energy E (4.241e-04 J) + H (5.498e-04 J) = 9.739e-04 J
S[1][1] = -6.064e-01+6.026e-02i, |S[1][1]| = -4.302e+00, arg(S[1][1]) = +1.743e+02
S[2][1] = +2.338e-02-1.854e-01i, |S[2][1]| = -1.457e+01, arg(S[2][1]) = -8.281e+01
It 173/300: ω/2π = 5.795e+01 GHz (total elapsed time = 2.05e+02 s)
Calculating boundary modes at wave ports for ω/2π = 5.795e+01 GHz (9.716e-01)
Port 1, mode 1: kₙ = 4.081e+03-1.877e-01i m⁻¹
Port 2, mode 1: kₙ = 4.081e+03-1.877e-01i m⁻¹
Sol. ||E|| = 1.422076e+01
Field energy E (4.241e-04 J) + H (5.496e-04 J) = 9.738e-04 J
S[1][1] = -6.056e-01+6.047e-02i, |S[1][1]| = -4.313e+00, arg(S[1][1]) = +1.743e+02
S[2][1] = +2.141e-02-1.851e-01i, |S[2][1]| = -1.459e+01, arg(S[2][1]) = -8.340e+01
It 174/300: ω/2π = 5.828e+01 GHz (total elapsed time = 2.06e+02 s)
Calculating boundary modes at wave ports for ω/2π = 5.828e+01 GHz (9.772e-01)
Port 1, mode 1: kₙ = 4.104e+03-1.888e-01i m⁻¹
Port 2, mode 1: kₙ = 4.104e+03-1.888e-01i m⁻¹
Sol. ||E|| = 1.422141e+01
Field energy E (4.242e-04 J) + H (5.495e-04 J) = 9.736e-04 J
S[1][1] = -6.048e-01+6.068e-02i, |S[1][1]| = -4.324e+00, arg(S[1][1]) = +1.743e+02
S[2][1] = +1.945e-02-1.848e-01i, |S[2][1]| = -1.462e+01, arg(S[2][1]) = -8.399e+01
It 175/300: ω/2π = 5.861e+01 GHz (total elapsed time = 2.06e+02 s)
Calculating boundary modes at wave ports for ω/2π = 5.861e+01 GHz (9.827e-01)
Port 1, mode 1: kₙ = 4.128e+03-1.899e-01i m⁻¹
Port 2, mode 1: kₙ = 4.128e+03-1.898e-01i m⁻¹
Sol. ||E|| = 1.422211e+01
Field energy E (4.242e-04 J) + H (5.494e-04 J) = 9.735e-04 J
S[1][1] = -6.041e-01+6.088e-02i, |S[1][1]| = -4.334e+00, arg(S[1][1]) = +1.742e+02
S[2][1] = +1.749e-02-1.845e-01i, |S[2][1]| = -1.464e+01, arg(S[2][1]) = -8.459e+01
It 176/300: ω/2π = 5.894e+01 GHz (total elapsed time = 2.06e+02 s)
Calculating boundary modes at wave ports for ω/2π = 5.894e+01 GHz (9.883e-01)
Port 1, mode 1: kₙ = 4.151e+03-1.909e-01i m⁻¹
Port 2, mode 1: kₙ = 4.151e+03-1.909e-01i m⁻¹
Sol. ||E|| = 1.422287e+01
Field energy E (4.242e-04 J) + H (5.492e-04 J) = 9.734e-04 J
S[1][1] = -6.033e-01+6.109e-02i, |S[1][1]| = -4.345e+00, arg(S[1][1]) = +1.742e+02
S[2][1] = +1.553e-02-1.842e-01i, |S[2][1]| = -1.466e+01, arg(S[2][1]) = -8.518e+01
It 177/300: ω/2π = 5.927e+01 GHz (total elapsed time = 2.07e+02 s)
Calculating boundary modes at wave ports for ω/2π = 5.927e+01 GHz (9.938e-01)
Port 1, mode 1: kₙ = 4.174e+03-1.920e-01i m⁻¹
Port 2, mode 1: kₙ = 4.174e+03-1.920e-01i m⁻¹
Sol. ||E|| = 1.422367e+01
Field energy E (4.243e-04 J) + H (5.491e-04 J) = 9.733e-04 J
S[1][1] = -6.026e-01+6.129e-02i, |S[1][1]| = -4.355e+00, arg(S[1][1]) = +1.742e+02
S[2][1] = +1.358e-02-1.839e-01i, |S[2][1]| = -1.469e+01, arg(S[2][1]) = -8.578e+01
It 178/300: ω/2π = 5.961e+01 GHz (total elapsed time = 2.07e+02 s)
Calculating boundary modes at wave ports for ω/2π = 5.961e+01 GHz (9.994e-01)
Port 1, mode 1: kₙ = 4.198e+03-1.931e-01i m⁻¹
Port 2, mode 1: kₙ = 4.198e+03-1.931e-01i m⁻¹
Sol. ||E|| = 1.422453e+01
Field energy E (4.243e-04 J) + H (5.489e-04 J) = 9.732e-04 J
S[1][1] = -6.018e-01+6.149e-02i, |S[1][1]| = -4.366e+00, arg(S[1][1]) = +1.742e+02
S[2][1] = +1.163e-02-1.835e-01i, |S[2][1]| = -1.471e+01, arg(S[2][1]) = -8.637e+01
It 179/300: ω/2π = 5.994e+01 GHz (total elapsed time = 2.07e+02 s)
Calculating boundary modes at wave ports for ω/2π = 5.994e+01 GHz (1.005e+00)
Port 1, mode 1: kₙ = 4.221e+03-1.941e-01i m⁻¹
Port 2, mode 1: kₙ = 4.221e+03-1.941e-01i m⁻¹
Sol. ||E|| = 1.422544e+01
Field energy E (4.244e-04 J) + H (5.488e-04 J) = 9.732e-04 J
S[1][1] = -6.011e-01+6.169e-02i, |S[1][1]| = -4.376e+00, arg(S[1][1]) = +1.741e+02
S[2][1] = +9.695e-03-1.832e-01i, |S[2][1]| = -1.473e+01, arg(S[2][1]) = -8.697e+01
It 180/300: ω/2π = 6.027e+01 GHz (total elapsed time = 2.08e+02 s)
Calculating boundary modes at wave ports for ω/2π = 6.027e+01 GHz (1.010e+00)
Port 1, mode 1: kₙ = 4.244e+03-1.952e-01i m⁻¹
Port 2, mode 1: kₙ = 4.244e+03-1.952e-01i m⁻¹
Sol. ||E|| = 1.422639e+01
Field energy E (4.244e-04 J) + H (5.487e-04 J) = 9.731e-04 J
S[1][1] = -6.003e-01+6.188e-02i, |S[1][1]| = -4.387e+00, arg(S[1][1]) = +1.741e+02
S[2][1] = +7.762e-03-1.828e-01i, |S[2][1]| = -1.475e+01, arg(S[2][1]) = -8.757e+01
It 181/300: ω/2π = 6.060e+01 GHz (total elapsed time = 2.08e+02 s)
Calculating boundary modes at wave ports for ω/2π = 6.060e+01 GHz (1.016e+00)
Port 1, mode 1: kₙ = 4.268e+03-1.963e-01i m⁻¹
Port 2, mode 1: kₙ = 4.268e+03-1.963e-01i m⁻¹
Sol. ||E|| = 1.422740e+01
Field energy E (4.245e-04 J) + H (5.485e-04 J) = 9.730e-04 J
S[1][1] = -5.996e-01+6.208e-02i, |S[1][1]| = -4.397e+00, arg(S[1][1]) = +1.741e+02
S[2][1] = +5.834e-03-1.824e-01i, |S[2][1]| = -1.477e+01, arg(S[2][1]) = -8.817e+01
It 182/300: ω/2π = 6.093e+01 GHz (total elapsed time = 2.08e+02 s)
Calculating boundary modes at wave ports for ω/2π = 6.093e+01 GHz (1.022e+00)
Port 1, mode 1: kₙ = 4.291e+03-1.974e-01i m⁻¹
Port 2, mode 1: kₙ = 4.291e+03-1.973e-01i m⁻¹
Sol. ||E|| = 1.422846e+01
Field energy E (4.245e-04 J) + H (5.484e-04 J) = 9.729e-04 J
S[1][1] = -5.988e-01+6.227e-02i, |S[1][1]| = -4.407e+00, arg(S[1][1]) = +1.741e+02
S[2][1] = +3.913e-03-1.820e-01i, |S[2][1]| = -1.480e+01, arg(S[2][1]) = -8.877e+01
It 183/300: ω/2π = 6.126e+01 GHz (total elapsed time = 2.08e+02 s)
Calculating boundary modes at wave ports for ω/2π = 6.126e+01 GHz (1.027e+00)
Port 1, mode 1: kₙ = 4.314e+03-1.984e-01i m⁻¹
Port 2, mode 1: kₙ = 4.314e+03-1.984e-01i m⁻¹
Sol. ||E|| = 1.422956e+01
Field energy E (4.246e-04 J) + H (5.482e-04 J) = 9.728e-04 J
S[1][1] = -5.981e-01+6.245e-02i, |S[1][1]| = -4.418e+00, arg(S[1][1]) = +1.740e+02
S[2][1] = +1.999e-03-1.816e-01i, |S[2][1]| = -1.482e+01, arg(S[2][1]) = -8.937e+01
It 184/300: ω/2π = 6.159e+01 GHz (total elapsed time = 2.09e+02 s)
Calculating boundary modes at wave ports for ω/2π = 6.159e+01 GHz (1.033e+00)
Port 1, mode 1: kₙ = 4.338e+03-1.995e-01i m⁻¹
Port 2, mode 1: kₙ = 4.338e+03-1.995e-01i m⁻¹
Sol. ||E|| = 1.423072e+01
Field energy E (4.246e-04 J) + H (5.481e-04 J) = 9.727e-04 J
S[1][1] = -5.973e-01+6.264e-02i, |S[1][1]| = -4.428e+00, arg(S[1][1]) = +1.740e+02
S[2][1] = +9.044e-05-1.811e-01i, |S[2][1]| = -1.484e+01, arg(S[2][1]) = -8.997e+01
It 185/300: ω/2π = 6.192e+01 GHz (total elapsed time = 2.09e+02 s)
Calculating boundary modes at wave ports for ω/2π = 6.192e+01 GHz (1.038e+00)
Port 1, mode 1: kₙ = 4.361e+03-2.006e-01i m⁻¹
Port 2, mode 1: kₙ = 4.361e+03-2.006e-01i m⁻¹
Sol. ||E|| = 1.423192e+01
Field energy E (4.247e-04 J) + H (5.480e-04 J) = 9.727e-04 J
S[1][1] = -5.966e-01+6.282e-02i, |S[1][1]| = -4.439e+00, arg(S[1][1]) = +1.740e+02
S[2][1] = -1.811e-03-1.806e-01i, |S[2][1]| = -1.486e+01, arg(S[2][1]) = -9.057e+01
It 186/300: ω/2π = 6.225e+01 GHz (total elapsed time = 2.09e+02 s)
Calculating boundary modes at wave ports for ω/2π = 6.225e+01 GHz (1.044e+00)
Port 1, mode 1: kₙ = 4.384e+03-2.017e-01i m⁻¹
Port 2, mode 1: kₙ = 4.384e+03-2.016e-01i m⁻¹
Sol. ||E|| = 1.423317e+01
Field energy E (4.248e-04 J) + H (5.478e-04 J) = 9.726e-04 J
S[1][1] = -5.958e-01+6.300e-02i, |S[1][1]| = -4.449e+00, arg(S[1][1]) = +1.740e+02
S[2][1] = -3.705e-03-1.802e-01i, |S[2][1]| = -1.488e+01, arg(S[2][1]) = -9.118e+01
It 187/300: ω/2π = 6.259e+01 GHz (total elapsed time = 2.10e+02 s)
Calculating boundary modes at wave ports for ω/2π = 6.259e+01 GHz (1.049e+00)
Port 1, mode 1: kₙ = 4.408e+03-2.027e-01i m⁻¹
Port 2, mode 1: kₙ = 4.408e+03-2.027e-01i m⁻¹
Sol. ||E|| = 1.423447e+01
Field energy E (4.248e-04 J) + H (5.477e-04 J) = 9.725e-04 J
S[1][1] = -5.951e-01+6.318e-02i, |S[1][1]| = -4.459e+00, arg(S[1][1]) = +1.739e+02
S[2][1] = -5.593e-03-1.797e-01i, |S[2][1]| = -1.491e+01, arg(S[2][1]) = -9.178e+01
It 188/300: ω/2π = 6.292e+01 GHz (total elapsed time = 2.10e+02 s)
Calculating boundary modes at wave ports for ω/2π = 6.292e+01 GHz (1.055e+00)
Port 1, mode 1: kₙ = 4.431e+03-2.038e-01i m⁻¹
Port 2, mode 1: kₙ = 4.431e+03-2.038e-01i m⁻¹
Sol. ||E|| = 1.423581e+01
Field energy E (4.249e-04 J) + H (5.475e-04 J) = 9.724e-04 J
S[1][1] = -5.944e-01+6.336e-02i, |S[1][1]| = -4.470e+00, arg(S[1][1]) = +1.739e+02
S[2][1] = -7.473e-03-1.792e-01i, |S[2][1]| = -1.493e+01, arg(S[2][1]) = -9.239e+01
It 189/300: ω/2π = 6.325e+01 GHz (total elapsed time = 2.10e+02 s)
Calculating boundary modes at wave ports for ω/2π = 6.325e+01 GHz (1.060e+00)
Port 1, mode 1: kₙ = 4.454e+03-2.049e-01i m⁻¹
Port 2, mode 1: kₙ = 4.454e+03-2.049e-01i m⁻¹
Sol. ||E|| = 1.423720e+01
Field energy E (4.250e-04 J) + H (5.474e-04 J) = 9.724e-04 J
S[1][1] = -5.936e-01+6.353e-02i, |S[1][1]| = -4.480e+00, arg(S[1][1]) = +1.739e+02
S[2][1] = -9.346e-03-1.786e-01i, |S[2][1]| = -1.495e+01, arg(S[2][1]) = -9.300e+01
It 190/300: ω/2π = 6.358e+01 GHz (total elapsed time = 2.11e+02 s)
Calculating boundary modes at wave ports for ω/2π = 6.358e+01 GHz (1.066e+00)
Port 1, mode 1: kₙ = 4.477e+03-2.059e-01i m⁻¹
Port 2, mode 1: kₙ = 4.478e+03-2.059e-01i m⁻¹
Sol. ||E|| = 1.423863e+01
Field energy E (4.251e-04 J) + H (5.473e-04 J) = 9.723e-04 J
S[1][1] = -5.929e-01+6.370e-02i, |S[1][1]| = -4.490e+00, arg(S[1][1]) = +1.739e+02
S[2][1] = -1.121e-02-1.781e-01i, |S[2][1]| = -1.497e+01, arg(S[2][1]) = -9.360e+01
It 191/300: ω/2π = 6.391e+01 GHz (total elapsed time = 2.11e+02 s)
Calculating boundary modes at wave ports for ω/2π = 6.391e+01 GHz (1.072e+00)
Port 1, mode 1: kₙ = 4.501e+03-2.070e-01i m⁻¹
Port 2, mode 1: kₙ = 4.501e+03-2.070e-01i m⁻¹
Sol. ||E|| = 1.424011e+01
Field energy E (4.251e-04 J) + H (5.471e-04 J) = 9.722e-04 J
S[1][1] = -5.922e-01+6.387e-02i, |S[1][1]| = -4.501e+00, arg(S[1][1]) = +1.738e+02
S[2][1] = -1.307e-02-1.775e-01i, |S[2][1]| = -1.499e+01, arg(S[2][1]) = -9.421e+01
It 192/300: ω/2π = 6.424e+01 GHz (total elapsed time = 2.11e+02 s)
Calculating boundary modes at wave ports for ω/2π = 6.424e+01 GHz (1.077e+00)
Port 1, mode 1: kₙ = 4.524e+03-2.081e-01i m⁻¹
Port 2, mode 1: kₙ = 4.524e+03-2.081e-01i m⁻¹
Sol. ||E|| = 1.424164e+01
Field energy E (4.252e-04 J) + H (5.470e-04 J) = 9.722e-04 J
S[1][1] = -5.915e-01+6.404e-02i, |S[1][1]| = -4.511e+00, arg(S[1][1]) = +1.738e+02
S[2][1] = -1.492e-02-1.769e-01i, |S[2][1]| = -1.501e+01, arg(S[2][1]) = -9.482e+01
It 193/300: ω/2π = 6.457e+01 GHz (total elapsed time = 2.12e+02 s)
Calculating boundary modes at wave ports for ω/2π = 6.457e+01 GHz (1.083e+00)
Port 1, mode 1: kₙ = 4.547e+03-2.092e-01i m⁻¹
Port 2, mode 1: kₙ = 4.547e+03-2.091e-01i m⁻¹
Sol. ||E|| = 1.424321e+01
Field energy E (4.253e-04 J) + H (5.468e-04 J) = 9.721e-04 J
S[1][1] = -5.907e-01+6.420e-02i, |S[1][1]| = -4.521e+00, arg(S[1][1]) = +1.738e+02
S[2][1] = -1.676e-02-1.763e-01i, |S[2][1]| = -1.503e+01, arg(S[2][1]) = -9.543e+01
It 194/300: ω/2π = 6.490e+01 GHz (total elapsed time = 2.12e+02 s)
Calculating boundary modes at wave ports for ω/2π = 6.490e+01 GHz (1.088e+00)
Port 1, mode 1: kₙ = 4.571e+03-2.102e-01i m⁻¹
Port 2, mode 1: kₙ = 4.571e+03-2.102e-01i m⁻¹
Sol. ||E|| = 1.424482e+01
Field energy E (4.254e-04 J) + H (5.467e-04 J) = 9.721e-04 J
S[1][1] = -5.900e-01+6.436e-02i, |S[1][1]| = -4.531e+00, arg(S[1][1]) = +1.738e+02
S[2][1] = -1.859e-02-1.757e-01i, |S[2][1]| = -1.506e+01, arg(S[2][1]) = -9.604e+01
It 195/300: ω/2π = 6.523e+01 GHz (total elapsed time = 2.12e+02 s)
Calculating boundary modes at wave ports for ω/2π = 6.523e+01 GHz (1.094e+00)
Port 1, mode 1: kₙ = 4.594e+03-2.113e-01i m⁻¹
Port 2, mode 1: kₙ = 4.594e+03-2.113e-01i m⁻¹
Sol. ||E|| = 1.424647e+01
Field energy E (4.255e-04 J) + H (5.465e-04 J) = 9.720e-04 J
S[1][1] = -5.893e-01+6.452e-02i, |S[1][1]| = -4.542e+00, arg(S[1][1]) = +1.738e+02
S[2][1] = -2.042e-02-1.751e-01i, |S[2][1]| = -1.508e+01, arg(S[2][1]) = -9.665e+01
It 196/300: ω/2π = 6.557e+01 GHz (total elapsed time = 2.13e+02 s)
Calculating boundary modes at wave ports for ω/2π = 6.557e+01 GHz (1.099e+00)
Port 1, mode 1: kₙ = 4.617e+03-2.124e-01i m⁻¹
Port 2, mode 1: kₙ = 4.617e+03-2.124e-01i m⁻¹
Sol. ||E|| = 1.424817e+01
Field energy E (4.256e-04 J) + H (5.464e-04 J) = 9.720e-04 J
S[1][1] = -5.886e-01+6.468e-02i, |S[1][1]| = -4.552e+00, arg(S[1][1]) = +1.737e+02
S[2][1] = -2.223e-02-1.744e-01i, |S[2][1]| = -1.510e+01, arg(S[2][1]) = -9.726e+01
It 197/300: ω/2π = 6.590e+01 GHz (total elapsed time = 2.13e+02 s)
Calculating boundary modes at wave ports for ω/2π = 6.590e+01 GHz (1.105e+00)
Port 1, mode 1: kₙ = 4.641e+03-2.134e-01i m⁻¹
Port 2, mode 1: kₙ = 4.641e+03-2.134e-01i m⁻¹
Sol. ||E|| = 1.424991e+01
Field energy E (4.257e-04 J) + H (5.462e-04 J) = 9.719e-04 J
S[1][1] = -5.879e-01+6.483e-02i, |S[1][1]| = -4.562e+00, arg(S[1][1]) = +1.737e+02
S[2][1] = -2.404e-02-1.738e-01i, |S[2][1]| = -1.512e+01, arg(S[2][1]) = -9.788e+01
It 198/300: ω/2π = 6.623e+01 GHz (total elapsed time = 2.13e+02 s)
Calculating boundary modes at wave ports for ω/2π = 6.623e+01 GHz (1.110e+00)
Port 1, mode 1: kₙ = 4.664e+03-2.145e-01i m⁻¹
Port 2, mode 1: kₙ = 4.664e+03-2.145e-01i m⁻¹
Sol. ||E|| = 1.425169e+01
Field energy E (4.258e-04 J) + H (5.461e-04 J) = 9.719e-04 J
S[1][1] = -5.872e-01+6.498e-02i, |S[1][1]| = -4.572e+00, arg(S[1][1]) = +1.737e+02
S[2][1] = -2.584e-02-1.731e-01i, |S[2][1]| = -1.514e+01, arg(S[2][1]) = -9.849e+01
It 199/300: ω/2π = 6.656e+01 GHz (total elapsed time = 2.14e+02 s)
Calculating boundary modes at wave ports for ω/2π = 6.656e+01 GHz (1.116e+00)
Port 1, mode 1: kₙ = 4.687e+03-2.156e-01i m⁻¹
Port 2, mode 1: kₙ = 4.687e+03-2.156e-01i m⁻¹
Sol. ||E|| = 1.425351e+01
Field energy E (4.259e-04 J) + H (5.460e-04 J) = 9.718e-04 J
S[1][1] = -5.864e-01+6.513e-02i, |S[1][1]| = -4.582e+00, arg(S[1][1]) = +1.737e+02
S[2][1] = -2.763e-02-1.724e-01i, |S[2][1]| = -1.516e+01, arg(S[2][1]) = -9.911e+01
It 200/300: ω/2π = 6.689e+01 GHz (total elapsed time = 2.14e+02 s)
Calculating boundary modes at wave ports for ω/2π = 6.689e+01 GHz (1.122e+00)
Port 1, mode 1: kₙ = 4.711e+03-2.167e-01i m⁻¹
Port 2, mode 1: kₙ = 4.711e+03-2.166e-01i m⁻¹
Sol. ||E|| = 1.425537e+01
Field energy E (4.260e-04 J) + H (5.458e-04 J) = 9.718e-04 J
S[1][1] = -5.857e-01+6.528e-02i, |S[1][1]| = -4.592e+00, arg(S[1][1]) = +1.736e+02
S[2][1] = -2.941e-02-1.717e-01i, |S[2][1]| = -1.518e+01, arg(S[2][1]) = -9.972e+01
It 201/300: ω/2π = 6.722e+01 GHz (total elapsed time = 2.14e+02 s)
Calculating boundary modes at wave ports for ω/2π = 6.722e+01 GHz (1.127e+00)
Port 1, mode 1: kₙ = 4.734e+03-2.177e-01i m⁻¹
Port 2, mode 1: kₙ = 4.734e+03-2.177e-01i m⁻¹
Sol. ||E|| = 1.425728e+01
Field energy E (4.261e-04 J) + H (5.457e-04 J) = 9.717e-04 J
S[1][1] = -5.850e-01+6.542e-02i, |S[1][1]| = -4.602e+00, arg(S[1][1]) = +1.736e+02
S[2][1] = -3.118e-02-1.710e-01i, |S[2][1]| = -1.520e+01, arg(S[2][1]) = -1.003e+02
It 202/300: ω/2π = 6.755e+01 GHz (total elapsed time = 2.15e+02 s)
Calculating boundary modes at wave ports for ω/2π = 6.755e+01 GHz (1.133e+00)
Port 1, mode 1: kₙ = 4.757e+03-2.188e-01i m⁻¹
Port 2, mode 1: kₙ = 4.757e+03-2.188e-01i m⁻¹
Sol. ||E|| = 1.425922e+01
Field energy E (4.262e-04 J) + H (5.455e-04 J) = 9.717e-04 J
S[1][1] = -5.843e-01+6.556e-02i, |S[1][1]| = -4.612e+00, arg(S[1][1]) = +1.736e+02
S[2][1] = -3.295e-02-1.702e-01i, |S[2][1]| = -1.522e+01, arg(S[2][1]) = -1.010e+02
It 203/300: ω/2π = 6.788e+01 GHz (total elapsed time = 2.15e+02 s)
Calculating boundary modes at wave ports for ω/2π = 6.788e+01 GHz (1.138e+00)
Port 1, mode 1: kₙ = 4.781e+03-2.199e-01i m⁻¹
Port 2, mode 1: kₙ = 4.781e+03-2.199e-01i m⁻¹
Sol. ||E|| = 1.426120e+01
Field energy E (4.263e-04 J) + H (5.454e-04 J) = 9.717e-04 J
S[1][1] = -5.836e-01+6.570e-02i, |S[1][1]| = -4.622e+00, arg(S[1][1]) = +1.736e+02
S[2][1] = -3.470e-02-1.695e-01i, |S[2][1]| = -1.524e+01, arg(S[2][1]) = -1.016e+02
It 204/300: ω/2π = 6.821e+01 GHz (total elapsed time = 2.15e+02 s)
Calculating boundary modes at wave ports for ω/2π = 6.821e+01 GHz (1.144e+00)
Port 1, mode 1: kₙ = 4.804e+03-2.210e-01i m⁻¹
Port 2, mode 1: kₙ = 4.804e+03-2.209e-01i m⁻¹
Sol. ||E|| = 1.426321e+01
Field energy E (4.264e-04 J) + H (5.452e-04 J) = 9.716e-04 J
S[1][1] = -5.829e-01+6.584e-02i, |S[1][1]| = -4.632e+00, arg(S[1][1]) = +1.736e+02
S[2][1] = -3.644e-02-1.687e-01i, |S[2][1]| = -1.526e+01, arg(S[2][1]) = -1.022e+02
It 205/300: ω/2π = 6.855e+01 GHz (total elapsed time = 2.16e+02 s)
Calculating boundary modes at wave ports for ω/2π = 6.855e+01 GHz (1.149e+00)
Port 1, mode 1: kₙ = 4.827e+03-2.220e-01i m⁻¹
Port 2, mode 1: kₙ = 4.827e+03-2.220e-01i m⁻¹
Sol. ||E|| = 1.426527e+01
Field energy E (4.265e-04 J) + H (5.451e-04 J) = 9.716e-04 J
S[1][1] = -5.823e-01+6.597e-02i, |S[1][1]| = -4.642e+00, arg(S[1][1]) = +1.735e+02
S[2][1] = -3.817e-02-1.679e-01i, |S[2][1]| = -1.528e+01, arg(S[2][1]) = -1.028e+02
It 206/300: ω/2π = 6.888e+01 GHz (total elapsed time = 2.16e+02 s)
Calculating boundary modes at wave ports for ω/2π = 6.888e+01 GHz (1.155e+00)
Port 1, mode 1: kₙ = 4.851e+03-2.231e-01i m⁻¹
Port 2, mode 1: kₙ = 4.851e+03-2.231e-01i m⁻¹
Sol. ||E|| = 1.426736e+01
Field energy E (4.266e-04 J) + H (5.449e-04 J) = 9.716e-04 J
S[1][1] = -5.816e-01+6.610e-02i, |S[1][1]| = -4.652e+00, arg(S[1][1]) = +1.735e+02
S[2][1] = -3.990e-02-1.671e-01i, |S[2][1]| = -1.530e+01, arg(S[2][1]) = -1.034e+02
It 207/300: ω/2π = 6.921e+01 GHz (total elapsed time = 2.16e+02 s)
Calculating boundary modes at wave ports for ω/2π = 6.921e+01 GHz (1.160e+00)
Port 1, mode 1: kₙ = 4.874e+03-2.242e-01i m⁻¹
Port 2, mode 1: kₙ = 4.874e+03-2.242e-01i m⁻¹
Sol. ||E|| = 1.426949e+01
Field energy E (4.268e-04 J) + H (5.448e-04 J) = 9.716e-04 J
S[1][1] = -5.809e-01+6.623e-02i, |S[1][1]| = -4.662e+00, arg(S[1][1]) = +1.735e+02
S[2][1] = -4.161e-02-1.663e-01i, |S[2][1]| = -1.532e+01, arg(S[2][1]) = -1.040e+02
It 208/300: ω/2π = 6.954e+01 GHz (total elapsed time = 2.17e+02 s)
Calculating boundary modes at wave ports for ω/2π = 6.954e+01 GHz (1.166e+00)
Port 1, mode 1: kₙ = 4.897e+03-2.252e-01i m⁻¹
Port 2, mode 1: kₙ = 4.897e+03-2.252e-01i m⁻¹
Sol. ||E|| = 1.427166e+01
Field energy E (4.269e-04 J) + H (5.446e-04 J) = 9.715e-04 J
S[1][1] = -5.802e-01+6.636e-02i, |S[1][1]| = -4.672e+00, arg(S[1][1]) = +1.735e+02
S[2][1] = -4.331e-02-1.654e-01i, |S[2][1]| = -1.534e+01, arg(S[2][1]) = -1.047e+02
It 209/300: ω/2π = 6.987e+01 GHz (total elapsed time = 2.17e+02 s)
Calculating boundary modes at wave ports for ω/2π = 6.987e+01 GHz (1.171e+00)
Port 1, mode 1: kₙ = 4.921e+03-2.263e-01i m⁻¹
Port 2, mode 1: kₙ = 4.921e+03-2.263e-01i m⁻¹
Sol. ||E|| = 1.427386e+01
Field energy E (4.270e-04 J) + H (5.445e-04 J) = 9.715e-04 J
S[1][1] = -5.795e-01+6.649e-02i, |S[1][1]| = -4.682e+00, arg(S[1][1]) = +1.735e+02
S[2][1] = -4.500e-02-1.646e-01i, |S[2][1]| = -1.536e+01, arg(S[2][1]) = -1.053e+02
It 210/300: ω/2π = 7.020e+01 GHz (total elapsed time = 2.17e+02 s)
Calculating boundary modes at wave ports for ω/2π = 7.020e+01 GHz (1.177e+00)
Port 1, mode 1: kₙ = 4.944e+03-2.274e-01i m⁻¹
Port 2, mode 1: kₙ = 4.944e+03-2.274e-01i m⁻¹
Sol. ||E|| = 1.427609e+01
Field energy E (4.271e-04 J) + H (5.443e-04 J) = 9.715e-04 J
S[1][1] = -5.788e-01+6.661e-02i, |S[1][1]| = -4.692e+00, arg(S[1][1]) = +1.734e+02
S[2][1] = -4.668e-02-1.637e-01i, |S[2][1]| = -1.538e+01, arg(S[2][1]) = -1.059e+02
It 211/300: ω/2π = 7.053e+01 GHz (total elapsed time = 2.18e+02 s)
Calculating boundary modes at wave ports for ω/2π = 7.053e+01 GHz (1.183e+00)
Port 1, mode 1: kₙ = 4.967e+03-2.285e-01i m⁻¹
Port 2, mode 1: kₙ = 4.967e+03-2.284e-01i m⁻¹
Sol. ||E|| = 1.427836e+01
Field energy E (4.273e-04 J) + H (5.442e-04 J) = 9.715e-04 J
S[1][1] = -5.782e-01+6.673e-02i, |S[1][1]| = -4.702e+00, arg(S[1][1]) = +1.734e+02
S[2][1] = -4.835e-02-1.628e-01i, |S[2][1]| = -1.540e+01, arg(S[2][1]) = -1.065e+02
It 212/300: ω/2π = 7.086e+01 GHz (total elapsed time = 2.18e+02 s)
Calculating boundary modes at wave ports for ω/2π = 7.086e+01 GHz (1.188e+00)
Port 1, mode 1: kₙ = 4.990e+03-2.295e-01i m⁻¹
Port 2, mode 1: kₙ = 4.990e+03-2.295e-01i m⁻¹
Sol. ||E|| = 1.428067e+01
Field energy E (4.274e-04 J) + H (5.440e-04 J) = 9.714e-04 J
S[1][1] = -5.775e-01+6.685e-02i, |S[1][1]| = -4.711e+00, arg(S[1][1]) = +1.734e+02
S[2][1] = -5.001e-02-1.619e-01i, |S[2][1]| = -1.542e+01, arg(S[2][1]) = -1.072e+02
It 213/300: ω/2π = 7.119e+01 GHz (total elapsed time = 2.18e+02 s)
Calculating boundary modes at wave ports for ω/2π = 7.119e+01 GHz (1.194e+00)
Port 1, mode 1: kₙ = 5.014e+03-2.306e-01i m⁻¹
Port 2, mode 1: kₙ = 5.014e+03-2.306e-01i m⁻¹
Sol. ||E|| = 1.428300e+01
Field energy E (4.275e-04 J) + H (5.439e-04 J) = 9.714e-04 J
S[1][1] = -5.768e-01+6.696e-02i, |S[1][1]| = -4.721e+00, arg(S[1][1]) = +1.734e+02
S[2][1] = -5.166e-02-1.610e-01i, |S[2][1]| = -1.544e+01, arg(S[2][1]) = -1.078e+02
It 214/300: ω/2π = 7.153e+01 GHz (total elapsed time = 2.19e+02 s)
Calculating boundary modes at wave ports for ω/2π = 7.153e+01 GHz (1.199e+00)
Port 1, mode 1: kₙ = 5.037e+03-2.317e-01i m⁻¹
Port 2, mode 1: kₙ = 5.037e+03-2.317e-01i m⁻¹
Sol. ||E|| = 1.428537e+01
Field energy E (4.277e-04 J) + H (5.437e-04 J) = 9.714e-04 J
S[1][1] = -5.761e-01+6.708e-02i, |S[1][1]| = -4.731e+00, arg(S[1][1]) = +1.734e+02
S[2][1] = -5.330e-02-1.601e-01i, |S[2][1]| = -1.546e+01, arg(S[2][1]) = -1.084e+02
It 215/300: ω/2π = 7.186e+01 GHz (total elapsed time = 2.19e+02 s)
Calculating boundary modes at wave ports for ω/2π = 7.186e+01 GHz (1.205e+00)
Port 1, mode 1: kₙ = 5.060e+03-2.327e-01i m⁻¹
Port 2, mode 1: kₙ = 5.060e+03-2.327e-01i m⁻¹
Sol. ||E|| = 1.428777e+01
Field energy E (4.278e-04 J) + H (5.436e-04 J) = 9.714e-04 J
S[1][1] = -5.755e-01+6.719e-02i, |S[1][1]| = -4.741e+00, arg(S[1][1]) = +1.733e+02
S[2][1] = -5.493e-02-1.592e-01i, |S[2][1]| = -1.547e+01, arg(S[2][1]) = -1.090e+02
It 216/300: ω/2π = 7.219e+01 GHz (total elapsed time = 2.19e+02 s)
Calculating boundary modes at wave ports for ω/2π = 7.219e+01 GHz (1.210e+00)
Port 1, mode 1: kₙ = 5.084e+03-2.338e-01i m⁻¹
Port 2, mode 1: kₙ = 5.084e+03-2.338e-01i m⁻¹
Sol. ||E|| = 1.429020e+01
Field energy E (4.279e-04 J) + H (5.434e-04 J) = 9.714e-04 J
S[1][1] = -5.748e-01+6.729e-02i, |S[1][1]| = -4.750e+00, arg(S[1][1]) = +1.733e+02
S[2][1] = -5.654e-02-1.582e-01i, |S[2][1]| = -1.549e+01, arg(S[2][1]) = -1.097e+02
It 217/300: ω/2π = 7.252e+01 GHz (total elapsed time = 2.20e+02 s)
Calculating boundary modes at wave ports for ω/2π = 7.252e+01 GHz (1.216e+00)
Port 1, mode 1: kₙ = 5.107e+03-2.349e-01i m⁻¹
Port 2, mode 1: kₙ = 5.107e+03-2.349e-01i m⁻¹
Sol. ||E|| = 1.429267e+01
Field energy E (4.281e-04 J) + H (5.433e-04 J) = 9.714e-04 J
S[1][1] = -5.742e-01+6.740e-02i, |S[1][1]| = -4.760e+00, arg(S[1][1]) = +1.733e+02
S[2][1] = -5.814e-02-1.573e-01i, |S[2][1]| = -1.551e+01, arg(S[2][1]) = -1.103e+02
It 218/300: ω/2π = 7.285e+01 GHz (total elapsed time = 2.20e+02 s)
Calculating boundary modes at wave ports for ω/2π = 7.285e+01 GHz (1.221e+00)
Port 1, mode 1: kₙ = 5.130e+03-2.360e-01i m⁻¹
Port 2, mode 1: kₙ = 5.130e+03-2.359e-01i m⁻¹
Sol. ||E|| = 1.429516e+01
Field energy E (4.282e-04 J) + H (5.431e-04 J) = 9.714e-04 J
S[1][1] = -5.735e-01+6.750e-02i, |S[1][1]| = -4.769e+00, arg(S[1][1]) = +1.733e+02
S[2][1] = -5.973e-02-1.563e-01i, |S[2][1]| = -1.553e+01, arg(S[2][1]) = -1.109e+02
It 219/300: ω/2π = 7.318e+01 GHz (total elapsed time = 2.20e+02 s)
Calculating boundary modes at wave ports for ω/2π = 7.318e+01 GHz (1.227e+00)
Port 1, mode 1: kₙ = 5.154e+03-2.370e-01i m⁻¹
Port 2, mode 1: kₙ = 5.154e+03-2.370e-01i m⁻¹
Sol. ||E|| = 1.429768e+01
Field energy E (4.284e-04 J) + H (5.430e-04 J) = 9.714e-04 J
S[1][1] = -5.729e-01+6.761e-02i, |S[1][1]| = -4.779e+00, arg(S[1][1]) = +1.733e+02
S[2][1] = -6.131e-02-1.553e-01i, |S[2][1]| = -1.555e+01, arg(S[2][1]) = -1.115e+02
It 220/300: ω/2π = 7.351e+01 GHz (total elapsed time = 2.21e+02 s)
Calculating boundary modes at wave ports for ω/2π = 7.351e+01 GHz (1.233e+00)
Port 1, mode 1: kₙ = 5.177e+03-2.381e-01i m⁻¹
Port 2, mode 1: kₙ = 5.177e+03-2.381e-01i m⁻¹
Sol. ||E|| = 1.430023e+01
Field energy E (4.285e-04 J) + H (5.429e-04 J) = 9.714e-04 J
S[1][1] = -5.722e-01+6.771e-02i, |S[1][1]| = -4.788e+00, arg(S[1][1]) = +1.733e+02
S[2][1] = -6.288e-02-1.543e-01i, |S[2][1]| = -1.557e+01, arg(S[2][1]) = -1.122e+02
It 221/300: ω/2π = 7.384e+01 GHz (total elapsed time = 2.21e+02 s)
Calculating boundary modes at wave ports for ω/2π = 7.384e+01 GHz (1.238e+00)
Port 1, mode 1: kₙ = 5.200e+03-2.392e-01i m⁻¹
Port 2, mode 1: kₙ = 5.200e+03-2.392e-01i m⁻¹
Sol. ||E|| = 1.430281e+01
Field energy E (4.287e-04 J) + H (5.427e-04 J) = 9.714e-04 J
S[1][1] = -5.716e-01+6.780e-02i, |S[1][1]| = -4.798e+00, arg(S[1][1]) = +1.732e+02
S[2][1] = -6.443e-02-1.532e-01i, |S[2][1]| = -1.559e+01, arg(S[2][1]) = -1.128e+02
It 222/300: ω/2π = 7.417e+01 GHz (total elapsed time = 2.21e+02 s)
Calculating boundary modes at wave ports for ω/2π = 7.417e+01 GHz (1.244e+00)
Port 1, mode 1: kₙ = 5.224e+03-2.402e-01i m⁻¹
Port 2, mode 1: kₙ = 5.224e+03-2.402e-01i m⁻¹
Sol. ||E|| = 1.430542e+01
Field energy E (4.288e-04 J) + H (5.426e-04 J) = 9.714e-04 J
S[1][1] = -5.709e-01+6.790e-02i, |S[1][1]| = -4.807e+00, arg(S[1][1]) = +1.732e+02
S[2][1] = -6.598e-02-1.522e-01i, |S[2][1]| = -1.560e+01, arg(S[2][1]) = -1.134e+02
It 223/300: ω/2π = 7.451e+01 GHz (total elapsed time = 2.22e+02 s)
Calculating boundary modes at wave ports for ω/2π = 7.451e+01 GHz (1.249e+00)
Port 1, mode 1: kₙ = 5.247e+03-2.413e-01i m⁻¹
Port 2, mode 1: kₙ = 5.247e+03-2.413e-01i m⁻¹
Sol. ||E|| = 1.430805e+01
Field energy E (4.290e-04 J) + H (5.424e-04 J) = 9.714e-04 J
S[1][1] = -5.703e-01+6.799e-02i, |S[1][1]| = -4.817e+00, arg(S[1][1]) = +1.732e+02
S[2][1] = -6.751e-02-1.512e-01i, |S[2][1]| = -1.562e+01, arg(S[2][1]) = -1.141e+02
It 224/300: ω/2π = 7.484e+01 GHz (total elapsed time = 2.22e+02 s)
Calculating boundary modes at wave ports for ω/2π = 7.484e+01 GHz (1.255e+00)
Port 1, mode 1: kₙ = 5.270e+03-2.424e-01i m⁻¹
Port 2, mode 1: kₙ = 5.270e+03-2.424e-01i m⁻¹
Sol. ||E|| = 1.431072e+01
Field energy E (4.291e-04 J) + H (5.423e-04 J) = 9.714e-04 J
S[1][1] = -5.696e-01+6.808e-02i, |S[1][1]| = -4.826e+00, arg(S[1][1]) = +1.732e+02
S[2][1] = -6.902e-02-1.501e-01i, |S[2][1]| = -1.564e+01, arg(S[2][1]) = -1.147e+02
It 225/300: ω/2π = 7.517e+01 GHz (total elapsed time = 2.23e+02 s)
Calculating boundary modes at wave ports for ω/2π = 7.517e+01 GHz (1.260e+00)
Port 1, mode 1: kₙ = 5.294e+03-2.435e-01i m⁻¹
Port 2, mode 1: kₙ = 5.294e+03-2.434e-01i m⁻¹
Sol. ||E|| = 1.431340e+01
Field energy E (4.293e-04 J) + H (5.421e-04 J) = 9.714e-04 J
S[1][1] = -5.690e-01+6.817e-02i, |S[1][1]| = -4.836e+00, arg(S[1][1]) = +1.732e+02
S[2][1] = -7.053e-02-1.490e-01i, |S[2][1]| = -1.566e+01, arg(S[2][1]) = -1.153e+02
It 226/300: ω/2π = 7.550e+01 GHz (total elapsed time = 2.23e+02 s)
Calculating boundary modes at wave ports for ω/2π = 7.550e+01 GHz (1.266e+00)
Port 1, mode 1: kₙ = 5.317e+03-2.445e-01i m⁻¹
Port 2, mode 1: kₙ = 5.317e+03-2.445e-01i m⁻¹
Sol. ||E|| = 1.431611e+01
Field energy E (4.294e-04 J) + H (5.420e-04 J) = 9.714e-04 J
S[1][1] = -5.684e-01+6.826e-02i, |S[1][1]| = -4.845e+00, arg(S[1][1]) = +1.732e+02
S[2][1] = -7.202e-02-1.479e-01i, |S[2][1]| = -1.567e+01, arg(S[2][1]) = -1.160e+02
It 227/300: ω/2π = 7.583e+01 GHz (total elapsed time = 2.23e+02 s)
Calculating boundary modes at wave ports for ω/2π = 7.583e+01 GHz (1.271e+00)
Port 1, mode 1: kₙ = 5.340e+03-2.456e-01i m⁻¹
Port 2, mode 1: kₙ = 5.340e+03-2.456e-01i m⁻¹
Sol. ||E|| = 1.431885e+01
Field energy E (4.296e-04 J) + H (5.418e-04 J) = 9.714e-04 J
S[1][1] = -5.678e-01+6.834e-02i, |S[1][1]| = -4.854e+00, arg(S[1][1]) = +1.731e+02
S[2][1] = -7.350e-02-1.468e-01i, |S[2][1]| = -1.569e+01, arg(S[2][1]) = -1.166e+02
It 228/300: ω/2π = 7.616e+01 GHz (total elapsed time = 2.24e+02 s)
Calculating boundary modes at wave ports for ω/2π = 7.616e+01 GHz (1.277e+00)
Port 1, mode 1: kₙ = 5.364e+03-2.467e-01i m⁻¹
Port 2, mode 1: kₙ = 5.364e+03-2.467e-01i m⁻¹
Sol. ||E|| = 1.432161e+01
Field energy E (4.298e-04 J) + H (5.417e-04 J) = 9.714e-04 J
S[1][1] = -5.671e-01+6.842e-02i, |S[1][1]| = -4.863e+00, arg(S[1][1]) = +1.731e+02
S[2][1] = -7.497e-02-1.457e-01i, |S[2][1]| = -1.571e+01, arg(S[2][1]) = -1.172e+02
It 229/300: ω/2π = 7.649e+01 GHz (total elapsed time = 2.24e+02 s)
Calculating boundary modes at wave ports for ω/2π = 7.649e+01 GHz (1.283e+00)
Port 1, mode 1: kₙ = 5.387e+03-2.478e-01i m⁻¹
Port 2, mode 1: kₙ = 5.387e+03-2.477e-01i m⁻¹
Sol. ||E|| = 1.432440e+01
Field energy E (4.299e-04 J) + H (5.415e-04 J) = 9.714e-04 J
S[1][1] = -5.665e-01+6.850e-02i, |S[1][1]| = -4.873e+00, arg(S[1][1]) = +1.731e+02
S[2][1] = -7.642e-02-1.446e-01i, |S[2][1]| = -1.573e+01, arg(S[2][1]) = -1.179e+02
It 230/300: ω/2π = 7.682e+01 GHz (total elapsed time = 2.24e+02 s)
Calculating boundary modes at wave ports for ω/2π = 7.682e+01 GHz (1.288e+00)
Port 1, mode 1: kₙ = 5.410e+03-2.488e-01i m⁻¹
Port 2, mode 1: kₙ = 5.410e+03-2.488e-01i m⁻¹
Sol. ||E|| = 1.432721e+01
Field energy E (4.301e-04 J) + H (5.414e-04 J) = 9.714e-04 J
S[1][1] = -5.659e-01+6.858e-02i, |S[1][1]| = -4.882e+00, arg(S[1][1]) = +1.731e+02
S[2][1] = -7.786e-02-1.434e-01i, |S[2][1]| = -1.574e+01, arg(S[2][1]) = -1.185e+02
It 231/300: ω/2π = 7.715e+01 GHz (total elapsed time = 2.25e+02 s)
Calculating boundary modes at wave ports for ω/2π = 7.715e+01 GHz (1.294e+00)
Port 1, mode 1: kₙ = 5.434e+03-2.499e-01i m⁻¹
Port 2, mode 1: kₙ = 5.434e+03-2.499e-01i m⁻¹
Sol. ||E|| = 1.433004e+01
Field energy E (4.302e-04 J) + H (5.412e-04 J) = 9.714e-04 J
S[1][1] = -5.653e-01+6.866e-02i, |S[1][1]| = -4.891e+00, arg(S[1][1]) = +1.731e+02
S[2][1] = -7.929e-02-1.423e-01i, |S[2][1]| = -1.576e+01, arg(S[2][1]) = -1.191e+02
It 232/300: ω/2π = 7.748e+01 GHz (total elapsed time = 2.25e+02 s)
Calculating boundary modes at wave ports for ω/2π = 7.748e+01 GHz (1.299e+00)
Port 1, mode 1: kₙ = 5.457e+03-2.510e-01i m⁻¹
Port 2, mode 1: kₙ = 5.457e+03-2.510e-01i m⁻¹
Sol. ||E|| = 1.433289e+01
Field energy E (4.304e-04 J) + H (5.411e-04 J) = 9.715e-04 J
S[1][1] = -5.647e-01+6.873e-02i, |S[1][1]| = -4.900e+00, arg(S[1][1]) = +1.731e+02
S[2][1] = -8.070e-02-1.411e-01i, |S[2][1]| = -1.578e+01, arg(S[2][1]) = -1.198e+02
It 233/300: ω/2π = 7.782e+01 GHz (total elapsed time = 2.25e+02 s)
Calculating boundary modes at wave ports for ω/2π = 7.782e+01 GHz (1.305e+00)
Port 1, mode 1: kₙ = 5.480e+03-2.520e-01i m⁻¹
Port 2, mode 1: kₙ = 5.480e+03-2.520e-01i m⁻¹
Sol. ||E|| = 1.433576e+01
Field energy E (4.306e-04 J) + H (5.409e-04 J) = 9.715e-04 J
S[1][1] = -5.641e-01+6.880e-02i, |S[1][1]| = -4.909e+00, arg(S[1][1]) = +1.730e+02
S[2][1] = -8.210e-02-1.399e-01i, |S[2][1]| = -1.580e+01, arg(S[2][1]) = -1.204e+02
It 234/300: ω/2π = 7.815e+01 GHz (total elapsed time = 2.26e+02 s)
Calculating boundary modes at wave ports for ω/2π = 7.815e+01 GHz (1.310e+00)
Port 1, mode 1: kₙ = 5.503e+03-2.531e-01i m⁻¹
Port 2, mode 1: kₙ = 5.503e+03-2.531e-01i m⁻¹
Sol. ||E|| = 1.433865e+01
Field energy E (4.307e-04 J) + H (5.408e-04 J) = 9.715e-04 J
S[1][1] = -5.635e-01+6.887e-02i, |S[1][1]| = -4.918e+00, arg(S[1][1]) = +1.730e+02
S[2][1] = -8.348e-02-1.388e-01i, |S[2][1]| = -1.581e+01, arg(S[2][1]) = -1.210e+02
It 235/300: ω/2π = 7.848e+01 GHz (total elapsed time = 2.26e+02 s)
Calculating boundary modes at wave ports for ω/2π = 7.848e+01 GHz (1.316e+00)
Port 1, mode 1: kₙ = 5.527e+03-2.542e-01i m⁻¹
Port 2, mode 1: kₙ = 5.527e+03-2.542e-01i m⁻¹
Sol. ||E|| = 1.434157e+01
Field energy E (4.309e-04 J) + H (5.406e-04 J) = 9.715e-04 J
S[1][1] = -5.629e-01+6.894e-02i, |S[1][1]| = -4.927e+00, arg(S[1][1]) = +1.730e+02
S[2][1] = -8.486e-02-1.375e-01i, |S[2][1]| = -1.583e+01, arg(S[2][1]) = -1.217e+02
It 236/300: ω/2π = 7.881e+01 GHz (total elapsed time = 2.26e+02 s)
Calculating boundary modes at wave ports for ω/2π = 7.881e+01 GHz (1.321e+00)
Port 1, mode 1: kₙ = 5.550e+03-2.553e-01i m⁻¹
Port 2, mode 1: kₙ = 5.550e+03-2.552e-01i m⁻¹
Sol. ||E|| = 1.434450e+01
Field energy E (4.311e-04 J) + H (5.405e-04 J) = 9.715e-04 J
S[1][1] = -5.623e-01+6.900e-02i, |S[1][1]| = -4.936e+00, arg(S[1][1]) = +1.730e+02
S[2][1] = -8.621e-02-1.363e-01i, |S[2][1]| = -1.585e+01, arg(S[2][1]) = -1.223e+02
It 237/300: ω/2π = 7.914e+01 GHz (total elapsed time = 2.27e+02 s)
Calculating boundary modes at wave ports for ω/2π = 7.914e+01 GHz (1.327e+00)
Port 1, mode 1: kₙ = 5.573e+03-2.563e-01i m⁻¹
Port 2, mode 1: kₙ = 5.573e+03-2.563e-01i m⁻¹
Sol. ||E|| = 1.434745e+01
Field energy E (4.313e-04 J) + H (5.403e-04 J) = 9.716e-04 J
S[1][1] = -5.617e-01+6.907e-02i, |S[1][1]| = -4.945e+00, arg(S[1][1]) = +1.730e+02
S[2][1] = -8.756e-02-1.351e-01i, |S[2][1]| = -1.586e+01, arg(S[2][1]) = -1.229e+02
It 238/300: ω/2π = 7.947e+01 GHz (total elapsed time = 2.27e+02 s)
Calculating boundary modes at wave ports for ω/2π = 7.947e+01 GHz (1.332e+00)
Port 1, mode 1: kₙ = 5.597e+03-2.574e-01i m⁻¹
Port 2, mode 1: kₙ = 5.597e+03-2.574e-01i m⁻¹
Sol. ||E|| = 1.435042e+01
Field energy E (4.314e-04 J) + H (5.402e-04 J) = 9.716e-04 J
S[1][1] = -5.611e-01+6.913e-02i, |S[1][1]| = -4.954e+00, arg(S[1][1]) = +1.730e+02
S[2][1] = -8.889e-02-1.339e-01i, |S[2][1]| = -1.588e+01, arg(S[2][1]) = -1.236e+02
It 239/300: ω/2π = 7.980e+01 GHz (total elapsed time = 2.28e+02 s)
Calculating boundary modes at wave ports for ω/2π = 7.980e+01 GHz (1.338e+00)
Port 1, mode 1: kₙ = 5.620e+03-2.585e-01i m⁻¹
Port 2, mode 1: kₙ = 5.620e+03-2.585e-01i m⁻¹
Sol. ||E|| = 1.435341e+01
Field energy E (4.316e-04 J) + H (5.400e-04 J) = 9.716e-04 J
S[1][1] = -5.605e-01+6.919e-02i, |S[1][1]| = -4.963e+00, arg(S[1][1]) = +1.730e+02
S[2][1] = -9.020e-02-1.326e-01i, |S[2][1]| = -1.590e+01, arg(S[2][1]) = -1.242e+02
It 240/300: ω/2π = 8.013e+01 GHz (total elapsed time = 2.28e+02 s)
Calculating boundary modes at wave ports for ω/2π = 8.013e+01 GHz (1.344e+00)
Port 1, mode 1: kₙ = 5.643e+03-2.595e-01i m⁻¹
Port 2, mode 1: kₙ = 5.643e+03-2.595e-01i m⁻¹
Sol. ||E|| = 1.435642e+01
Field energy E (4.318e-04 J) + H (5.399e-04 J) = 9.716e-04 J
S[1][1] = -5.599e-01+6.925e-02i, |S[1][1]| = -4.971e+00, arg(S[1][1]) = +1.729e+02
S[2][1] = -9.150e-02-1.314e-01i, |S[2][1]| = -1.591e+01, arg(S[2][1]) = -1.249e+02
It 241/300: ω/2π = 8.046e+01 GHz (total elapsed time = 2.28e+02 s)
Calculating boundary modes at wave ports for ω/2π = 8.046e+01 GHz (1.349e+00)
Port 1, mode 1: kₙ = 5.667e+03-2.606e-01i m⁻¹
Port 2, mode 1: kₙ = 5.667e+03-2.606e-01i m⁻¹
Sol. ||E|| = 1.435944e+01
Field energy E (4.320e-04 J) + H (5.397e-04 J) = 9.717e-04 J
S[1][1] = -5.594e-01+6.930e-02i, |S[1][1]| = -4.980e+00, arg(S[1][1]) = +1.729e+02
S[2][1] = -9.279e-02-1.301e-01i, |S[2][1]| = -1.593e+01, arg(S[2][1]) = -1.255e+02
It 242/300: ω/2π = 8.080e+01 GHz (total elapsed time = 2.29e+02 s)
Calculating boundary modes at wave ports for ω/2π = 8.080e+01 GHz (1.355e+00)
Port 1, mode 1: kₙ = 5.690e+03-2.617e-01i m⁻¹
Port 2, mode 1: kₙ = 5.690e+03-2.617e-01i m⁻¹
Sol. ||E|| = 1.436248e+01
Field energy E (4.321e-04 J) + H (5.396e-04 J) = 9.717e-04 J
S[1][1] = -5.588e-01+6.936e-02i, |S[1][1]| = -4.989e+00, arg(S[1][1]) = +1.729e+02
S[2][1] = -9.406e-02-1.288e-01i, |S[2][1]| = -1.595e+01, arg(S[2][1]) = -1.261e+02
It 243/300: ω/2π = 8.113e+01 GHz (total elapsed time = 2.29e+02 s)
Calculating boundary modes at wave ports for ω/2π = 8.113e+01 GHz (1.360e+00)
Port 1, mode 1: kₙ = 5.713e+03-2.628e-01i m⁻¹
Port 2, mode 1: kₙ = 5.713e+03-2.627e-01i m⁻¹
Sol. ||E|| = 1.436553e+01
Field energy E (4.323e-04 J) + H (5.394e-04 J) = 9.717e-04 J
S[1][1] = -5.582e-01+6.941e-02i, |S[1][1]| = -4.997e+00, arg(S[1][1]) = +1.729e+02
S[2][1] = -9.532e-02-1.275e-01i, |S[2][1]| = -1.596e+01, arg(S[2][1]) = -1.268e+02
It 244/300: ω/2π = 8.146e+01 GHz (total elapsed time = 2.30e+02 s)
Calculating boundary modes at wave ports for ω/2π = 8.146e+01 GHz (1.366e+00)
Port 1, mode 1: kₙ = 5.737e+03-2.638e-01i m⁻¹
Port 2, mode 1: kₙ = 5.737e+03-2.638e-01i m⁻¹
Sol. ||E|| = 1.436860e+01
Field energy E (4.325e-04 J) + H (5.393e-04 J) = 9.718e-04 J
S[1][1] = -5.576e-01+6.946e-02i, |S[1][1]| = -5.006e+00, arg(S[1][1]) = +1.729e+02
S[2][1] = -9.656e-02-1.262e-01i, |S[2][1]| = -1.598e+01, arg(S[2][1]) = -1.274e+02
It 245/300: ω/2π = 8.179e+01 GHz (total elapsed time = 2.30e+02 s)
Calculating boundary modes at wave ports for ω/2π = 8.179e+01 GHz (1.371e+00)
Port 1, mode 1: kₙ = 5.760e+03-2.649e-01i m⁻¹
Port 2, mode 1: kₙ = 5.760e+03-2.649e-01i m⁻¹
Sol. ||E|| = 1.437168e+01
Field energy E (4.327e-04 J) + H (5.391e-04 J) = 9.718e-04 J
S[1][1] = -5.571e-01+6.951e-02i, |S[1][1]| = -5.015e+00, arg(S[1][1]) = +1.729e+02
S[2][1] = -9.778e-02-1.249e-01i, |S[2][1]| = -1.599e+01, arg(S[2][1]) = -1.281e+02
It 246/300: ω/2π = 8.212e+01 GHz (total elapsed time = 2.31e+02 s)
Calculating boundary modes at wave ports for ω/2π = 8.212e+01 GHz (1.377e+00)
Port 1, mode 1: kₙ = 5.783e+03-2.660e-01i m⁻¹
Port 2, mode 1: kₙ = 5.783e+03-2.660e-01i m⁻¹
Sol. ||E|| = 1.437477e+01
Field energy E (4.328e-04 J) + H (5.390e-04 J) = 9.718e-04 J
S[1][1] = -5.565e-01+6.956e-02i, |S[1][1]| = -5.023e+00, arg(S[1][1]) = +1.729e+02
S[2][1] = -9.900e-02-1.236e-01i, |S[2][1]| = -1.601e+01, arg(S[2][1]) = -1.287e+02
It 247/300: ω/2π = 8.245e+01 GHz (total elapsed time = 2.31e+02 s)
Calculating boundary modes at wave ports for ω/2π = 8.245e+01 GHz (1.382e+00)
Port 1, mode 1: kₙ = 5.807e+03-2.671e-01i m⁻¹
Port 2, mode 1: kₙ = 5.807e+03-2.670e-01i m⁻¹
Sol. ||E|| = 1.437788e+01
Field energy E (4.330e-04 J) + H (5.388e-04 J) = 9.719e-04 J
S[1][1] = -5.560e-01+6.960e-02i, |S[1][1]| = -5.032e+00, arg(S[1][1]) = +1.729e+02
S[2][1] = -1.002e-01-1.222e-01i, |S[2][1]| = -1.602e+01, arg(S[2][1]) = -1.293e+02
It 248/300: ω/2π = 8.278e+01 GHz (total elapsed time = 2.31e+02 s)
Calculating boundary modes at wave ports for ω/2π = 8.278e+01 GHz (1.388e+00)
Port 1, mode 1: kₙ = 5.830e+03-2.681e-01i m⁻¹
Port 2, mode 1: kₙ = 5.830e+03-2.681e-01i m⁻¹
Sol. ||E|| = 1.438100e+01
Field energy E (4.332e-04 J) + H (5.387e-04 J) = 9.719e-04 J
S[1][1] = -5.554e-01+6.965e-02i, |S[1][1]| = -5.040e+00, arg(S[1][1]) = +1.729e+02
S[2][1] = -1.014e-01-1.209e-01i, |S[2][1]| = -1.604e+01, arg(S[2][1]) = -1.300e+02
It 249/300: ω/2π = 8.311e+01 GHz (total elapsed time = 2.32e+02 s)
Calculating boundary modes at wave ports for ω/2π = 8.311e+01 GHz (1.394e+00)
Port 1, mode 1: kₙ = 5.853e+03-2.692e-01i m⁻¹
Port 2, mode 1: kₙ = 5.853e+03-2.692e-01i m⁻¹
Sol. ||E|| = 1.438414e+01
Field energy E (4.334e-04 J) + H (5.386e-04 J) = 9.720e-04 J
S[1][1] = -5.549e-01+6.969e-02i, |S[1][1]| = -5.048e+00, arg(S[1][1]) = +1.728e+02
S[2][1] = -1.025e-01-1.195e-01i, |S[2][1]| = -1.606e+01, arg(S[2][1]) = -1.306e+02
It 250/300: ω/2π = 8.344e+01 GHz (total elapsed time = 2.32e+02 s)
Calculating boundary modes at wave ports for ω/2π = 8.344e+01 GHz (1.399e+00)
Port 1, mode 1: kₙ = 5.877e+03-2.703e-01i m⁻¹
Port 2, mode 1: kₙ = 5.877e+03-2.702e-01i m⁻¹
Sol. ||E|| = 1.438728e+01
Field energy E (4.336e-04 J) + H (5.384e-04 J) = 9.720e-04 J
S[1][1] = -5.543e-01+6.973e-02i, |S[1][1]| = -5.057e+00, arg(S[1][1]) = +1.728e+02
S[2][1] = -1.037e-01-1.181e-01i, |S[2][1]| = -1.607e+01, arg(S[2][1]) = -1.313e+02
It 251/300: ω/2π = 8.378e+01 GHz (total elapsed time = 2.32e+02 s)
Calculating boundary modes at wave ports for ω/2π = 8.378e+01 GHz (1.405e+00)
Port 1, mode 1: kₙ = 5.900e+03-2.713e-01i m⁻¹
Port 2, mode 1: kₙ = 5.900e+03-2.713e-01i m⁻¹
Sol. ||E|| = 1.439044e+01
Field energy E (4.338e-04 J) + H (5.383e-04 J) = 9.720e-04 J
S[1][1] = -5.538e-01+6.977e-02i, |S[1][1]| = -5.065e+00, arg(S[1][1]) = +1.728e+02
S[2][1] = -1.048e-01-1.168e-01i, |S[2][1]| = -1.609e+01, arg(S[2][1]) = -1.319e+02
It 252/300: ω/2π = 8.411e+01 GHz (total elapsed time = 2.33e+02 s)
Calculating boundary modes at wave ports for ω/2π = 8.411e+01 GHz (1.410e+00)
Port 1, mode 1: kₙ = 5.923e+03-2.724e-01i m⁻¹
Port 2, mode 1: kₙ = 5.923e+03-2.724e-01i m⁻¹
Sol. ||E|| = 1.439360e+01
Field energy E (4.340e-04 J) + H (5.381e-04 J) = 9.721e-04 J
S[1][1] = -5.532e-01+6.981e-02i, |S[1][1]| = -5.073e+00, arg(S[1][1]) = +1.728e+02
S[2][1] = -1.059e-01-1.154e-01i, |S[2][1]| = -1.610e+01, arg(S[2][1]) = -1.326e+02
It 253/300: ω/2π = 8.444e+01 GHz (total elapsed time = 2.33e+02 s)
Calculating boundary modes at wave ports for ω/2π = 8.444e+01 GHz (1.416e+00)
Port 1, mode 1: kₙ = 5.947e+03-2.735e-01i m⁻¹
Port 2, mode 1: kₙ = 5.947e+03-2.735e-01i m⁻¹
Sol. ||E|| = 1.439678e+01
Field energy E (4.341e-04 J) + H (5.380e-04 J) = 9.721e-04 J
S[1][1] = -5.527e-01+6.984e-02i, |S[1][1]| = -5.082e+00, arg(S[1][1]) = +1.728e+02
S[2][1] = -1.070e-01-1.140e-01i, |S[2][1]| = -1.612e+01, arg(S[2][1]) = -1.332e+02
It 254/300: ω/2π = 8.477e+01 GHz (total elapsed time = 2.33e+02 s)
Calculating boundary modes at wave ports for ω/2π = 8.477e+01 GHz (1.421e+00)
Port 1, mode 1: kₙ = 5.970e+03-2.746e-01i m⁻¹
Port 2, mode 1: kₙ = 5.970e+03-2.745e-01i m⁻¹
Sol. ||E|| = 1.439996e+01
Field energy E (4.343e-04 J) + H (5.378e-04 J) = 9.722e-04 J
S[1][1] = -5.522e-01+6.988e-02i, |S[1][1]| = -5.090e+00, arg(S[1][1]) = +1.728e+02
S[2][1] = -1.081e-01-1.126e-01i, |S[2][1]| = -1.613e+01, arg(S[2][1]) = -1.338e+02
It 255/300: ω/2π = 8.510e+01 GHz (total elapsed time = 2.34e+02 s)
Calculating boundary modes at wave ports for ω/2π = 8.510e+01 GHz (1.427e+00)
Port 1, mode 1: kₙ = 5.993e+03-2.756e-01i m⁻¹
Port 2, mode 1: kₙ = 5.993e+03-2.756e-01i m⁻¹
Sol. ||E|| = 1.440315e+01
Field energy E (4.345e-04 J) + H (5.377e-04 J) = 9.722e-04 J
S[1][1] = -5.516e-01+6.991e-02i, |S[1][1]| = -5.098e+00, arg(S[1][1]) = +1.728e+02
S[2][1] = -1.092e-01-1.112e-01i, |S[2][1]| = -1.615e+01, arg(S[2][1]) = -1.345e+02
It 256/300: ω/2π = 8.543e+01 GHz (total elapsed time = 2.34e+02 s)
Calculating boundary modes at wave ports for ω/2π = 8.543e+01 GHz (1.432e+00)
Port 1, mode 1: kₙ = 6.016e+03-2.767e-01i m⁻¹
Port 2, mode 1: kₙ = 6.016e+03-2.767e-01i m⁻¹
Sol. ||E|| = 1.440635e+01
Field energy E (4.347e-04 J) + H (5.376e-04 J) = 9.723e-04 J
S[1][1] = -5.511e-01+6.994e-02i, |S[1][1]| = -5.106e+00, arg(S[1][1]) = +1.728e+02
S[2][1] = -1.103e-01-1.097e-01i, |S[2][1]| = -1.616e+01, arg(S[2][1]) = -1.351e+02
It 257/300: ω/2π = 8.576e+01 GHz (total elapsed time = 2.34e+02 s)
Calculating boundary modes at wave ports for ω/2π = 8.576e+01 GHz (1.438e+00)
Port 1, mode 1: kₙ = 6.040e+03-2.778e-01i m⁻¹
Port 2, mode 1: kₙ = 6.040e+03-2.777e-01i m⁻¹
Sol. ||E|| = 1.440956e+01
Field energy E (4.349e-04 J) + H (5.374e-04 J) = 9.723e-04 J
S[1][1] = -5.506e-01+6.997e-02i, |S[1][1]| = -5.114e+00, arg(S[1][1]) = +1.728e+02
S[2][1] = -1.113e-01-1.083e-01i, |S[2][1]| = -1.618e+01, arg(S[2][1]) = -1.358e+02
It 258/300: ω/2π = 8.609e+01 GHz (total elapsed time = 2.35e+02 s)
Calculating boundary modes at wave ports for ω/2π = 8.609e+01 GHz (1.444e+00)
Port 1, mode 1: kₙ = 6.063e+03-2.788e-01i m⁻¹
Port 2, mode 1: kₙ = 6.063e+03-2.788e-01i m⁻¹
Sol. ||E|| = 1.441278e+01
Field energy E (4.351e-04 J) + H (5.373e-04 J) = 9.724e-04 J
S[1][1] = -5.501e-01+7.000e-02i, |S[1][1]| = -5.122e+00, arg(S[1][1]) = +1.727e+02
S[2][1] = -1.123e-01-1.069e-01i, |S[2][1]| = -1.619e+01, arg(S[2][1]) = -1.364e+02
It 259/300: ω/2π = 8.642e+01 GHz (total elapsed time = 2.35e+02 s)
Calculating boundary modes at wave ports for ω/2π = 8.642e+01 GHz (1.449e+00)
Port 1, mode 1: kₙ = 6.086e+03-2.799e-01i m⁻¹
Port 2, mode 1: kₙ = 6.086e+03-2.799e-01i m⁻¹
Sol. ||E|| = 1.441600e+01
Field energy E (4.353e-04 J) + H (5.371e-04 J) = 9.724e-04 J
S[1][1] = -5.496e-01+7.003e-02i, |S[1][1]| = -5.130e+00, arg(S[1][1]) = +1.727e+02
S[2][1] = -1.133e-01-1.054e-01i, |S[2][1]| = -1.621e+01, arg(S[2][1]) = -1.371e+02
It 260/300: ω/2π = 8.676e+01 GHz (total elapsed time = 2.35e+02 s)
Calculating boundary modes at wave ports for ω/2π = 8.676e+01 GHz (1.455e+00)
Port 1, mode 1: kₙ = 6.110e+03-2.810e-01i m⁻¹
Port 2, mode 1: kₙ = 6.110e+03-2.810e-01i m⁻¹
Sol. ||E|| = 1.441923e+01
Field energy E (4.355e-04 J) + H (5.370e-04 J) = 9.725e-04 J
S[1][1] = -5.490e-01+7.005e-02i, |S[1][1]| = -5.138e+00, arg(S[1][1]) = +1.727e+02
S[2][1] = -1.143e-01-1.040e-01i, |S[2][1]| = -1.622e+01, arg(S[2][1]) = -1.377e+02
It 261/300: ω/2π = 8.709e+01 GHz (total elapsed time = 2.36e+02 s)
Calculating boundary modes at wave ports for ω/2π = 8.709e+01 GHz (1.460e+00)
Port 1, mode 1: kₙ = 6.133e+03-2.821e-01i m⁻¹
Port 2, mode 1: kₙ = 6.133e+03-2.820e-01i m⁻¹
Sol. ||E|| = 1.442246e+01
Field energy E (4.357e-04 J) + H (5.369e-04 J) = 9.725e-04 J
S[1][1] = -5.485e-01+7.008e-02i, |S[1][1]| = -5.145e+00, arg(S[1][1]) = +1.727e+02
S[2][1] = -1.153e-01-1.025e-01i, |S[2][1]| = -1.623e+01, arg(S[2][1]) = -1.384e+02
It 262/300: ω/2π = 8.742e+01 GHz (total elapsed time = 2.36e+02 s)
Calculating boundary modes at wave ports for ω/2π = 8.742e+01 GHz (1.466e+00)
Port 1, mode 1: kₙ = 6.156e+03-2.831e-01i m⁻¹
Port 2, mode 1: kₙ = 6.156e+03-2.831e-01i m⁻¹
Sol. ||E|| = 1.442570e+01
Field energy E (4.359e-04 J) + H (5.367e-04 J) = 9.726e-04 J
S[1][1] = -5.480e-01+7.010e-02i, |S[1][1]| = -5.153e+00, arg(S[1][1]) = +1.727e+02
S[2][1] = -1.163e-01-1.010e-01i, |S[2][1]| = -1.625e+01, arg(S[2][1]) = -1.390e+02
It 263/300: ω/2π = 8.775e+01 GHz (total elapsed time = 2.37e+02 s)
Calculating boundary modes at wave ports for ω/2π = 8.775e+01 GHz (1.471e+00)
Port 1, mode 1: kₙ = 6.180e+03-2.842e-01i m⁻¹
Port 2, mode 1: kₙ = 6.180e+03-2.842e-01i m⁻¹
Sol. ||E|| = 1.442894e+01
Field energy E (4.360e-04 J) + H (5.366e-04 J) = 9.726e-04 J
S[1][1] = -5.475e-01+7.012e-02i, |S[1][1]| = -5.161e+00, arg(S[1][1]) = +1.727e+02
S[2][1] = -1.172e-01-9.954e-02i, |S[2][1]| = -1.626e+01, arg(S[2][1]) = -1.397e+02
It 264/300: ω/2π = 8.808e+01 GHz (total elapsed time = 2.37e+02 s)
Calculating boundary modes at wave ports for ω/2π = 8.808e+01 GHz (1.477e+00)
Port 1, mode 1: kₙ = 6.203e+03-2.853e-01i m⁻¹
Port 2, mode 1: kₙ = 6.203e+03-2.853e-01i m⁻¹
Sol. ||E|| = 1.443219e+01
Field energy E (4.362e-04 J) + H (5.364e-04 J) = 9.727e-04 J
S[1][1] = -5.470e-01+7.014e-02i, |S[1][1]| = -5.169e+00, arg(S[1][1]) = +1.727e+02
S[2][1] = -1.181e-01-9.805e-02i, |S[2][1]| = -1.628e+01, arg(S[2][1]) = -1.403e+02
It 265/300: ω/2π = 8.841e+01 GHz (total elapsed time = 2.37e+02 s)
Calculating boundary modes at wave ports for ω/2π = 8.841e+01 GHz (1.482e+00)
Port 1, mode 1: kₙ = 6.226e+03-2.863e-01i m⁻¹
Port 2, mode 1: kₙ = 6.226e+03-2.863e-01i m⁻¹
Sol. ||E|| = 1.443543e+01
Field energy E (4.364e-04 J) + H (5.363e-04 J) = 9.727e-04 J
S[1][1] = -5.466e-01+7.016e-02i, |S[1][1]| = -5.176e+00, arg(S[1][1]) = +1.727e+02
S[2][1] = -1.190e-01-9.655e-02i, |S[2][1]| = -1.629e+01, arg(S[2][1]) = -1.410e+02
It 266/300: ω/2π = 8.874e+01 GHz (total elapsed time = 2.38e+02 s)
Calculating boundary modes at wave ports for ω/2π = 8.874e+01 GHz (1.488e+00)
Port 1, mode 1: kₙ = 6.250e+03-2.874e-01i m⁻¹
Port 2, mode 1: kₙ = 6.250e+03-2.874e-01i m⁻¹
Sol. ||E|| = 1.443869e+01
Field energy E (4.366e-04 J) + H (5.362e-04 J) = 9.728e-04 J
S[1][1] = -5.461e-01+7.018e-02i, |S[1][1]| = -5.184e+00, arg(S[1][1]) = +1.727e+02
S[2][1] = -1.199e-01-9.504e-02i, |S[2][1]| = -1.630e+01, arg(S[2][1]) = -1.416e+02
It 267/300: ω/2π = 8.907e+01 GHz (total elapsed time = 2.38e+02 s)
Calculating boundary modes at wave ports for ω/2π = 8.907e+01 GHz (1.493e+00)
Port 1, mode 1: kₙ = 6.273e+03-2.885e-01i m⁻¹
Port 2, mode 1: kₙ = 6.273e+03-2.885e-01i m⁻¹
Sol. ||E|| = 1.444194e+01
Field energy E (4.368e-04 J) + H (5.360e-04 J) = 9.729e-04 J
S[1][1] = -5.456e-01+7.020e-02i, |S[1][1]| = -5.191e+00, arg(S[1][1]) = +1.727e+02
S[2][1] = -1.208e-01-9.353e-02i, |S[2][1]| = -1.632e+01, arg(S[2][1]) = -1.423e+02
It 268/300: ω/2π = 8.940e+01 GHz (total elapsed time = 2.38e+02 s)
Calculating boundary modes at wave ports for ω/2π = 8.940e+01 GHz (1.499e+00)
Port 1, mode 1: kₙ = 6.296e+03-2.896e-01i m⁻¹
Port 2, mode 1: kₙ = 6.296e+03-2.895e-01i m⁻¹
Sol. ||E|| = 1.444520e+01
Field energy E (4.370e-04 J) + H (5.359e-04 J) = 9.729e-04 J
S[1][1] = -5.451e-01+7.021e-02i, |S[1][1]| = -5.199e+00, arg(S[1][1]) = +1.727e+02
S[2][1] = -1.217e-01-9.201e-02i, |S[2][1]| = -1.633e+01, arg(S[2][1]) = -1.429e+02
It 269/300: ω/2π = 8.974e+01 GHz (total elapsed time = 2.39e+02 s)
Calculating boundary modes at wave ports for ω/2π = 8.974e+01 GHz (1.505e+00)
Port 1, mode 1: kₙ = 6.320e+03-2.906e-01i m⁻¹
Port 2, mode 1: kₙ = 6.320e+03-2.906e-01i m⁻¹
Sol. ||E|| = 1.444845e+01
Field energy E (4.372e-04 J) + H (5.358e-04 J) = 9.730e-04 J
S[1][1] = -5.446e-01+7.023e-02i, |S[1][1]| = -5.206e+00, arg(S[1][1]) = +1.727e+02
S[2][1] = -1.225e-01-9.049e-02i, |S[2][1]| = -1.635e+01, arg(S[2][1]) = -1.435e+02
It 270/300: ω/2π = 9.007e+01 GHz (total elapsed time = 2.39e+02 s)
Calculating boundary modes at wave ports for ω/2π = 9.007e+01 GHz (1.510e+00)
Port 1, mode 1: kₙ = 6.343e+03-2.917e-01i m⁻¹
Port 2, mode 1: kₙ = 6.343e+03-2.917e-01i m⁻¹
Sol. ||E|| = 1.445171e+01
Field energy E (4.374e-04 J) + H (5.356e-04 J) = 9.731e-04 J
S[1][1] = -5.442e-01+7.024e-02i, |S[1][1]| = -5.214e+00, arg(S[1][1]) = +1.726e+02
S[2][1] = -1.233e-01-8.895e-02i, |S[2][1]| = -1.636e+01, arg(S[2][1]) = -1.442e+02
It 271/300: ω/2π = 9.040e+01 GHz (total elapsed time = 2.39e+02 s)
Calculating boundary modes at wave ports for ω/2π = 9.040e+01 GHz (1.516e+00)
Port 1, mode 1: kₙ = 6.366e+03-2.928e-01i m⁻¹
Port 2, mode 1: kₙ = 6.366e+03-2.928e-01i m⁻¹
Sol. ||E|| = 1.445497e+01
Field energy E (4.376e-04 J) + H (5.355e-04 J) = 9.731e-04 J
S[1][1] = -5.437e-01+7.026e-02i, |S[1][1]| = -5.221e+00, arg(S[1][1]) = +1.726e+02
S[2][1] = -1.241e-01-8.741e-02i, |S[2][1]| = -1.637e+01, arg(S[2][1]) = -1.448e+02
It 272/300: ω/2π = 9.073e+01 GHz (total elapsed time = 2.40e+02 s)
Calculating boundary modes at wave ports for ω/2π = 9.073e+01 GHz (1.521e+00)
Port 1, mode 1: kₙ = 6.390e+03-2.938e-01i m⁻¹
Port 2, mode 1: kₙ = 6.390e+03-2.938e-01i m⁻¹
Sol. ||E|| = 1.445823e+01
Field energy E (4.378e-04 J) + H (5.354e-04 J) = 9.732e-04 J
S[1][1] = -5.432e-01+7.027e-02i, |S[1][1]| = -5.228e+00, arg(S[1][1]) = +1.726e+02
S[2][1] = -1.249e-01-8.587e-02i, |S[2][1]| = -1.639e+01, arg(S[2][1]) = -1.455e+02
It 273/300: ω/2π = 9.106e+01 GHz (total elapsed time = 2.40e+02 s)
Calculating boundary modes at wave ports for ω/2π = 9.106e+01 GHz (1.527e+00)
Port 1, mode 1: kₙ = 6.413e+03-2.949e-01i m⁻¹
Port 2, mode 1: kₙ = 6.413e+03-2.949e-01i m⁻¹
Sol. ||E|| = 1.446149e+01
Field energy E (4.380e-04 J) + H (5.353e-04 J) = 9.732e-04 J
S[1][1] = -5.428e-01+7.028e-02i, |S[1][1]| = -5.235e+00, arg(S[1][1]) = +1.726e+02
S[2][1] = -1.257e-01-8.432e-02i, |S[2][1]| = -1.640e+01, arg(S[2][1]) = -1.461e+02
It 274/300: ω/2π = 9.139e+01 GHz (total elapsed time = 2.41e+02 s)
Calculating boundary modes at wave ports for ω/2π = 9.139e+01 GHz (1.532e+00)
Port 1, mode 1: kₙ = 6.436e+03-2.960e-01i m⁻¹
Port 2, mode 1: kₙ = 6.436e+03-2.960e-01i m⁻¹
Sol. ||E|| = 1.446474e+01
Field energy E (4.382e-04 J) + H (5.351e-04 J) = 9.733e-04 J
S[1][1] = -5.423e-01+7.029e-02i, |S[1][1]| = -5.243e+00, arg(S[1][1]) = +1.726e+02
S[2][1] = -1.265e-01-8.276e-02i, |S[2][1]| = -1.641e+01, arg(S[2][1]) = -1.468e+02
It 275/300: ω/2π = 9.172e+01 GHz (total elapsed time = 2.41e+02 s)
Calculating boundary modes at wave ports for ω/2π = 9.172e+01 GHz (1.538e+00)
Port 1, mode 1: kₙ = 6.460e+03-2.971e-01i m⁻¹
Port 2, mode 1: kₙ = 6.460e+03-2.970e-01i m⁻¹
Sol. ||E|| = 1.446800e+01
Field energy E (4.384e-04 J) + H (5.350e-04 J) = 9.734e-04 J
S[1][1] = -5.419e-01+7.030e-02i, |S[1][1]| = -5.250e+00, arg(S[1][1]) = +1.726e+02
S[2][1] = -1.272e-01-8.120e-02i, |S[2][1]| = -1.643e+01, arg(S[2][1]) = -1.474e+02
It 276/300: ω/2π = 9.205e+01 GHz (total elapsed time = 2.41e+02 s)
Calculating boundary modes at wave ports for ω/2π = 9.205e+01 GHz (1.543e+00)
Port 1, mode 1: kₙ = 6.483e+03-2.981e-01i m⁻¹
Port 2, mode 1: kₙ = 6.483e+03-2.981e-01i m⁻¹
Sol. ||E|| = 1.447125e+01
Field energy E (4.386e-04 J) + H (5.349e-04 J) = 9.735e-04 J
S[1][1] = -5.414e-01+7.031e-02i, |S[1][1]| = -5.257e+00, arg(S[1][1]) = +1.726e+02
S[2][1] = -1.279e-01-7.963e-02i, |S[2][1]| = -1.644e+01, arg(S[2][1]) = -1.481e+02
It 277/300: ω/2π = 9.238e+01 GHz (total elapsed time = 2.42e+02 s)
Calculating boundary modes at wave ports for ω/2π = 9.238e+01 GHz (1.549e+00)
Port 1, mode 1: kₙ = 6.506e+03-2.992e-01i m⁻¹
Port 2, mode 1: kₙ = 6.506e+03-2.992e-01i m⁻¹
Sol. ||E|| = 1.447450e+01
Field energy E (4.388e-04 J) + H (5.348e-04 J) = 9.735e-04 J
S[1][1] = -5.410e-01+7.032e-02i, |S[1][1]| = -5.264e+00, arg(S[1][1]) = +1.726e+02
S[2][1] = -1.286e-01-7.805e-02i, |S[2][1]| = -1.645e+01, arg(S[2][1]) = -1.487e+02
It 278/300: ω/2π = 9.272e+01 GHz (total elapsed time = 2.42e+02 s)
Calculating boundary modes at wave ports for ω/2π = 9.272e+01 GHz (1.555e+00)
Port 1, mode 1: kₙ = 6.529e+03-3.003e-01i m⁻¹
Port 2, mode 1: kₙ = 6.529e+03-3.003e-01i m⁻¹
Sol. ||E|| = 1.447775e+01
Field energy E (4.390e-04 J) + H (5.346e-04 J) = 9.736e-04 J
S[1][1] = -5.405e-01+7.033e-02i, |S[1][1]| = -5.271e+00, arg(S[1][1]) = +1.726e+02
S[2][1] = -1.293e-01-7.647e-02i, |S[2][1]| = -1.646e+01, arg(S[2][1]) = -1.494e+02
It 279/300: ω/2π = 9.305e+01 GHz (total elapsed time = 2.42e+02 s)
Calculating boundary modes at wave ports for ω/2π = 9.305e+01 GHz (1.560e+00)
Port 1, mode 1: kₙ = 6.553e+03-3.014e-01i m⁻¹
Port 2, mode 1: kₙ = 6.553e+03-3.013e-01i m⁻¹
Sol. ||E|| = 1.448100e+01
Field energy E (4.392e-04 J) + H (5.345e-04 J) = 9.737e-04 J
S[1][1] = -5.401e-01+7.033e-02i, |S[1][1]| = -5.278e+00, arg(S[1][1]) = +1.726e+02
S[2][1] = -1.300e-01-7.489e-02i, |S[2][1]| = -1.648e+01, arg(S[2][1]) = -1.501e+02
It 280/300: ω/2π = 9.338e+01 GHz (total elapsed time = 2.43e+02 s)
Calculating boundary modes at wave ports for ω/2π = 9.338e+01 GHz (1.566e+00)
Port 1, mode 1: kₙ = 6.576e+03-3.024e-01i m⁻¹
Port 2, mode 1: kₙ = 6.576e+03-3.024e-01i m⁻¹
Sol. ||E|| = 1.448424e+01
Field energy E (4.394e-04 J) + H (5.344e-04 J) = 9.737e-04 J
S[1][1] = -5.397e-01+7.034e-02i, |S[1][1]| = -5.285e+00, arg(S[1][1]) = +1.726e+02
S[2][1] = -1.306e-01-7.330e-02i, |S[2][1]| = -1.649e+01, arg(S[2][1]) = -1.507e+02
It 281/300: ω/2π = 9.371e+01 GHz (total elapsed time = 2.43e+02 s)
Calculating boundary modes at wave ports for ω/2π = 9.371e+01 GHz (1.571e+00)
Port 1, mode 1: kₙ = 6.599e+03-3.035e-01i m⁻¹
Port 2, mode 1: kₙ = 6.599e+03-3.035e-01i m⁻¹
Sol. ||E|| = 1.448747e+01
Field energy E (4.396e-04 J) + H (5.343e-04 J) = 9.738e-04 J
S[1][1] = -5.392e-01+7.034e-02i, |S[1][1]| = -5.291e+00, arg(S[1][1]) = +1.726e+02
S[2][1] = -1.313e-01-7.170e-02i, |S[2][1]| = -1.650e+01, arg(S[2][1]) = -1.514e+02
It 282/300: ω/2π = 9.404e+01 GHz (total elapsed time = 2.43e+02 s)
Calculating boundary modes at wave ports for ω/2π = 9.404e+01 GHz (1.577e+00)
Port 1, mode 1: kₙ = 6.623e+03-3.046e-01i m⁻¹
Port 2, mode 1: kₙ = 6.623e+03-3.045e-01i m⁻¹
Sol. ||E|| = 1.449070e+01
Field energy E (4.397e-04 J) + H (5.341e-04 J) = 9.739e-04 J
S[1][1] = -5.388e-01+7.035e-02i, |S[1][1]| = -5.298e+00, arg(S[1][1]) = +1.726e+02
S[2][1] = -1.319e-01-7.010e-02i, |S[2][1]| = -1.652e+01, arg(S[2][1]) = -1.520e+02
It 283/300: ω/2π = 9.437e+01 GHz (total elapsed time = 2.44e+02 s)
Calculating boundary modes at wave ports for ω/2π = 9.437e+01 GHz (1.582e+00)
Port 1, mode 1: kₙ = 6.646e+03-3.056e-01i m⁻¹
Port 2, mode 1: kₙ = 6.646e+03-3.056e-01i m⁻¹
Sol. ||E|| = 1.449393e+01
Field energy E (4.399e-04 J) + H (5.340e-04 J) = 9.740e-04 J
S[1][1] = -5.384e-01+7.035e-02i, |S[1][1]| = -5.305e+00, arg(S[1][1]) = +1.726e+02
S[2][1] = -1.325e-01-6.850e-02i, |S[2][1]| = -1.653e+01, arg(S[2][1]) = -1.527e+02
It 284/300: ω/2π = 9.470e+01 GHz (total elapsed time = 2.44e+02 s)
Calculating boundary modes at wave ports for ω/2π = 9.470e+01 GHz (1.588e+00)
Port 1, mode 1: kₙ = 6.669e+03-3.067e-01i m⁻¹
Port 2, mode 1: kₙ = 6.669e+03-3.067e-01i m⁻¹
Sol. ||E|| = 1.449715e+01
Field energy E (4.401e-04 J) + H (5.339e-04 J) = 9.740e-04 J
S[1][1] = -5.380e-01+7.035e-02i, |S[1][1]| = -5.311e+00, arg(S[1][1]) = +1.725e+02
S[2][1] = -1.331e-01-6.689e-02i, |S[2][1]| = -1.654e+01, arg(S[2][1]) = -1.533e+02
It 285/300: ω/2π = 9.503e+01 GHz (total elapsed time = 2.45e+02 s)
Calculating boundary modes at wave ports for ω/2π = 9.503e+01 GHz (1.593e+00)
Port 1, mode 1: kₙ = 6.693e+03-3.078e-01i m⁻¹
Port 2, mode 1: kₙ = 6.693e+03-3.078e-01i m⁻¹
Sol. ||E|| = 1.450037e+01
Field energy E (4.403e-04 J) + H (5.338e-04 J) = 9.741e-04 J
S[1][1] = -5.375e-01+7.036e-02i, |S[1][1]| = -5.318e+00, arg(S[1][1]) = +1.725e+02
S[2][1] = -1.336e-01-6.528e-02i, |S[2][1]| = -1.655e+01, arg(S[2][1]) = -1.540e+02
It 286/300: ω/2π = 9.536e+01 GHz (total elapsed time = 2.45e+02 s)
Calculating boundary modes at wave ports for ω/2π = 9.536e+01 GHz (1.599e+00)
Port 1, mode 1: kₙ = 6.716e+03-3.089e-01i m⁻¹
Port 2, mode 1: kₙ = 6.716e+03-3.088e-01i m⁻¹
Sol. ||E|| = 1.450358e+01
Field energy E (4.405e-04 J) + H (5.337e-04 J) = 9.742e-04 J
S[1][1] = -5.371e-01+7.036e-02i, |S[1][1]| = -5.324e+00, arg(S[1][1]) = +1.725e+02
S[2][1] = -1.342e-01-6.366e-02i, |S[2][1]| = -1.656e+01, arg(S[2][1]) = -1.546e+02
It 287/300: ω/2π = 9.570e+01 GHz (total elapsed time = 2.46e+02 s)
Calculating boundary modes at wave ports for ω/2π = 9.570e+01 GHz (1.605e+00)
Port 1, mode 1: kₙ = 6.739e+03-3.099e-01i m⁻¹
Port 2, mode 1: kₙ = 6.739e+03-3.099e-01i m⁻¹
Sol. ||E|| = 1.450678e+01
Field energy E (4.407e-04 J) + H (5.336e-04 J) = 9.743e-04 J
S[1][1] = -5.367e-01+7.036e-02i, |S[1][1]| = -5.331e+00, arg(S[1][1]) = +1.725e+02
S[2][1] = -1.347e-01-6.204e-02i, |S[2][1]| = -1.658e+01, arg(S[2][1]) = -1.553e+02
It 288/300: ω/2π = 9.603e+01 GHz (total elapsed time = 2.46e+02 s)
Calculating boundary modes at wave ports for ω/2π = 9.603e+01 GHz (1.610e+00)
Port 1, mode 1: kₙ = 6.763e+03-3.110e-01i m⁻¹
Port 2, mode 1: kₙ = 6.763e+03-3.110e-01i m⁻¹
Sol. ||E|| = 1.450997e+01
Field energy E (4.409e-04 J) + H (5.334e-04 J) = 9.743e-04 J
S[1][1] = -5.363e-01+7.036e-02i, |S[1][1]| = -5.337e+00, arg(S[1][1]) = +1.725e+02
S[2][1] = -1.352e-01-6.042e-02i, |S[2][1]| = -1.659e+01, arg(S[2][1]) = -1.559e+02
It 289/300: ω/2π = 9.636e+01 GHz (total elapsed time = 2.46e+02 s)
Calculating boundary modes at wave ports for ω/2π = 9.636e+01 GHz (1.616e+00)
Port 1, mode 1: kₙ = 6.786e+03-3.121e-01i m⁻¹
Port 2, mode 1: kₙ = 6.786e+03-3.120e-01i m⁻¹
Sol. ||E|| = 1.451316e+01
Field energy E (4.411e-04 J) + H (5.333e-04 J) = 9.744e-04 J
S[1][1] = -5.359e-01+7.036e-02i, |S[1][1]| = -5.344e+00, arg(S[1][1]) = +1.725e+02
S[2][1] = -1.357e-01-5.879e-02i, |S[2][1]| = -1.660e+01, arg(S[2][1]) = -1.566e+02
It 290/300: ω/2π = 9.669e+01 GHz (total elapsed time = 2.47e+02 s)
Calculating boundary modes at wave ports for ω/2π = 9.669e+01 GHz (1.621e+00)
Port 1, mode 1: kₙ = 6.809e+03-3.131e-01i m⁻¹
Port 2, mode 1: kₙ = 6.809e+03-3.131e-01i m⁻¹
Sol. ||E|| = 1.451634e+01
Field energy E (4.413e-04 J) + H (5.332e-04 J) = 9.745e-04 J
S[1][1] = -5.355e-01+7.036e-02i, |S[1][1]| = -5.350e+00, arg(S[1][1]) = +1.725e+02
S[2][1] = -1.362e-01-5.716e-02i, |S[2][1]| = -1.661e+01, arg(S[2][1]) = -1.572e+02
It 291/300: ω/2π = 9.702e+01 GHz (total elapsed time = 2.47e+02 s)
Calculating boundary modes at wave ports for ω/2π = 9.702e+01 GHz (1.627e+00)
Port 1, mode 1: kₙ = 6.833e+03-3.142e-01i m⁻¹
Port 2, mode 1: kₙ = 6.833e+03-3.142e-01i m⁻¹
Sol. ||E|| = 1.451951e+01
Field energy E (4.415e-04 J) + H (5.331e-04 J) = 9.746e-04 J
S[1][1] = -5.351e-01+7.037e-02i, |S[1][1]| = -5.356e+00, arg(S[1][1]) = +1.725e+02
S[2][1] = -1.366e-01-5.553e-02i, |S[2][1]| = -1.662e+01, arg(S[2][1]) = -1.579e+02
It 292/300: ω/2π = 9.735e+01 GHz (total elapsed time = 2.48e+02 s)
Calculating boundary modes at wave ports for ω/2π = 9.735e+01 GHz (1.632e+00)
Port 1, mode 1: kₙ = 6.856e+03-3.153e-01i m⁻¹
Port 2, mode 1: kₙ = 6.856e+03-3.153e-01i m⁻¹
Sol. ||E|| = 1.452267e+01
Field energy E (4.417e-04 J) + H (5.330e-04 J) = 9.747e-04 J
S[1][1] = -5.347e-01+7.037e-02i, |S[1][1]| = -5.363e+00, arg(S[1][1]) = +1.725e+02
S[2][1] = -1.371e-01-5.389e-02i, |S[2][1]| = -1.664e+01, arg(S[2][1]) = -1.585e+02
It 293/300: ω/2π = 9.768e+01 GHz (total elapsed time = 2.48e+02 s)
Calculating boundary modes at wave ports for ω/2π = 9.768e+01 GHz (1.638e+00)
Port 1, mode 1: kₙ = 6.879e+03-3.164e-01i m⁻¹
Port 2, mode 1: kₙ = 6.879e+03-3.163e-01i m⁻¹
Sol. ||E|| = 1.452583e+01
Field energy E (4.419e-04 J) + H (5.329e-04 J) = 9.748e-04 J
S[1][1] = -5.344e-01+7.037e-02i, |S[1][1]| = -5.369e+00, arg(S[1][1]) = +1.725e+02
S[2][1] = -1.375e-01-5.225e-02i, |S[2][1]| = -1.665e+01, arg(S[2][1]) = -1.592e+02
It 294/300: ω/2π = 9.801e+01 GHz (total elapsed time = 2.48e+02 s)
Calculating boundary modes at wave ports for ω/2π = 9.801e+01 GHz (1.643e+00)
Port 1, mode 1: kₙ = 6.903e+03-3.174e-01i m⁻¹
Port 2, mode 1: kₙ = 6.903e+03-3.174e-01i m⁻¹
Sol. ||E|| = 1.452897e+01
Field energy E (4.421e-04 J) + H (5.328e-04 J) = 9.748e-04 J
S[1][1] = -5.340e-01+7.037e-02i, |S[1][1]| = -5.375e+00, arg(S[1][1]) = +1.725e+02
S[2][1] = -1.379e-01-5.061e-02i, |S[2][1]| = -1.666e+01, arg(S[2][1]) = -1.598e+02
It 295/300: ω/2π = 9.834e+01 GHz (total elapsed time = 2.49e+02 s)
Calculating boundary modes at wave ports for ω/2π = 9.834e+01 GHz (1.649e+00)
Port 1, mode 1: kₙ = 6.926e+03-3.185e-01i m⁻¹
Port 2, mode 1: kₙ = 6.926e+03-3.185e-01i m⁻¹
Sol. ||E|| = 1.453210e+01
Field energy E (4.422e-04 J) + H (5.327e-04 J) = 9.749e-04 J
S[1][1] = -5.336e-01+7.036e-02i, |S[1][1]| = -5.381e+00, arg(S[1][1]) = +1.725e+02
S[2][1] = -1.383e-01-4.897e-02i, |S[2][1]| = -1.667e+01, arg(S[2][1]) = -1.605e+02
It 296/300: ω/2π = 9.868e+01 GHz (total elapsed time = 2.49e+02 s)
Calculating boundary modes at wave ports for ω/2π = 9.868e+01 GHz (1.654e+00)
Port 1, mode 1: kₙ = 6.949e+03-3.196e-01i m⁻¹
Port 2, mode 1: kₙ = 6.949e+03-3.195e-01i m⁻¹
Sol. ||E|| = 1.453523e+01
Field energy E (4.424e-04 J) + H (5.326e-04 J) = 9.750e-04 J
S[1][1] = -5.332e-01+7.036e-02i, |S[1][1]| = -5.387e+00, arg(S[1][1]) = +1.725e+02
S[2][1] = -1.387e-01-4.732e-02i, |S[2][1]| = -1.668e+01, arg(S[2][1]) = -1.612e+02
It 297/300: ω/2π = 9.901e+01 GHz (total elapsed time = 2.49e+02 s)
Calculating boundary modes at wave ports for ω/2π = 9.901e+01 GHz (1.660e+00)
Port 1, mode 1: kₙ = 6.973e+03-3.206e-01i m⁻¹
Port 2, mode 1: kₙ = 6.973e+03-3.206e-01i m⁻¹
Sol. ||E|| = 1.453834e+01
Field energy E (4.426e-04 J) + H (5.325e-04 J) = 9.751e-04 J
S[1][1] = -5.329e-01+7.036e-02i, |S[1][1]| = -5.393e+00, arg(S[1][1]) = +1.725e+02
S[2][1] = -1.390e-01-4.567e-02i, |S[2][1]| = -1.669e+01, arg(S[2][1]) = -1.618e+02
It 298/300: ω/2π = 9.934e+01 GHz (total elapsed time = 2.50e+02 s)
Calculating boundary modes at wave ports for ω/2π = 9.934e+01 GHz (1.666e+00)
Port 1, mode 1: kₙ = 6.996e+03-3.217e-01i m⁻¹
Port 2, mode 1: kₙ = 6.996e+03-3.217e-01i m⁻¹
Sol. ||E|| = 1.454144e+01
Field energy E (4.428e-04 J) + H (5.324e-04 J) = 9.752e-04 J
S[1][1] = -5.325e-01+7.036e-02i, |S[1][1]| = -5.399e+00, arg(S[1][1]) = +1.725e+02
S[2][1] = -1.393e-01-4.402e-02i, |S[2][1]| = -1.671e+01, arg(S[2][1]) = -1.625e+02
It 299/300: ω/2π = 9.967e+01 GHz (total elapsed time = 2.50e+02 s)
Calculating boundary modes at wave ports for ω/2π = 9.967e+01 GHz (1.671e+00)
Port 1, mode 1: kₙ = 7.019e+03-3.228e-01i m⁻¹
Port 2, mode 1: kₙ = 7.019e+03-3.228e-01i m⁻¹
Sol. ||E|| = 1.454454e+01
Field energy E (4.430e-04 J) + H (5.323e-04 J) = 9.753e-04 J
S[1][1] = -5.321e-01+7.036e-02i, |S[1][1]| = -5.404e+00, arg(S[1][1]) = +1.725e+02
S[2][1] = -1.397e-01-4.237e-02i, |S[2][1]| = -1.672e+01, arg(S[2][1]) = -1.631e+02
It 300/300: ω/2π = 1.000e+02 GHz (total elapsed time = 2.51e+02 s)
Calculating boundary modes at wave ports for ω/2π = 1.000e+02 GHz (1.677e+00)
Port 1, mode 1: kₙ = 7.042e+03-3.239e-01i m⁻¹
Port 2, mode 1: kₙ = 7.042e+03-3.238e-01i m⁻¹
Sol. ||E|| = 1.454762e+01
Field energy E (4.432e-04 J) + H (5.322e-04 J) = 9.754e-04 J
S[1][1] = -5.318e-01+7.036e-02i, |S[1][1]| = -5.410e+00, arg(S[1][1]) = +1.725e+02
S[2][1] = -1.400e-01-4.072e-02i, |S[2][1]| = -1.673e+01, arg(S[2][1]) = -1.638e+02
Completed 0 iterations of adaptive mesh refinement (AMR):
Indicator norm = 1.193e-01, global unknowns = 1171104
Max. iterations = 0, tol. = 1.000e-02
Elapsed Time Report (s) Min. Max. Avg.
==============================================================
Initialization 0.089 0.099 0.092
Mesh Preprocessing 1.390 1.393 1.392
Operator Construction 46.244 46.333 46.294
Wave Ports 35.135 35.866 35.817
Linear Solve 5.811 6.480 5.983
Setup 63.075 63.090 63.088
Preconditioner 45.110 46.104 45.782
Coarse Solve 10.135 10.788 10.390
PROM Construction 0.481 0.502 0.487
PROM Solve 0.974 1.046 1.006
Estimation 0.210 0.249 0.224
Construction 2.872 2.878 2.875
Solve 23.514 23.552 23.539
Postprocessing 19.146 19.909 19.208
Disk IO 0.625 0.628 0.627
--------------------------------------------------------------
Total 257.070 257.073 257.070
Simulation completed successfully
Results saved to palace-sim-cpw-waveport/output/palace
Plot S-parameters¶
Port mapping: Port 1: p1, Port 2: p2
Port mapping: Port 1: p1, Port 2: p2