Coupling Between Sources and Destinations
Some boundary conditions, like the Port and Scattering Boundary Condition, provide options for well-defined input fields. If such an input condition is used, it defines the input power variable, ewfd.Pin, where ewfd is the tag of the physics interface.
The input power variable is only defined for driven study steps, like the Frequency Domain and Wavelength Domain study steps, but not for Eigenfrequency, Mode Analysis, and Boundary Mode Analysis study steps.
At boundaries, where the waves leave the simulation domain, such as at the boundaries toward Perfectly Matched Layer domains, or at Port and Scattering Boundary Condition boundaries, the power of the outgoing waves is computed and stored in variables named like ewfd.sctr1.Pout, where sctr1 is the tag of the particular physics feature defined on the boundary. The different output power contributions are then summed up hierarchically with ewfd.Pout representing the total power of all outgoing waves from the physics interface. All output power variables are summarized in Table 2-11.
ewfd.wee1.pml1.Pout
Power of outgoing wave flowing from the Wave Equation, Electric node wee1 into the Perfectly Matched layer node pml1.
ewfd.wee1.Pout
ewfd.sctr1.Pout
ewfd.port1.Pout
ewfd.PoutMPort_N
Sum of all power of outgoing waves matching any the Port nodes on the boundary of the Port node named N.
ewfd.PoutNMPort_N
Power of outgoing waves not matching any of the Port nodes on the boundary of the node named N.
ewfd.PoutPort_N
Sum of ewfd.PoutMPort_N and ewfd.PoutNMPort_N.
ewfd.Pout
For the variables ewfd.PoutMPort_N, ewfd.PoutNMPort_N, and ewfd.PoutPort_N, the suffix N represents the value of the Port name parameter for the first Port node listed by the physics on the particular boundary.
The variable ewfd.PoutNMPort_N is always equal to zero, unless the Activate slit condition on interior port checkbox is enabled and Slit type is set to Domain-backed in the Port Settings.
When The Electromagnetic Waves, Beam Envelopes Interface is used, the power variables related to the Wave Equation, Beam Envelopes node are called ewbe.webe1.pml1.Pout and ewbe.webe1.Pout, representing the power flowing from the Wave Equation, Beam Envelopes node webe1 into the Perfectly Matched Layer node pml1 or into all Perfectly Matched Layer nodes overlapping with the Wave Equation, Beam Envelopes node, respectively.
Currently, the output power variables are only defined by Port and Scattering Boundary Condition features. In addition, it is also defined on interior boundaries adjacent to Perfectly Matched Layer domains.
When there is a single feature that provides the input power, it is possible to calculate the coupling of power from that input feature to the different output boundaries. These outcoupling variables form a similar hierarchy as the variables for the power of the outgoing waves. All outcoupling variables are summarized in Table 2-12.
ewfd.wee1.pml1.etaOut
ewfd.wee1.pml1.Pout/ewfd.Pin
ewfd.wee1.etaOut
ewfd.wee1.Pout/ewfd.Pin
ewfd.sctr1.etaOut
ewfd.sctr1.Pout/ewfd.Pin
ewfd.port1.etaOut
ewfd.port1.Pout/ewfd.Pin
ewfd.etaOutMPort_N
ewfd.PoutMPort_N/ewfd.Pin
ewfd.etaOutNMPort_N
ewfd.PoutNMPort_N/ewfd.Pin
ewfd.etaOutPort_N
ewfd.PoutPort_N/ewfd.Pin
ewfd.etaOut
ewfd.Pout/ewfd.Pin
See Table 2-11 for the definition of the variables for the power of the outgoing waves. The suffix N for the Port-related variables, represents the value of the Port name parameter.
For convenience, there are also variables representing scattering loss. With scattering loss means outcoupling through boundaries that almost always represents some sort of unwanted leakage of radiation. The scattering loss variables are summarized in Table 2-13.
ewfd.wee1.pml1.Lsca
ewfd.wee1.pml1.etaOut
ewfd.wee1.Lsca
ewfd.wee1.etaOut
ewfd.LscaPort_N
ewfd.etaOutNMPort_N
ewfd.Lsca
There is no scattering loss variable defined for the Scattering Boundary Condition, as the outgoing waves through Scattering Boundary Condition boundaries often represent “useful” radiation. As a consequence, the outcoupling from Scattering Boundary Condition nodes is not included in the summation variable ewfd.Lsca.
Similarly, for Port nodes, only the part of the outgoing waves that does not match any of the port modes on the boundary is considered as scattering loss.
To account for absorption in domains and at boundaries, loss variables are defined as listed in Table 2-14.
Table 2-14: Loss Variables.
ewfd.wee1.Ploss
ewfd.imp1.Ploss
ewfd.libc1.Ploss
ewfd.ltbc1.Ploss
ewfd.trans1.Ploss
ewfd.Ploss
When the input power variable is defined, it is possible to define the absorptance for each lossy feature and for the total absorptance. The different absorptance variables are summarized in Table 2-15.
ewfd.wee1.A
ewfd.wee1.Ploss/ewfd.Pin
ewfd.imp1.A
ewfd.imp1.Ploss/ewfd.Pin
ewfd.libc1.A
ewfd.libc1.Ploss/ewfd.Pin
ewfd.ltbc1.A
ewfd.ltbc1.Ploss/ewfd.Pin
ewfd.trans1.A
ewfd.trans1.Ploss/ewfd.Pin
ewfd.Atotal
ewfd.Ploss/ewfd.Pin
For an example model demonstrating the use of the outcoupling and absorptance variables discussed above, see Modeling a Scatterer Near an Optical Waveguide: Application Library path Wave_Optics_Module/Waveguides/waveguide_with_scatterer.