physics-interfacePreview
Wave Optics
Fixed-frequency scalar-polarization Helmholtz wave optics for isotropic, lossless, nonmagnetic dielectric media.
Reference contract
| Field | Value | Description |
|---|---|---|
| constraints | [] | — |
| coupled_runtime | null | — |
| differentiable_runtime | {"certification":"WaveOpticsComplexHelmholtzRuntime","coordinate_expression_gradient":true,"coordinate_gradient":true,"design_properties":["permittivity"],"execution_backend":"telion-v2-shared-execution","expression_objectives":true,"material_expression_gradient":true,"material_gradient":true,"objective_rules":[{"entity_dimensions":["global","domain","boundary","point"],"modes":["stationary"],"operators":["integral","average","minimum","maximum","rms","norm","smooth-maximum","smooth-minimum"],"supports_selection":true,"symbols":["ewfd.E"],"value_kind":"field"},{"entity_dimensions":["global"],"modes":["stationary"],"operators":["value"],"supports_selection":false,"symbols":["ewfd.energy"],"value_kind":"scalar-global"},{"entity_dimensions":["global"],"modes":["stationary"],"operators":["value"],"supports_selection":false,"symbols":["ewfd.compliance"],"value_kind":"scalar-global"}],"residual_owner":"WaveOptics.element_residual","state_fields":["E"],"supported_objective_symbols":{"coordinate":["ewfd.E","ewfd.energy","ewfd.compliance"],"material":["ewfd.E","ewfd.energy","ewfd.compliance"],"topology":["ewfd.E","ewfd.energy","ewfd.compliance"]},"topology_expression_gradient":true} | — |
| dynamic_outputs | [] | — |
| equation_summary | -div(grad(E)) - omega^2*mu0*epsilon*E = i*omega*mu0*J | — |
| frequency_domain_runtime | {"certification":"WaveOpticsComplexHelmholtzRuntime","operator_terms":[{"angular_frequency_power":2,"coefficient":"permittivity","phase":"real"}],"runtime":"scalar-complex-helmholtz","state_fields":["E"],"supports_sweep":false} | — |
| metadata | {"releaseSupport":{"certifiedStudies":[],"manifest":"docs/september-2026-classroom-physics-matrix.json","manifestSha256":"8f1273eda113099a6658438b1513d127c2c4c99c511c5a6fc5b82637cf6bc949","profile":"september-2026-classroom","reason":"Wave Optics has no certified study in the September 2026 classroom support matrix.","selectable":false}} | — |
| preferred_material | null | — |
| schema_version | 2.0.0 | — |
| studies | [{"certified":false,"differentiability":"exact-ad","kind":"frequency-domain","reason":"Wave Optics frequency domain is outside the September 2026 classroom support matrix."},{"certified":false,"differentiability":"exact-ad","kind":"sensitivity","reason":"Wave Optics sensitivity is outside the September 2026 classroom support matrix."},{"certified":false,"differentiability":"exact-ad","kind":"optimization","reason":"Wave Optics optimization is outside the September 2026 classroom support matrix."}] | — |
| transient_runtime | null | — |
| weak_contributions | [{"differentiability":"exact-ad","entity_dimension":"domain","expression":"dot(grad(test(ewfd.E)),grad(ewfd.E)) - angularFrequency^2*mu0*permittivity*test(ewfd.E)*ewfd.E - i*angularFrequency*mu0*test(ewfd.E)*electricCurrentSource","name":"ewfd.wave","test_field":"ewfd.E"}] | — |
| category | Wave Optics | — |
| description | Fixed-frequency scalar-polarization Helmholtz wave optics for isotropic, lossless, nonmagnetic dielectric media. | — |
| dimensions | [3] | — |
| display_name | Wave Optics | — |
| kind | Wave Optics | — |
| namespace | ewfd | — |
| status | development | — |
| visible | false | — |
Fixed-frequency scalar-polarization Helmholtz wave optics for isotropic, lossless, nonmagnetic dielectric media.
Contract
| Property | Value |
|---|---|
| constraints | [] |
| coupled_runtime | null |
| differentiable_runtime | {"certification":"WaveOpticsComplexHelmholtzRuntime","coordinate_expression_gradient":true,"coordinate_gradient":true,"design_properties":["permittivity"],"execution_backend":"telion-v2-shared-execution","expression_objectives":true,"material_expression_gradient":true,"material_gradient":true,"objective_rules":[{"entity_dimensions":["global","domain","boundary","point"],"modes":["stationary"],"operators":["integral","average","minimum","maximum","rms","norm","smooth-maximum","smooth-minimum"]... |
| dynamic_outputs | [] |
| equation_summary | -div(grad(E)) - omega^2*mu0*epsilon*E = i*omega*mu0*J |
| frequency_domain_runtime | {"certification":"WaveOpticsComplexHelmholtzRuntime","operator_terms":[{"angular_frequency_power":2,"coefficient":"permittivity","phase":"real"}],"runtime":"scalar-complex-helmholtz","state_fields":["E"],"supports_sweep":false} |
| metadata | {"releaseSupport":{"certifiedStudies":[],"manifest":"docs/september-2026-classroom-physics-matrix.json","manifestSha256":"8f1273eda113099a6658438b1513d127c2c4c99c511c5a6fc5b82637cf6bc949","profile":"september-2026-classroom","reason":"Wave Optics has no certified study in the September 2026 classroom support matrix.","selectable":false}} |
| preferred_material | null |
| schema_version | 2.0.0 |
| studies | [{"certified":false,"differentiability":"exact-ad","kind":"frequency-domain","reason":"Wave Optics frequency domain is outside the September 2026 classroom support matrix."},{"certified":false,"differentiability":"exact-ad","kind":"sensitivity","reason":"Wave Optics sensitivity is outside the September 2026 classroom support matrix."},{"certified":false,"differentiability":"exact-ad","kind":"optimization","reason":"Wave Optics optimization is outside the September 2026 classroom support matri... |
| transient_runtime | null |
| weak_contributions | [{"differentiability":"exact-ad","entity_dimension":"domain","expression":"dot(grad(test(ewfd.E)),grad(ewfd.E)) - angularFrequency^2*mu0*permittivity*test(ewfd.E)*ewfd.E - i*angularFrequency*mu0*test(ewfd.E)*electricCurrentSource","name":"ewfd.wave","test_field":"ewfd.E"}] |
| category | Wave Optics |
| description | Fixed-frequency scalar-polarization Helmholtz wave optics for isotropic, lossless, nonmagnetic dielectric media. |
| dimensions | [3] |
| display_name | Wave Optics |
| kind | Wave Optics |
| namespace | ewfd |
| status | development |
| visible | false |