tidy3d.components.data.monitor_data.ElectromagneticFieldData#
- class ElectromagneticFieldData[source]#
Bases:
AbstractFieldData
,ElectromagneticFieldDataset
,ABC
Collection of electromagnetic fields.
- Parameters:
Ex (Attribute:
Ex
) –Type
Union[ScalarFieldDataArray, ScalarFieldTimeDataArray, ScalarModeFieldDataArray]
Default
= None
Description
Spatial distribution of the x-component of the electric field.
Ey (Attribute:
Ey
) –Type
Union[ScalarFieldDataArray, ScalarFieldTimeDataArray, ScalarModeFieldDataArray]
Default
= None
Description
Spatial distribution of the y-component of the electric field.
Ez (Attribute:
Ez
) –Type
Union[ScalarFieldDataArray, ScalarFieldTimeDataArray, ScalarModeFieldDataArray]
Default
= None
Description
Spatial distribution of the z-component of the electric field.
Hx (Attribute:
Hx
) –Type
Union[ScalarFieldDataArray, ScalarFieldTimeDataArray, ScalarModeFieldDataArray]
Default
= None
Description
Spatial distribution of the x-component of the magnetic field.
Hy (Attribute:
Hy
) –Type
Union[ScalarFieldDataArray, ScalarFieldTimeDataArray, ScalarModeFieldDataArray]
Default
= None
Description
Spatial distribution of the y-component of the magnetic field.
Hz (Attribute:
Hz
) –Type
Union[ScalarFieldDataArray, ScalarFieldTimeDataArray, ScalarModeFieldDataArray]
Default
= None
Description
Spatial distribution of the z-component of the magnetic field.
monitor (Attribute:
monitor
) –Type
Union[FieldMonitor, FieldTimeMonitor, PermittivityMonitor, ModeSolverMonitor]
Default
symmetry (Attribute:
symmetry
) –Type
Tuple[Literal[0, -1, 1], Literal[0, -1, 1], Literal[0, -1, 1]]
Default
= (0, 0, 0)
Description
Symmetry eigenvalues of the original simulation in x, y, and z.
symmetry_center (Attribute:
symmetry_center
) –Type
Optional[Tuple[float, float, float]]
Default
= None
Description
Center of the symmetry planes of the original simulation in x, y, and z. Required only if any of the
symmetry
field are non-zero.grid_expanded (Attribute:
grid_expanded
) –Type
Optional[Grid]
Default
= None
Description
Grid
discretization of the associated monitor in the simulation which created the data. Required if symmetries are present, as well as in order to use some functionalities like getting poynting and flux.grid_primal_correction (Attribute:
grid_primal_correction
) –Type
Union[float, FreqDataArray, TimeDataArray, FreqModeDataArray]
Default
= 1.0
Description
Correction factor that needs to be applied for data corresponding to a 2D monitor to take into account the finite grid in the normal direction in the simulation in which the data was computed. The factor is applied to fields defined on the primal grid locations along the normal direction.
grid_dual_correction (Attribute:
grid_dual_correction
) –Type
Union[float, FreqDataArray, TimeDataArray, FreqModeDataArray]
Default
= 1.0
Description
Correction factor that needs to be applied for data corresponding to a 2D monitor to take into account the finite grid in the normal direction in the simulation in which the data was computed. The factor is applied to fields defined on the dual grid locations along the normal direction.
Attributes
Coordinates to be used for colocation of the data to grid boundaries.
Coordinates to be used for colocation of the data to grid centers.
Flux for data corresponding to a 2D monitor.
Return a copy of self with grid correction factors applied (if necessary) and symmetry expanded.
Return the sum of the squared absolute electric field components.
Effective mode area corresponding to a 2D monitor.
Time-averaged Poynting vector for frequency-domain data associated to a 2D monitor, projected to the direction normal to the monitor plane.
Make a copy of the data with time-reversed fields.
Methods
dot
(field_data[, conjugate])Dot product (modal overlap) with another
FieldData
object.outer_dot
(field_data[, conjugate])Dot product (modal overlap) with another
FieldData
object.package_flux_results
(flux_values)How to package flux
- grid_primal_correction#
- grid_dual_correction#
- property colocation_boundaries#
Coordinates to be used for colocation of the data to grid boundaries.
- property colocation_centers#
Coordinates to be used for colocation of the data to grid centers.
- property grid_corrected_copy#
Return a copy of self with grid correction factors applied (if necessary) and symmetry expanded.
- property intensity#
Return the sum of the squared absolute electric field components.
- property poynting#
Time-averaged Poynting vector for frequency-domain data associated to a 2D monitor, projected to the direction normal to the monitor plane.
- property flux#
Flux for data corresponding to a 2D monitor.
- property mode_area#
Effective mode area corresponding to a 2D monitor.
Effective mode area is calculated as: (∫|E|²dA)² / (∫|E|⁴dA)
- dot(field_data, conjugate=True)[source]#
Dot product (modal overlap) with another
FieldData
object. Both datasets have to be frequency-domain data associated with a 2D monitor. Along the tangential directions, the datasets have to have the same discretization. Along the normal direction, the monitor position may differ and is ignored. Other coordinates (frequency
,mode_index
) have to be either identical or broadcastable. Broadcasting is also supported in the case in which the otherfield_data
has a dimension of size1
whose coordinate is not in the list of coordinates in theself
dataset along the corresponding dimension. In that case, the coordinates of theself
dataset are used in the output.- Parameters:
field_data (
ElectromagneticFieldData
) – A data instance to compute the dot product with.conjugate (bool, optional) – If
True
(default), the dot product is defined as1 / 4
times the integral ofE_self* x H_other - H_self* x E_other
, wherex
is the cross product and*
is complex conjugation. IfFalse
, the complex conjugation is skipped.
Note
The dot product with and without conjugation is equivalent (up to a phase) for modes in lossless waveguides but differs for modes in lossy materials. In that case, the conjugated dot product can be interpreted as the fraction of the power of the first mode carried by the second, but modes are not orthogonal with respect to that product and the sum of carried power fractions may be different from the total flux. In the non-conjugated definition, modes are orthogonal, but the interpretation of the dot product power carried by a given mode is no longer valid.
- outer_dot(field_data, conjugate=True)[source]#
Dot product (modal overlap) with another
FieldData
object.The tangential fields from
field_data
are interpolated to this object’s grid, so the data arrays don’t need to have the same discretization. The calculation is performed for all common frequencies between data arrays. In the output,mode_index_0
andmode_index_1
are the mode indices from this object andfield_data
, respectively, if they are instances ofModeSolverData
.- Parameters:
field_data (
ElectromagneticFieldData
) – A data instance to compute the dot product with.conjugate (bool = True) – If
True
(default), the dot product is defined as1 / 4
times the integral ofE_self* x H_other - H_self* x E_other
, wherex
is the cross product and*
is complex conjugation. IfFalse
, the complex conjugation is skipped.
- Returns:
Data array with the complex-valued modal overlaps between the two mode data.
- Return type:
xarray.DataArray
See also
- property time_reversed_copy#
Make a copy of the data with time-reversed fields.
- __hash__()#
Hash method.