tidy3d.ModeSpec#
- class ModeSpec[source]#
Bases:
Tidy3dBaseModel
Stores specifications for the mode solver to find an electromagntic mode.
- Parameters:
attrs (dict = {}) โ Dictionary storing arbitrary metadata for a Tidy3D object. This dictionary can be freely used by the user for storing data without affecting the operation of Tidy3D as it is not used internally. Note that, unlike regular Tidy3D fields,
attrs
are mutable. For example, the following is allowed for setting anattr
obj.attrs['foo'] = bar
. Also note that Tidy3D` will raise aTypeError
ifattrs
contain objects that can not be serialized. One can check ifattrs
are serializable by callingobj.json()
.num_modes (PositiveInt = 1) โ Number of modes returned by mode solver.
target_neff (Optional[PositiveFloat] = None) โ Guess for effective index of the mode.
num_pml (Tuple[NonNegativeInt, NonNegativeInt] = (0, 0)) โ Number of standard pml layers to add in the two tangential axes.
filter_pol (Optional[Literal['te', 'tm']] = None) โ The solver always computes the
num_modes
modes closest to the giventarget_neff
. Iffilter_pol==None
, they are simply sorted in order of decreasing effective index. If a polarization filter is selected, the modes are rearranged such that the firstn_pol
modes in the list are the ones with the selected polarization fraction larger than or equal to 0.5, while the nextnum_modes - n_pol
modes are the ones where it is smaller than 0.5 (i.e. the opposite polarization fraction is larger than 0.5). Within each polarization subset, the modes are still ordered by decreasing effective index.te
-fraction is defined as the integrated intensity of the E-field component parallel to the first plane axis, normalized to the total in-plane E-field intensity. Conversely,tm
-fraction uses the E field component parallel to the second plane axis.angle_theta (float = 0.0) โ [units = rad]. Polar angle of the propagation axis from the injection axis.
angle_phi (float = 0.0) โ [units = rad]. Azimuth angle of the propagation axis in the plane orthogonal to the injection axis.
precision (Literal['single', 'double'] = single) โ The solver will be faster and using less memory under single precision, but more accurate under double precision.
bend_radius (Optional[float] = None) โ [units = um]. A curvature radius for simulation of waveguide bends. Can be negative, in which case the mode plane center has a smaller value than the curvature center along the tangential axis perpendicular to the bend axis.
bend_axis (Optional[Literal[0, 1]] = None) โ Index into the two tangential axes defining the normal to the plane in which the bend lies. This must be provided if
bend_radius
is notNone
. For example, for a ring in the global xy-plane, and a mode plane in either the xz or the yz plane, thebend_axis
is always 1 (the global z axis).track_freq (Optional[Literal['central', 'lowest', 'highest']] = central) โ Parameter that turns on/off mode tracking based on their similarity. Can take values
'lowest'
,'central'
, or'highest'
, which correspond to mode tracking based on the lowest, central, or highest frequency. IfNone
no mode tracking is performed.group_index_step (Union[PositiveFloat, bool] = False) โ Control the computation of the group index alongside the effective index. If set to a positive value, it sets the fractional frequency step used in the numerical differentiation of the effective index to compute the group index. If set to True, the default of 0.005 is used.
Notes
The
angle_theta
andangle_phi
parameters define the injection axis as illustrated in the figure below, with respect to the axis normal to the mode plane (x
in the figure). Note thatangle_theta
must be smaller than \(\frac{pi}{2}\). To inject in the backward direction, we can still use thedirection
parameter as also shown in the figure. Similarly, the mode amplitudes computed in mode monitors are defined w.r.t. theforward
andbackward
directions as illustrated. Note, the planar axes are found by popping the injection axis from{x,y,z}
. For example, if injection axis isy
, the planar axes are ordered{x,z}
.The
bend_axis
is the axis normal to the plane in which the bend lies, (z
in the diagram below). In the mode specification, it is defined locally for the mode plane as one of the two axes tangential to the plane. In the case of bends that lie in thexy
-plane, the mode plane would be either inxz
or inyz
, so in both cases the correct setting isbend_axis=1
, selecting the globalz
. Thebend_radius
is counted from the center of the mode plane to the center of the curvature, along the tangential axis perpendicular to the bend axis. This radius can also be negative, if the center of the mode plane is smaller than the center of the bend.Example
>>> mode_spec = ModeSpec(num_modes=3, target_neff=1.5)
See also
Attributes
Methods
Assign the default fractional frequency step value if not provided.
bend_axis_given
(val,ย values)Check that
bend_axis
is provided ifbend_radius
is notNone
bend_radius_not_zero
(val,ย values)Check that
bend_raidus
magnitude is not close to zero.`Ensure a reasonable group index step is used.
check_precision
(values)Verify critical ModeSpec settings for group index calculation.
glancing_incidence
(val)Warn if close to glancing incidence.
Inherited Common Usage
- num_modes#
- target_neff#
- num_pml#
- filter_pol#
- angle_theta#
- angle_phi#
- precision#
- bend_radius#
- bend_axis#
- track_freq#
- group_index_step#
- classmethod bend_axis_given(val, values)[source]#
Check that
bend_axis
is provided ifbend_radius
is notNone
- classmethod bend_radius_not_zero(val, values)[source]#
Check that
bend_raidus
magnitude is not close to zero.`
- classmethod assign_default_on_true(val)[source]#
Assign the default fractional frequency step value if not provided.
- classmethod check_precision(values)[source]#
Verify critical ModeSpec settings for group index calculation.
- __hash__()#
Hash method.