tidy3d.Medium2D#
- class Medium2D[source]#
Bases:
AbstractMedium
2D diagonally anisotropic medium.
- Parameters:
name (Attribute:
name
) –Type
Optional[str]
Default
= None
Description
Optional unique name for medium.
frequency_range (Attribute:
frequency_range
) –Type
Optional[Tuple[float, float]]
Default
= None
Units
(Hz, Hz)
Description
Optional range of validity for the medium.
allow_gain (Attribute:
allow_gain
) –Type
bool
Default
= False
Description
Allow the medium to be active. Caution: simulations with a gain medium are unstable, and are likely to diverge.Simulations where ‘allow_gain’ is set to ‘True’ will still be charged even if diverged. Monitor data up to the divergence point will still be returned and can be useful in some cases.
nonlinear_spec (Attribute:
nonlinear_spec
) –Type
Union[NonlinearSpec, NonlinearSusceptibility]
Default
= None
Description
Nonlinear spec applied on top of the base medium properties.
modulation_spec (Attribute:
modulation_spec
) –Type
Optional[ModulationSpec]
Default
= None
Description
Modulation spec applied on top of the base medium properties.
heat_spec (Attribute:
heat_spec
) –Type
Union[FluidSpec, SolidSpec, NoneType]
Default
= None
Description
Specification of the medium heat properties. They are used for solving the heat equation via the
HeatSimulation
interface. Such simulations can be used for investigating the influence of heat propagation on the properties of optical systems. Once the temperature distribution in the system is found usingHeatSimulation
object,Simulation.perturbed_mediums_copy()
can be used to convert mediums with perturbation models defined into spatially dependent custom mediums. Otherwise, theheat_spec
does not directly affect the running of an opticalSimulation
.ss (Attribute:
ss
) –Type
Union[Medium, PoleResidue, Sellmeier, Lorentz, Debye, Drude, PECMedium]
Default
Description
Medium describing the ss-component of the diagonal permittivity tensor. The ss-component refers to the in-plane dimension of the medium that is the first component in order of ‘x’, ‘y’, ‘z’. If the 2D material is normal to the y-axis, for example, then this determines the xx-component of the corresponding 3D medium.
tt (Attribute:
tt
) –Type
Union[Medium, PoleResidue, Sellmeier, Lorentz, Debye, Drude, PECMedium]
Default
Description
Medium describing the tt-component of the diagonal permittivity tensor. The tt-component refers to the in-plane dimension of the medium that is the second component in order of ‘x’, ‘y’, ‘z’. If the 2D material is normal to the y-axis, for example, then this determines the zz-component of the corresponding 3D medium.
Notes
Only diagonal anisotropy is currently supported.
Example
>>> drude_medium = Drude(eps_inf=2.0, coeffs=[(1,2), (3,4)]) >>> medium2d = Medium2D(ss=drude_medium, tt=drude_medium)
Attributes
The diagonal elements of the 2D medium as a dictionary.
Whether the medium is a PEC.
This property computes the index of refraction related to CFL condition, so that the FDTD with this medium is stable when the time step size that doesn't take material factor into account is multiplied by
n_cfl
.Methods
eps_diagonal
(frequency)Main diagonal of the complex-valued permittivity tensor as a function of frequency.
eps_model
(frequency)Complex-valued permittivity as a function of frequency.
from_anisotropic_medium
(medium, axis, thickness)Generate a
Medium2D
equivalent of aAnisotropicMedium
with given normal axis and thickness.from_dispersive_medium
(medium, thickness)Generate a
Medium2D
equivalent of aDispersiveMedium
with a given thickness.from_medium
(medium, thickness)Generate a
Medium2D
equivalent of aMedium
with a given thickness.is_comp_pec_2d
(comp, axis)Whether the medium is a PEC.
plot
(freqs[, ax])Plot n, k of a
Medium
as a function of frequency.plot_sigma
(freqs[, ax])Plot the surface conductivity of the 2D material.
sigma_model
(freq)Complex-valued conductivity as a function of frequency.
to_anisotropic_medium
(axis, thickness)Generate a 3D
AnisotropicMedium
equivalent of a given thickness.to_medium
(thickness)Generate a
Medium
equivalent of a given thickness.to_pole_residue
(thickness)Generate a
PoleResidue
equivalent of a given thickness.volumetric_equivalent
(axis, adjacent_media, ...)Produces a 3D volumetric equivalent medium.
- ss#
- tt#
- volumetric_equivalent(axis, adjacent_media, adjacent_dls)[source]#
Produces a 3D volumetric equivalent medium. The new medium has thickness equal to the average of the
dls
in theaxis
direction. The ss and tt components of the 2D material are mapped in order onto the xx, yy, and zz components of the 3D material, excluding theaxis
component. The conductivity and residues (in the case of a dispersive 2D material) are rescaled by1/dl
. The neighboring medianeighbors
enter in as a background for the resulting volumetric equivalent.- Parameters:
axis (Axis) – Index (0, 1, or 2 for x, y, or z respectively) of the normal direction to the 2D material.
adjacent_media (Tuple[MediumType3D, MediumType3D]) – The neighboring media on either side of the 2D material. The first element is directly on the - side of the 2D material in the supplied axis, and the second element is directly on the + side.
adjacent_dls (Tuple[float, float]) – Each dl represents twice the thickness of the desired volumetric model on the respective side of the 2D material.
- Returns:
The 3D material corresponding to this 2D material.
- Return type:
- to_anisotropic_medium(axis, thickness)[source]#
Generate a 3D
AnisotropicMedium
equivalent of a given thickness.- Parameters:
axis (Axis) – The normal axis to the 2D medium.
thickness (float) – The thickness of the desired 3D medium.
- Returns:
The 3D equivalent of this 2D medium.
- Return type:
- to_pole_residue(thickness)[source]#
Generate a
PoleResidue
equivalent of a given thickness. The 2D medium to be isotropic in-plane (otherwise the components are averaged).- Parameters:
thickness (float) – The thickness of the desired 3D medium.
- Returns:
The 3D equivalent pole residue model of this 2D medium.
- Return type:
- to_medium(thickness)[source]#
Generate a
Medium
equivalent of a given thickness. The 2D medium must be isotropic in-plane (otherwise the components are averaged) and non-dispersive besides a constant conductivity.- Parameters:
thickness (float) – The thickness of the desired 3D medium.
- Returns:
The 3D equivalent of this 2D medium.
- Return type:
- classmethod from_medium(medium, thickness)[source]#
Generate a
Medium2D
equivalent of aMedium
with a given thickness.
- classmethod from_dispersive_medium(medium, thickness)[source]#
Generate a
Medium2D
equivalent of aDispersiveMedium
with a given thickness.- Parameters:
medium (
DispersiveMedium
) – The 3D dispersive medium to convert.thickness (float) – The thickness of the 3D material.
- Returns:
The 2D equivalent of the given 3D medium.
- Return type:
- classmethod from_anisotropic_medium(medium, axis, thickness)[source]#
Generate a
Medium2D
equivalent of aAnisotropicMedium
with given normal axis and thickness. Thess
andtt
components of the resulting 2D medium correspond to the first of thexx
,yy
, andzz
components of the 3D medium, with theaxis
component removed.- Parameters:
medium (
AnisotropicMedium
) – The 3D anisotropic medium to convert.axis (
Axis
) – The normal axis to the 2D material.thickness (float) – The thickness of the 3D material.
- Returns:
The 2D equivalent of the given 3D medium.
- Return type:
- eps_diagonal(frequency)[source]#
Main diagonal of the complex-valued permittivity tensor as a function of frequency.
- sigma_model(freq)[source]#
Complex-valued conductivity as a function of frequency.
- Parameters:
freq (float) – Frequency to evaluate conductivity at (Hz).
- Returns:
Complex conductivity at this frequency.
- Return type:
complex
- property elements#
The diagonal elements of the 2D medium as a dictionary.
- property n_cfl#
This property computes the index of refraction related to CFL condition, so that the FDTD with this medium is stable when the time step size that doesn’t take material factor into account is multiplied by
n_cfl
.
- property is_pec#
Whether the medium is a PEC.
- __hash__()#
Hash method.