tidy3d.components.medium.AbstractMedium

class AbstractMedium

Bases: ABC, Tidy3dBaseModel

A medium within which electromagnetic waves propagate.

Parameters:

• name (Optional[str] = None) – Optional unique name for medium.

• frequency_range (Optional[Tuple[float, float]] = None) – [units = (Hz, Hz)]. Optional range of validity for the medium.

• allow_gain (bool = False) – 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 (Union[NonlinearSpec, NonlinearSusceptibility] = None) – Nonlinear spec applied on top of the base medium properties.

• modulation_spec (Optional[ModulationSpec] = None) – Modulation spec applied on top of the base medium properties.

• heat_spec (Union[FluidSpec, SolidSpec, NoneType] = None) – 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 using HeatSimulation object, Simulation.perturbed_mediums_copy() can be used to convert mediums with perturbation models defined into spatially dependent custom mediums. Otherwise, the heat_spec does not directly affect the running of an optical Simulation.

Attributes

is_pec	Whether the medium is a PEC.
n_cfl	To ensure a stable FDTD simulation, it is essential to select an appropriate time step size in accordance with the CFL condition.
time_modulated	Whether any component of the medium is time modulated.

Methods

eps_comp(row, col, frequency)	Single component of the complex-valued permittivity tensor as a function of frequency.
eps_complex_to_eps_sigma(eps_complex, freq)	Convert complex permittivity at frequency freq to permittivity and conductivity values.
eps_complex_to_nk(eps_c)	Convert complex permittivity to n, k values.
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.
eps_sigma_to_eps_complex(eps_real, sigma, freq)	convert permittivity and conductivity to complex permittivity at freq
nk_model(frequency)	Real and imaginary parts of the refactive index as a function of frequency.
nk_to_eps_complex(n[, k])	Convert n, k to complex permittivity.
nk_to_eps_sigma(n, k, freq)	Convert n, k at frequency freq to permittivity and conductivity values.
plot(freqs[, ax])	Plot n, k of a Medium as a function of frequency.
sel_inside(bounds)	Return a new medium that contains the minimal amount data necessary to cover a spatial region defined by bounds.
sigma_model(freq)	Complex-valued conductivity as a function of frequency.

name

frequency_range

allow_gain

nonlinear_spec

modulation_spec

heat_spec

property time_modulated

Whether any component of the medium is time modulated.

abstract eps_model(frequency)

Complex-valued permittivity as a function of frequency.

Parameters:

frequency (float) – Frequency to evaluate permittivity at (Hz).

Returns:

Complex-valued relative permittivity evaluated at frequency.

Return type:

complex

nk_model(frequency)

Real and imaginary parts of the refactive index as a function of frequency.

Parameters:

frequency (float) – Frequency to evaluate permittivity at (Hz).

Returns:

Real part (n) and imaginary part (k) of refractive index of medium.

Return type:

Tuple[float, float]

eps_diagonal(frequency)

Main diagonal of the complex-valued permittivity tensor as a function of frequency.

Parameters:

frequency (float) – Frequency to evaluate permittivity at (Hz).

Returns:

The diagonal elements of the relative permittivity tensor evaluated at frequency.

Return type:

complex

eps_comp(row, col, frequency)

Single component of the complex-valued permittivity tensor as a function of frequency.

Parameters:

• row (int) – Component’s row in the permittivity tensor (0, 1, or 2 for x, y, or z respectively).

• col (int) – Component’s column in the permittivity tensor (0, 1, or 2 for x, y, or z respectively).

• frequency (float) – Frequency to evaluate permittivity at (Hz).

Returns:

Element of the relative permittivity tensor evaluated at frequency.

Return type:

complex

abstract property n_cfl

To ensure a stable FDTD simulation, it is essential to select an appropriate time step size in accordance with the CFL condition. The maximal time step size is inversely proportional to the speed of light in the medium, and thus proportional to the index of refraction. However, for dispersive medium, anisotropic medium, and other more complicated media, there are complications in deciding on the choice of the index of refraction.

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.

plot(freqs, ax=None)

Plot n, k of a Medium as a function of frequency.

Parameters:

• freqs (float) – Frequencies (Hz) to evaluate the medium properties at.

• ax (matplotlib.axes._subplots.Axes = None) – Matplotlib axes to plot on, if not specified, one is created.

Returns:

The supplied or created matplotlib axes.

Return type:

matplotlib.axes._subplots.Axes

static nk_to_eps_complex(n, k=0.0)

Convert n, k to complex permittivity.

Parameters:

• n (float) – Real part of refractive index.

• k (float = 0.0) – Imaginary part of refrative index.

Returns:

Complex-valued relative permittivity.

Return type:

complex

static eps_complex_to_nk(eps_c)

Convert complex permittivity to n, k values.

Parameters:

eps_c (complex) – Complex-valued relative permittivity.

Returns:

Real and imaginary parts of refractive index (n & k).

Return type:

Tuple[float, float]

static nk_to_eps_sigma(n, k, freq)

Convert n, k at frequency freq to permittivity and conductivity values.

Parameters:

• n (float) – Real part of refractive index.

• k (float = 0.0) – Imaginary part of refrative index.

• frequency (float) – Frequency to evaluate permittivity at (Hz).

Returns:

Real part of relative permittivity & electric conductivity.

Return type:

Tuple[float, float]

static eps_sigma_to_eps_complex(eps_real, sigma, freq)

convert permittivity and conductivity to complex permittivity at freq

Parameters:

• eps_real (float) – Real-valued relative permittivity.

• sigma (float) – Conductivity.

• freq (float) – Frequency to evaluate permittivity at (Hz). If not supplied, returns real part of permittivity (limit as frequency -> infinity.)

Returns:

Complex-valued relative permittivity.

Return type:

complex

static eps_complex_to_eps_sigma(eps_complex, freq)

Convert complex permittivity at frequency freq to permittivity and conductivity values.

Parameters:

• eps_complex (complex) – Complex-valued relative permittivity.

• freq (float) – Frequency to evaluate permittivity at (Hz).

Returns:

Real part of relative permittivity & electric conductivity.

Return type:

Tuple[float, float]

sigma_model(freq)

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 is_pec

Whether the medium is a PEC.

sel_inside(bounds)

Return a new medium that contains the minimal amount data necessary to cover a spatial region defined by bounds.

Parameters:

bounds (Tuple[float, float, float], Tuple[float, float float]) – Min and max bounds packaged as (minx, miny, minz), (maxx, maxy, maxz).

Returns:

Medium with reduced data.

Return type:

AbstractMedium

__hash__()

Hash method.