Plots the radiation pattern in polar coordinates. The angles increase clockwise with zero in the +z direction (the "pole") and π/2 in the +r

Plots the radiation pattern in polar coordinates. The angles increase clockwise with zero in the +z direction (the "pole") and π/2 in the +r

Plots the 3D radiation pattern as a contour plot. Args: dipole_pol: the polarization the electric dipole. Either x or y. radial_f

Plots the radiation pattern in 3d Cartesian coordinates. Args: radial_flux: radial flux of the far fields in polar coordinates.

Plots the radiation pattern in 3d Cartesian coordinates. Args: radial_flux: radial flux of the far fields at each angle.

Plots the radiation pattern in polar coordinates. The angles increase clockwise with zero at the top (+z direction). Args: radial_fl

Plots the radiation pattern in polar coordinates. Args: radial_flux: radial flux of the far fields at each angle.

Computes the radiation pattern from the far fields. Args: sim: a `Simulation` object. n2f_mon: a `DftNear2Far` object returned by

Computes the radiation pattern from the far fields. Args: sim: a `Simulation` object. n2f_mon: a `DftNear2Far` object returned by

Computes the radiation pattern from the far fields. Args: sim: a `Simulation` object. n2f_mon: a `DftNear2Far` object returned by

Computes the radiation pattern from the far fields. Args: e_field, h_field: the electric (Er, Ep, Ez) and magnetic (Hr, Hp, Hz)

Computes the radiation pattern from the near fields. Args: sim: a `Simulation` object. n2f_mon: a `DftNear2Far` object returned by `S

Returns the complex reflection coefficient of a TIR mode computed using the Fresnel equations. Args: pol: polarization of the inci

Returns the complex reflection coefficient of a TIR mode computed using mode decomposition. Args: pol: polarization of the inciden

Computes properties of the incident and reflected planewave. Args: theta_deg: angle of incident planewave. use_bfast: whe

allocate fields for components required by any source on any process ... this is needed after calling the low-level fields::add_srcdata

Lower level function called by `run_k_points` that runs a simulation for a single *k* point `k_point` and returns a `Harminv` instanc

Save the Fourier-transformed fields corresponding to the given flux object in an HDF5 file of the given `filename` without the `.h5`

from a previously created geom_epsilon object, set the materials as specified */

Is the current layout imbalanced enough to justify rebuilding the sim? Args: sim: the meep.Simulation object with the chunk layout

Compute quadrature points and weights for integrating on the unit sphere. x, y, z, and weight should be arrays of num_sq_pts values to hold the

Converts a point on the unit sphere from spherical to Cartesian coords. Args: polar_rad: polar angle of the point. 0° is +z. azim

this function is necessary to make equality commutative ... ugh

Computes the DFT fields from the mode source in a straight waveguide. The DFT fields are used as normalization of the reflectance measurement

Returns whether or not V is positive-definite. */

Returns whether or not V is positive-definite. */

Test that a 3D simulation with a 1D cell (zero size in X and Y) and Bloch-periodic boundaries does not crash. This exercises the boundary connection l