Returns the bounding box of the domain spanned in the plotfile */

Returns the physical co-ordinates of the upper corner in dimension, idim, * that corresponds the to the respective plotfile data. */

Returns the physical co-ordinates of the lower corner in dimension, idim, * that corresponds the to the respective plotfile data */

This function returns the particle data stored in a particular plot file and particle type. It returns two numpy arrays, the first conta

Replace equivalent names in ``txt``, e.g., "seconds" -> "s". Each key, value in ``equiv_dict`` is a preferred name and equivalent name list,

Compute the right-hand side of ODE system that solves the global model described below. The global model solves for the evolution of plasma densit

The theoretical size of a focusing beam (in the absence of space charge), at position z, given its emittance and size at focus.

The theoretical size of a focusing beam (in the absence of space charge), at position z, given its emittance and size at focus.

* \brief Shuffle the particles in each cell using the Fisher-Yates algorithm, for both species. * * @param[inout] a_indices_1 the indices of

\brief Convert a snake_case string to a camelCase one. * * WarpX uses snake_case internally for some component * names, but OpenPMD a

Calculate the coefficient in equation 14.13 from "Introduction to Plasma Physics", Goldston and Rutherford. ne: electron density Te: elect

ni: background ion density Ti: background ion temperature (eV) mi: background ion mass Zi: background ion charge state Zb: ion ch

Visualize densities and fields of a single iteration. :param ts: OpenPMDTimeSeries :param iteration: Output iteration (simulation timest

* \brief Accumulate velocity moments for matched temperature deposition using particle shapes * * \param[in,out] T_vf vector field of Temper

Add new_particles to existing to obtain the total number of particles of the species. \param[in] new_particles total particles in the new buff

This scales the mass matrices used in the PC by the inverse volume and wraps around the deposition at negative radius. It is faster to apply this on t

* \brief Update the B field at the boundary, using the Silver-Mueller condition */

* \brief Checks for known numerical issues involving different electromagnetic solvers */

* \brief For the face of cell pointing in direction idim, return the number of faces * we need to intrude with the eight-ways extension. *

* \brief For the face of cell pointing in direction idim, return the number of faces * we need to intrude with the one-way extension. Returns only

\brief Continuous injection of a flux of particles * Loop over all WarpXParticleContainer in MultiParticleContainer and * calls virtual function Con

\brief Continuous injection for particles initially outside of the domain. * \param injection_box: Domain where new particles should be injected. *

\brief Calculate temperature from the particles. * The result is put in the MultiFab registry. * \param lev Level of box that contains partic

Check if any diagnostics will be done

Whether the last timestep is always dumped */

Return the radial electric field as an array of the same length as z and r, in the half-plane theta=0

Return the radial electric field as an array of the same length as r, in the half-plane theta=0

Return the longitudinal electric field as an array of the same length as z and r, in the half-plane theta=0

Returns physical co-ordinates of the lower-corner for the i-th Fab. * \param[in] iFab id of the ith Fab in the list of Multifabs * \return

Returns physical co-ordinates of the lower-corner for the i-th Fab. * \param[in] iFab id of the ith Fab in the list of Multifabs * \return

Returns name of the ith fab stored in the MultiFab. */