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AlmaBTE
1.3
A solver of the space- and time-dependent Boltzmann transport equation for phonons
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Code related to BTE calculations beyond the RTA. More...
#include <constants.hpp>
#include <structures.hpp>
#include <qpoint_grid.hpp>
#include <processes.hpp>
#include <isotopic_scattering.hpp>
#include <boost/mpi.hpp>
#include <Eigen/Dense>
Go to the source code of this file.
Functions | |
Eigen::MatrixXd | alma::beyondRTA::calc_kappa (const alma::Crystal_structure &poscar, const alma::Gamma_grid &grid, const alma::Symmetry_operations &syms, const std::vector< alma::Threeph_process > &threeph_procs, const std::vector< alma::Twoph_process > &twoph_procs, const Eigen::Ref< const Eigen::ArrayXXd > &w0, double T, bool iterative, boost::mpi::communicator &world) |
Obtain the thermal conductivity of a bulk system under the full BTE (beyond Relaxation Time Approximation). More... | |
Code related to BTE calculations beyond the RTA.
Eigen::MatrixXd alma::beyondRTA::calc_kappa | ( | const alma::Crystal_structure & | poscar, |
const alma::Gamma_grid & | grid, | ||
const alma::Symmetry_operations & | syms, | ||
const std::vector< alma::Threeph_process > & | threeph_procs, | ||
const std::vector< alma::Twoph_process > & | twoph_procs, | ||
const Eigen::Ref< const Eigen::ArrayXXd > & | w0, | ||
double | T, | ||
bool | iterative, | ||
boost::mpi::communicator & | world | ||
) |
Obtain the thermal conductivity of a bulk system under the full BTE (beyond Relaxation Time Approximation).
This is achieved by deterministic solution a linear system for the irreducible q-points.
[in] | poscar | - description of the unit cell |
[in] | grid | - phonon spectrum on a regular q-point grid |
[in] | syms | - symmetry operations object |
[in] | threeph_procs | - list of 3-phonon processes |
[in] | twoph_procs | - list of 2-phonon processes |
[in] | w0 | - RTA scattering rates |
[in] | T | - temperature in K |
[in] | iterative | - use iterative Eigen solver for faster computation |