6#include <nda/layout/range.hpp>
7#include <nda/matrix_functions.hpp>
8#include <triqs/gfs.hpp>
9#include <triqs/utility/exceptions.hpp>
11#include <triqs/experimental/lattice/wannier_loader.hpp>
25 std::vector<atomic_orbs> atomic_shells) {
27 throw std::runtime_error(
"If performing a spin-polarized calculation, you need to supply two Wannier file paths for up and down channels.\n");
30 auto [R, HR, r_op, lvs] = read_wannier90_tb_data(wannier_file_path);
31 std::vector<tb_hk> tb_H;
32 tb_H.emplace_back(R, HR);
40 spin_kind_e spin_kind, std::vector<atomic_orbs> atomic_shells) {
43 throw std::runtime_error(
"For a non-spin polarized calculation, you should specify only one Wannier Hamiltonian.\n");
47 std::vector<tb_hk> tb_H;
48 for (
auto file : {wannier_file_path_up, wannier_file_path_dn}) {
49 auto [R, HR, r_op, lvs] = read_wannier90_tb_data(file);
50 tb_H.emplace_back(R, HR);
59 :
H{std::move(H_sigma)} {
62 if (
H[0].n_orbitals() !=
H[1].n_orbitals()) {
63 throw std::runtime_error(
64 "Cannot construct a one_body_elements "
65 "using up and down H_k that have a different number of orbitals.");
69 nda::array<nda::matrix<dcomplex>, 2> hloc =
Hloc(
H, atomic_shells);
72 double block_threshold = 1e-6;
73 bool diagonalize_hloc =
false;
74 auto [decomposition, U] =
discover_symmetries(hloc, atomic_shells, block_threshold, diagonalize_hloc);
82 nda::array<nda::matrix<dcomplex>, 2>
Hloc(std::vector<tb_hk>
const &H_sigma, std::vector<atomic_orbs>
const &atomic_shells) {
85 nda::array<nda::matrix<dcomplex>, 2> Hloc_result(atomic_shells.size(), H_sigma.size());
87 for (
auto [isigma, H] : enumerate(H_sigma)) {
91 for (
auto shell : atomic_shells) { n_orb += shell.dim; }
92 if (H.n_orbitals() != n_orb) {
93 throw std::runtime_error(
"TB Hamiltonian does not have the same number of orbitals as the provided atomic shells: HR "
94 + std::to_string(H.n_orbitals()) +
" , atomic_shells total " + std::to_string(n_orb));
98 auto iR0 = H.get_R_idx(std::array<long, 3>{0, 0, 0});
104 for (
auto &&[ishell, shell] : enumerate(atomic_shells)) {
105 auto Hloc0_ab = nda::zeros<dcomplex>(shell.dim, shell.dim);
107 for (
auto iorb : nda::range(shell.dim)) {
108 for (
auto jorb : nda::range(shell.dim)) { Hloc0_ab(iorb, jorb) = H[iR0](start_orb + iorb, start_orb + jorb); }
109 start_orb += shell.dim;
111 Hloc_result(ishell, isigma) = Hloc0_ab;
118 nda::array<nda::matrix<dcomplex>, 2> Hloc_result(1, obe.
C_space.
n_sigma());
119 for (
auto sigma : range(obe.
C_space.
n_sigma())) { Hloc_result(0, sigma) = obe.
H[sigma][{0, 0, 0}]; }
126 auto new_H = obe.
H | stdv::transform([&](
auto x) {
return fold(sl, x); }) | tl::to<std::vector>();
128 decltype(sh) new_atomic_shells;
130 nda::array<std::vector<long>, 2> new_dec(dec.extent(0) * sl.n_cluster_sites(), dec.extent(1));
131 for (
auto i : nda::range(sl.n_cluster_sites())) {
132 for (
auto &&[j, shell] : enumerate(sh)) {
133 new_atomic_shells.emplace_back(shell);
134 new_dec(i * sh.size() + j,
r_all) = dec(j,
r_all);
145 for (
auto &h : new_H) {
146 if (U.extent(0) != h.n_orbitals()) {
147 throw std::runtime_error(
148 "Cannot rotate a tb_hk with a unitary matrix that has a different number of rows than the number of orbitals in the Hamiltonian.");
150 for (
auto i : nda::range(
long(h.get_R_list().size()))) {
151 auto tR = nda::matrix<dcomplex>(h[i]);
152 h[i] = U * tR * dagger(U);
164 throw std::runtime_error(
"Can only extend to spin a non-spin-polarized one_body_elements_tb.");
167 auto const &Rs = obe.
H[0].get_R_list();
169 auto new_orb = 2 * n_orb;
171 auto extend_matrix = [&new_orb, &n_orb](
auto const &mat) {
172 auto ext_mat = nda::array<dcomplex, 2>(new_orb, new_orb);
173 for (
auto const &i : nda::range(n_orb)) {
174 for (
auto const &j : nda::range(n_orb)) {
175 ext_mat(i, j) = mat(i, j);
176 ext_mat(i + n_orb, j + n_orb) = mat(i, j);
182 std::vector<nda::array<dcomplex, 2>> new_hoppings;
183 for (
auto const &tR : obe.
H[0].hoppings()) new_hoppings.emplace_back(extend_matrix(tR));
184 auto new_tb_H = std::vector<tb_hk>{{Rs, std::move(new_hoppings)}};
187 auto new_atomic_shells = sh
188 | stdv::transform([](
auto const &s) {
return atomic_orbs{.dim = 2 * s.dim, .l = s.l, .cls_idx = s.cls_idx, .dft_idx = s.dft_idx}; })
189 | tl::to<std::vector>();
197 if (local_term.extent(0) != obe.
C_space.
dim()) {
198 throw std::runtime_error(
"Cannot add a local term with a different dimension than the one_body_elements_tb.");
201 auto new_tb_H = obe.
H;
202 for (
auto &h : new_tb_H) { h[{0, 0, 0}] += local_term; }
Describe the atomic orbitals within downfolded space.
spin_kind_e spin_kind() const
Spin kind of index.
long n_sigma() const
Dimension of the index.
nda::array< std::vector< long >, 2 > const & atoms_block_decomposition() const
2-dim array of all blocks spanning space -> atoms_block_decomposition.
long dim() const
Dimension of the correlated space.
std::vector< atomic_orbs > const & atomic_shells() const
List of all atomic shells spanning the space.
nda::array< nda::matrix< dcomplex >, 2 > impurity_levels(one_body_elements_on_grid const &obe)
Compute the local impurity levels from the single-particle dispersion.
one_body_elements_tb(std::vector< tb_hk > H_sigma, local_space ls)
Construct a one-body elements TB object from a list of tb_hk objects.
one_body_elements_tb one_body_elements_from_wannier90(std::string const &wannier_file_path, spin_kind_e spin_kind, std::vector< atomic_orbs > atomic_shells)
Construct a one-body elements TB object from Wannier90 in the case of a single spin index.
one_body_elements_tb rotate(one_body_elements_tb const &obe, nda::matrix< dcomplex > const &U)
Rotate a tight-binding Hamiltonian by a unitary matrix .
spin_kind_e
Kind of σ index.
nda::array< nda::matrix< dcomplex >, 2 > Hloc(std::vector< tb_hk > const &H_sigma, std::vector< atomic_orbs > const &atomic_shells)
Compute given tight binding Hamiltonians.
std::pair< nda::array< std::vector< long >, 2 >, nda::array< nda::matrix< dcomplex >, 2 > > discover_symmetries(nda::array< nda::matrix< dcomplex >, 2 > const &Hloc0, std::vector< atomic_orbs > const &atomic_shells, double block_threshold, bool diagonalize_hloc)
Find symmetries of the component of a Hamiltonian to determine a GF block structure.
one_body_elements_tb extend_to_spin(one_body_elements_tb const &obe)
one_body_elements_tb add_local_term(one_body_elements_tb const &obe, nda::matrix< dcomplex > const &local_term)
one_body_elements_tb fold(superlattice const &sl, one_body_elements_tb const &obe)
Convert a tight binding Hamiltonian to its superlattice equivalent.
static constexpr auto r_all
A one-body elements using a tight-binding Hamiltonian.
std::vector< tb_hk > H
List of TB Hamiltonians.
local_space C_space
Local space.