Program Listing for File kondoSC.hpp¶
↰ Return to documentation for file (models/kondoSC.hpp
)
#pragma once
#include "models/fermionBasis.hpp"
#include "nrgcore/qOperator.hpp"
#include "nrgcore/qsymmetry.hpp"
#include "utils/qmatrix.hpp"
#include <algorithm>
#include <cmath>
#include <complex>
#include <cstddef>
#include <iostream>
#include <map>
#include <optional>
#include <string>
#include <vector>
class kondoSC {
fermionBasis localSCbabsis;
public:
kondoSC(double JKondo, double spinS, double localDelta)
: localSCbabsis(2, fermionBasis::spinOnly) {
createBasis(JKondo, spinS,
localDelta); // create the basis in nstates x nstates
}
[[nodiscard]] std::vector<std::vector<int>> get_basis() const { return n_Q; }
[[nodiscard]] std::vector<std::vector<double>> get_eigenvaluesQ() const {
return eigenvalues_Q;
}
[[nodiscard]] std::vector<double> get_chi_Q() const { return chi_Q; }
//
std::vector<std::vector<double>> eigenvalues_Q;
std::vector<double> chi_Q;
std::vector<std::vector<int>> n_Q;
// ########################################
private:
void createBasis(double JKondo, double spinS, double localDelta) {
// TODO(saurabh): check spinS is multiple of 2.
auto spinDim = static_cast<size_t>(2. * spinS + 1.);
std::cout << "spinDim: " << spinDim << std::endl;
qmatrix<double> spinSz(spinDim, spinDim, 0);
qmatrix<double> spinSplus(spinDim, spinDim, 0);
// Spin Z
for (size_t i = 0; i < spinDim; i++) {
double m = -spinS + i * 1.0;
spinSz(i, i) = m;
if (i != (spinDim - 1)) {
std::cout << "spinDim: " << i << " " << spinDim << std::endl;
spinSplus(i, i + 1) = std::sqrt(spinS * (spinS + 1.) - m * (m + 1));
}
}
std::cout << "spinSz: \n" << spinSz << std::endl;
std::cout << "spinSplus: \n" << spinSplus << std::endl;
auto spinSminus = spinSplus.cTranspose();
auto spinSx = (spinSplus + spinSminus) * 0.5;
auto spinSy = (spinSplus - spinSminus) * 0.5; // -i is omitted here.
// ########################################
std::cout << "spinSx: " << spinSx << std::endl;
std::cout << "spinSy: " << spinSy << std::endl;
std::cout << "spinSz: " << spinSz << std::endl;
// ########################################
// create basis
qmatrix<> fdag = {0, 0, 1, 0};
qmatrix<> sigz = {1, 0, 0, -1};
qmatrix<> id2 = {1, 0, 0, 1};
// Create c_up and c_Down operator
// Addting and additional operators should be done in the same way.
auto c_up_dag = fdag.krDot(id2);
auto c_Down_dag = sigz.krDot(fdag);
// Create Wilson Site spin operators
auto wSpinx = (c_up_dag.dot(c_Down_dag.cTranspose()) +
c_Down_dag.dot(c_up_dag.cTranspose())) *
0.5;
auto wSpiny = (c_Down_dag.dot(c_up_dag.cTranspose()) -
c_up_dag.dot(c_Down_dag.cTranspose())) *
0.5; // -i is omitted here.
auto wSpinz = (c_up_dag.dot(c_up_dag.cTranspose()) -
c_Down_dag.dot(c_Down_dag.cTranspose())) *
0.5;
auto wNtotal =
(c_up_dag.dot(c_up_dag.cTranspose()) +
c_Down_dag.dot(
c_Down_dag.cTranspose())); // Create Hamiltonian spin operator
// ########################################################
std::cout << "wSpinx: " << wSpinx << std::endl;
std::cout << "wSpiny: " << wSpiny << std::endl;
std::cout << "wSpinz: " << wSpinz << std::endl;
// ############################################
auto Hamiltonian =
(spinSz.krDot(wSpinz) + spinSx.krDot(wSpinx) //
- spinSy.krDot(wSpiny)) * // Imaginary part is taken care here
JKondo
// SC term
+ spinSz.id().krDot(
(c_up_dag.dot(c_Down_dag) +
c_Down_dag.cTranspose().dot(c_Down_dag.cTranspose()))) *
localDelta;
// End
// std::cout << "spinSz: " << spinSz << std::endl;
spinSz = qmatrix(spinSz.krDot(wSpinx.id()));
// std::cout << "spinSz: " << spinSz << std::endl;
wSpinz = spinSx.id().krDot(wSpinz);
wNtotal = spinSx.id().krDot(wNtotal);
std::cout << "wSpinz: " << wSpinz * 2 << std::endl;
c_up_dag = spinSx.id().krDot(c_up_dag);
c_Down_dag = spinSx.id().krDot(c_Down_dag);
fnParticle.clear();
// Number of particles
fnParticle.push_back(((spinSz.id() + spinSz * 2.) * 0.5).getdiagonal());
fnParticle.push_back(((spinSz.id() - spinSz * 2.) * 0.5).getdiagonal());
fnParticle.push_back(((wNtotal + wSpinz * 2.) * 0.5).getdiagonal());
fnParticle.push_back(((wNtotal - wSpinz * 2.) * 0.5).getdiagonal());
//
std::cout << "fnParticle: " << fnParticle << std::endl;
// set the symmetries of the system
// create_QuantumNspinCharge();
// spin is only quantum number that is conserved
std::vector<size_t> tm1;
std::vector<size_t> tm2;
for (size_t j = 0; j < fnParticle.size(); j++) {
if (j % 2 == 0) { // Spin up
tm1.push_back(j);
} else { // Spin down
tm2.push_back(j);
}
}
std::vector<std::vector<size_t>> SpinSz = {tm1, tm2};
create_QuantumSpinOnly(SpinSz);
// create the quantum numbers
// create the quantum numbers
create_Block_structure();
// ####################################################################
n_Q = get_unique_Qnumbers();
// set chi_Q
chi_Q.clear();
for (auto ai : n_Q) {
double t_charge = std::accumulate(ai.begin(), ai.end(), 0);
chi_Q.push_back(std::pow(-1., t_charge));
}
//
// set foperator
auto h_blocked = get_block_Hamiltonian(Hamiltonian);
std::cout << "h_blocked: " << h_blocked << std::endl;
std::cout << "Hamiltonian: " << Hamiltonian << std::endl;
// Diagonalize the hamilton
eigenvalues_Q.clear();
eigenvalues_Q.resize(n_Q.size(), {});
for (size_t i = 0; i < n_Q.size(); i++) {
eigenvalues_Q[i] = (h_blocked.get(i, i)).value()->diag();
}
// TODO: rotate the f operator
// ####################################################################
f_dag_operator = get_block_operators({c_up_dag, c_Down_dag});
std::cout << "f_dag_operators: " << f_dag_operator.size() << std::endl;
std::vector<qOperator> topr(f_dag_operator.size(), qOperator());
for (size_t ip = 0; ip < f_dag_operator.size(); ip++) {
for (size_t i = 0; i < n_Q.size(); i++) {
for (size_t j = 0; j < n_Q.size(); j++) {
auto tfopr = f_dag_operator[ip].get(i, j);
if (tfopr) {
topr[ip].set((h_blocked.get(i, i))
.value()
->cTranspose()
.dot(*tfopr.value())
.dot(*(h_blocked.get(j, j)).value()),
i, j);
}
}
}
}
f_dag_operator = topr;
}
// ######################################
};