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- # -*- coding: utf-8 -*-
- """
- Created on Mon Jun 22 20:51:40 2020
- @author: Ian Lim
- """
- from statefuncs import State, Basis
- from qedstatefuncs import FermionState, FermionBasis
- from phi1234 import Phi1234
- from schwinger import Schwinger
- from scipy.constants import pi
- import numpy as np
- import unittest
- import time
- from numpy.testing import assert_array_equal
- def calculateAxialCharge(state):
-
- total = 0
-
- for wn in np.arange(state.nmin, state.nmax+1):
- if wn < 0:
- total -= (state[wn][0]-state[wn][1])
- elif wn > 0:
- total += (state[wn][0]-state[wn][1])
-
- return total
- def calculateAxialChargeArray(basis):
- axialCharge = np.empty(basis.size)
- for i in range(basis.size):
- axialCharge[i] = calculateAxialCharge(basis[i])
- #print(axialCharge)
- return axialCharge
- class TestQAxial(unittest.TestCase):
- def setUp(self):
- self.schwinger = Schwinger()
- self.schwinger.buildFullBasis(Emax=3., m=0, L=2*pi, bcs="antiperiodic")
-
-
- def testMatrix(self):
- verbose = False
-
- start = time.time()
-
- #print([state.occs for state in a.fullBasis[-1]])
- self.schwinger.buildMatrix()
-
- axialCharge = calculateAxialChargeArray(self.schwinger.fullBasis)
-
- if verbose:
- print(axialCharge)
- print(f"Basis size: {axialCharge.size}")
- potential = self.schwinger.potential.M.toarray()
-
- for i in np.arange(axialCharge.size):
- for j in np.arange(axialCharge.size):
- if axialCharge[i] != axialCharge[j]:
- assert(potential[i,j]==0)
-
- #print(f"Runtime: {time.time()-start}")
-
- if verbose:
- print("Free Hamiltonian:")
- print(self.schwinger.h0.M.toarray())
- # we could check that the diagonal elements are the expected energies
-
- #order zero is just the mass term, which comes out to 2*pi here.
- print("Order zero potential matrix:")
- print(self.schwinger.potential.M.toarray())
-
- # def testAxialCharge(self):
- # axialCharge = calculateAxialChargeArray(self.schwinger.fullBasis)
-
-
-
- if __name__ == '__main__':
- unittest.main()
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