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test.py
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import pytest
from abtools.tools import AbinitioToolsClass
from abtools.utils import heatmap_ao
from matplotlib import pyplot as plt
from pyscf import gto
from pyscf.fci import direct_spin1
import numpy as np
def generate_ints(norb, U=30, V=10):
int1e = np.zeros((norb, norb), dtype=float)
int2e = np.zeros((norb, norb, norb, norb), dtype=float)
for i in range(norb):
int1e[i, (i + 1) % norb] = 1
int1e[(i + 1) % norb, i] = 1
int2e[i, i, i, i] = U
int2e[i, i, (i + 1) % norb, (i + 1) % norb] = V
int2e[(i + 1) % norb, (i + 1) % norb, i, i] = V
return int1e, int2e
def test_spin_corr():
norb = 12
nelec = 18
mol = gto.Mole()
myclass = AbinitioToolsClass(mol)
int1e, int2e = generate_ints(norb)
cis = direct_spin1.FCISolver()
e, c = cis.kernel(int1e, int2e, norb, nelec)
dm1, dm2 = cis.make_rdm12s(c, norb, nelec)
myclass.dm1 = dm1
myclass.dm2 = dm2
s00 = myclass.calc_spin_corr(0, 0)
s01 = myclass.calc_spin_corr(0, 1)
s02 = myclass.calc_spin_corr(0, 2)
s03 = myclass.calc_spin_corr(0, 3)
print(s00, s01, s02, s03)
assert s00 > s01
assert s01 > s02
return
def test_chg_corr():
norb = 12
nelec = 18
mol = gto.Mole()
myclass = AbinitioToolsClass(mol)
int1e, int2e = generate_ints(norb)
cis = direct_spin1.FCISolver()
e, c = cis.kernel(int1e, int2e, norb, nelec)
dm1, dm2 = cis.make_rdm12s(c, norb, nelec)
myclass.dm1 = dm1
myclass.dm2 = dm2
c00 = myclass.calc_chg_corr(0, 0)
c01 = myclass.calc_chg_corr(0, 1)
c02 = myclass.calc_chg_corr(0, 2)
c03 = myclass.calc_chg_corr(0, 3)
print(c00, c01, c02, c03)
assert abs(c00) > abs(c01)
assert abs(c01) > abs(c02)
return
def test_cc_corr():
norb = 12
nelec = 18
mol = gto.Mole()
myclass = AbinitioToolsClass(mol)
int1e, int2e = generate_ints(norb)
myclass.hcore = int1e
cis = direct_spin1.FCISolver()
e, c = cis.kernel(int1e, int2e, norb, nelec)
dm1, dm2 = cis.make_rdm12s(c, norb, nelec)
myclass.dm1 = dm1
myclass.dm2 = dm2
jj01 = myclass.calc_jj(0, 1)
jj02 = myclass.calc_jj(0, 2)
jj03 = myclass.calc_jj(0, 3)
print(jj01, jj02, jj03)
assert jj01 >= jj02
assert jj02 >= jj03
return
def test_example():
dist = 0.7
hydrogen = gto.M(
atom=f"""
H 0.000000 0.00000 0.000000
H 0.000000 0.00000 {dist}
H 0.000000 0.00000 {dist*2}
H 0.000000 0.00000 {dist*3}
""",
basis="sto-3g", # 基底関数系: STO-3Gを使用
verbose=0,
)
mf_jj = AbinitioToolsClass(hydrogen)
mf_jj.run_uks()
mf_jj.calc_jj(0, 1)
dist = 0.7
hydrogen = gto.M(
atom=f"""
H 0.000000 0.00000 0.000000
H 0.000000 0.00000 {dist}
H 0.000000 0.00000 {dist*2}
H 0.000000 0.00000 {dist*3}
""",
basis="sto-3g",
verbose=0,
)
mf_jj = AbinitioToolsClass(hydrogen)
mf_jj.run_uks()
mf_jj.calc_spin_corr(0, 1)
return
def run_example(dist, frm, to):
hydrogen = gto.M(
atom=f"""
H 0.000000 0.00000 0.000000
H 0.000000 0.00000 {dist}
H 0.000000 0.00000 {dist*2}
H 0.000000 0.00000 {dist*3}
""",
basis="sto-3g", # 基底関数系: STO-3Gを使用
verbose=0,
)
mf_jj = AbinitioToolsClass(hydrogen)
mf_jj.run_uks()
jj = mf_jj.calc_jj(frm, to)
return jj
def test_jj():
dist = 1
frm = 1
to = 2
jj_1 = run_example(dist, frm, to)
dist = 2
frm = 1
to = 2
jj_2 = run_example(dist, frm, to)
dist = 3
frm = 1
to = 2
jj_3 = run_example(dist, frm, to)
assert jj_1 > jj_2
assert jj_2 > jj_3
print("test_jj1:", jj_1, jj_2, jj_3)
dist = 1
frm = 0
to = 3
jj_4 = run_example(dist, frm, to)
dist = 1
frm = 1
to = 2
jj_5 = run_example(dist, frm, to)
assert jj_5 > jj_4
print("test_jj2:", jj_4, jj_5)
# dist = 1
# E = 1
# frm = 0
# to = 2
# jj_6 = run_example(dist, E, frm, to)
# dist = 1
# E = 2
# frm = 0
# to = 2
# jj_7 = run_example(dist, E, frm, to)
# assert jj_7 > jj_6
# print("test_jj3:", jj_6, jj_7)
return
def test_util():
dist = 0.75
hydrogen = gto.M(
atom=f"""
H 0.000000 0.00000 0.000000
H 0.000000 0.00000 {dist}
H 0.000000 0.00000 {dist*2}
H 0.000000 0.00000 {dist*3}
""",
basis="sto-3g", # 基底関数系: STO-3Gを使用
verbose=0,
)
mf_jj = AbinitioToolsClass(hydrogen)
mf_jj.run_uks()
nao = len(hydrogen.ao_labels())
jj_all = np.zeros((nao, nao))
for i in range(nao):
for j in range(nao):
if i != j:
jj_all[i, j] = mf_jj.calc_jj(i, j)
heatmap_ao(mf_jj.mf, jj_all, path="heatmap_ao_jj.png")
return
def test_green():
dist = 0.75
hydrogen = gto.M(
atom=f"""
H 0.000000 0.00000 0.000000
H 0.000000 0.00000 {dist}
H 0.000000 0.00000 {dist*2}
H 0.000000 0.00000 {dist*3}
""",
basis="sto-3g", # 基底関数系: STO-3Gを使用
verbose=0,
)
mf_jj = AbinitioToolsClass(hydrogen)
mf_jj.run_rks()
moe = mf_jj.mf.mo_energy
omega = np.linspace(-2, 2, 400)
green = mf_jj.calc_green(omega_list=omega)
dos = np.trace(green, axis1=0, axis2=1).imag
plt.cla()
plt.plot(omega, dos)
for a in moe:
plt.axvline(x=a, color="r")
plt.savefig("./green.png")
return
def test_exciton():
dist = 0.75
hydrogen = gto.M(
atom=f"""
H 0.000000 0.00000 0.000000
Li 0.000000 0.00000 {dist}
""",
basis="sto-3g", # 基底関数系: STO-3Gを使用
verbose=0,
)
mf_jj = AbinitioToolsClass(hydrogen)
mf_jj.run_rks()
mf_jj.run_tddft()
mf_jj.calc_exciton_corr()
return