def test_eq_substitute():
H_0 = OperatorSymbol('H_0', hs=0)
ω, E0 = sympy.symbols('omega, E_0')
eq0 = Eq(H_0, ω * Create(hs=0) * Destroy(hs=0) + E0, tag='0')
eq1 = eq0.apply('substitute', {E0: 0}).reset()
eq2 = Eq(H_0, ω * Create(hs=0) * Destroy(hs=0))
assert eq1 == eq2
def test_indexed_hs_not_disjoint():
i, j = symbols('i, j', cls=IdxSym)
hs_i = LocalSpace(StrLabel(i))
hs_j = LocalSpace(StrLabel(j))
assert not hs_i.isdisjoint(hs_i)
assert not hs_i.isdisjoint(hs_j)
expr = Create(hs=hs_j) * Destroy(hs=hs_i)
assert expr.args == (Create(hs=hs_j), Destroy(hs=hs_i))
def test_eq_sub_const():
H_0 = OperatorSymbol('H_0', hs=0)
ω, E0 = sympy.symbols('omega, E_0')
eq0 = Eq(H_0, ω * Create(hs=0) * Destroy(hs=0) + E0, tag='0')
eq = eq0 - E0
assert eq.lhs == H_0 - E0
assert eq.rhs == ω * Create(hs=0) * Destroy(hs=0)
assert eq._tag is None
def test_ascii_operator_elements():
"""Test the ascii representation of "atomic" operator algebra elements"""
hs1 = LocalSpace('q1', dimension=2)
hs2 = LocalSpace('q2', dimension=2)
alpha, beta = symbols('alpha, beta')
assert ascii(OperatorSymbol("A", hs=hs1)) == 'A^(q1)'
A_1 = OperatorSymbol("A_1", hs=1)
assert ascii(A_1, show_hs_label='subscript') == 'A_1,(1)'
assert ascii(OperatorSymbol("A", hs=hs1), show_hs_label=False) == 'A'
assert ascii(OperatorSymbol("A_1", hs=hs1 * hs2)) == 'A_1^(q1*q2)'
assert ascii(OperatorSymbol("Xi_2", hs=('q1', 'q2'))) == 'Xi_2^(q1*q2)'
assert ascii(OperatorSymbol("Xi_full", hs=1)) == 'Xi_full^(1)'
assert ascii(OperatorSymbol("Xi", alpha, beta,
hs=1)) == ('Xi^(1)(alpha, beta)')
with pytest.raises(ValueError):
OperatorSymbol(r'\Xi^2', hs='a')
assert ascii(IdentityOperator) == "1"
assert ascii(ZeroOperator) == "0"
assert ascii(Create(hs=1)) == "a^(1)H"
assert ascii(Create(hs=1), show_hs_label=False) == "a^H"
assert ascii(Create(hs=1), show_hs_label='subscript') == "a_(1)^H"
assert ascii(Destroy(hs=1)) == "a^(1)"
fock1 = LocalSpace(1,
local_identifiers={
'Create': 'b',
'Destroy': 'b',
'Phase': 'Ph'
})
spin1 = SpinSpace(1,
spin=1,
local_identifiers={
'Jz': 'Z',
'Jplus': 'Jp',
'Jminus': 'Jm'
})
assert ascii(Create(hs=fock1)) == "b^(1)H"
assert ascii(Destroy(hs=fock1)) == "b^(1)"
assert ascii(Jz(hs=SpinSpace(1, spin=1))) == "J_z^(1)"
assert ascii(Jz(hs=spin1)) == "Z^(1)"
assert ascii(Jplus(hs=spin1)) == "Jp^(1)"
assert ascii(Jminus(hs=spin1)) == "Jm^(1)"
assert ascii(Phase(0.5, hs=1)) == 'Phase^(1)(0.5)'
assert ascii(Phase(0.5, hs=fock1)) == 'Ph^(1)(0.5)'
assert ascii(Displace(0.5, hs=1)) == 'D^(1)(0.5)'
assert ascii(Squeeze(0.5, hs=1)) == 'Squeeze^(1)(0.5)'
hs_tls = LocalSpace('1', basis=('g', 'e'))
sig_e_g = LocalSigma('e', 'g', hs=hs_tls)
assert ascii(sig_e_g) == '|e><g|^(1)'
assert ascii(sig_e_g, sig_as_ketbra=False) == 'sigma_e,g^(1)'
sig_e_e = LocalProjector('e', hs=hs_tls)
assert ascii(sig_e_e, sig_as_ketbra=False) == 'Pi_e^(1)'
assert (ascii(BasisKet(0, hs=1) * BasisKet(0, hs=2) *
BasisKet(0, hs=3)) == '|0,0,0>^(1*2*3)')
assert ascii(BasisKet(0, hs=hs1) * BasisKet(0, hs=hs2)) == '|00>^(q1*q2)'
assert (ascii(
BasisKet(0, hs=LocalSpace(0, dimension=20)) *
BasisKet(0, hs=LocalSpace(1, dimension=20))) == '|0,0>^(0*1)')
def test_apply_mtd():
H_0 = OperatorSymbol('H_0', hs=0)
H = OperatorSymbol('H', hs=0)
ω, E0 = sympy.symbols('omega, E_0')
eq0 = Eq(H_0, ω * Create(hs=0) * Destroy(hs=0) + E0, tag='0')
eq = eq0.apply('substitute', {H_0: H, E0: 0}).tag('new')
assert eq.lhs == H
assert eq.rhs == ω * Create(hs=0) * Destroy(hs=0)
assert eq._tag == 'new'
def test_eq_sub_eq():
ω, E0 = sympy.symbols('omega, E_0')
H_0 = OperatorSymbol('H_0', hs=0)
H_1 = OperatorSymbol('H_1', hs=0)
mu = OperatorSymbol('mu', hs=0)
eq0 = Eq(H_0, ω * Create(hs=0) * Destroy(hs=0) + E0, tag='0')
eq1 = Eq(H_1, mu + E0, tag='1')
eq = eq0 - eq1
assert eq.lhs == H_0 - H_1
assert eq.rhs == ω * Create(hs=0) * Destroy(hs=0) - mu
assert eq._tag is None
def operator_exprs():
"""Prepare a list of operator algebra expressions"""
hs1 = LocalSpace('q1', dimension=2)
hs2 = LocalSpace('q2', dimension=2)
A = OperatorSymbol("A", hs=hs1)
B = OperatorSymbol("B", hs=hs1)
C = OperatorSymbol("C", hs=hs2)
a, b = symbols('a, b')
A_ab = OperatorSymbol("A", a, b, hs=0)
gamma = symbols('gamma')
return [
OperatorSymbol("A", hs=hs1),
OperatorSymbol("A_1", hs=hs1 * hs2),
OperatorSymbol("A_1", symbols('alpha'), symbols('beta'), hs=hs1 * hs2),
A_ab.diff(a, n=2).diff(b),
A_ab.diff(a, n=2).diff(b).evaluate_at({a: 0}),
OperatorSymbol("Xi_2", hs=(r'q1', 'q2')),
OperatorSymbol("Xi_full", hs=1),
IdentityOperator,
ZeroOperator,
Create(hs=1),
Create(hs=LocalSpace(1, local_identifiers={'Create': 'b'})),
Destroy(hs=1),
Destroy(hs=LocalSpace(1, local_identifiers={'Destroy': 'b'})),
Jz(hs=SpinSpace(1, spin=1)),
Jz(hs=SpinSpace(1, spin=1, local_identifiers={'Jz': 'Z'})),
Jplus(hs=SpinSpace(1, spin=1, local_identifiers={'Jplus': 'Jp'})),
Jminus(hs=SpinSpace(1, spin=1, local_identifiers={'Jminus': 'Jm'})),
Phase(0.5, hs=1),
Phase(0.5, hs=LocalSpace(1, local_identifiers={'PhaseCC': 'Ph'})),
Displace(0.5, hs=1),
Squeeze(0.5, hs=1),
LocalSigma('e', 'g', hs=LocalSpace(1, basis=('g', 'e'))),
LocalSigma('e', 'e', hs=LocalSpace(1, basis=('g', 'e'))),
A + B,
A * B,
A * C,
2 * A,
2j * A,
(1 + 2j) * A,
gamma**2 * A,
-(gamma**2) / 2 * A,
tr(A * C, over_space=hs2),
Adjoint(A),
Adjoint(A + B),
PseudoInverse(A),
NullSpaceProjector(A),
A - B,
2 * A - sqrt(gamma) * (B + C),
Commutator(A, B),
]
def test_ascii_equation():
"""Test printing of the Eq class"""
eq_1 = Eq(lhs=OperatorSymbol('H', hs=0), rhs=Create(hs=0) * Destroy(hs=0))
# fmt: off
eq = (eq_1.apply_to_lhs(lambda expr: expr + 1).apply_to_rhs(
lambda expr: expr + 1).apply_to_rhs(lambda expr: expr**2).tag(
3).transform(lambda eq: eq + 1).tag(4).apply_to_rhs('expand').
apply_to_lhs(lambda expr: expr**2).tag(5).apply(
'expand').apply_to_lhs(lambda expr: expr**2).tag(6).apply_to_lhs(
'expand').apply_to_rhs(lambda expr: expr + 1))
# fmt: on
assert ascii(eq_1) == 'H^(0) = a^(0)H * a^(0)'
assert ascii(eq_1.tag(1).reset()) == 'H^(0) = a^(0)H * a^(0) (1)'
assert ascii(eq, show_hs_label=False).strip() == (r'''
H = a^H * a
1 + H = a^H * a
= 1 + a^H * a
= (1 + a^H * a) * (1 + a^H * a) (3)
2 + H = 1 + (1 + a^H * a) * (1 + a^H * a) (4)
= 2 + a^H * a^H * a * a + 3 * a^H * a
(2 + H) * (2 + H) = 2 + a^H * a^H * a * a + 3 * a^H * a (5)
4 + 4 * H + H * H = 2 + a^H * a^H * a * a + 3 * a^H * a
(4 + 4 * H + H * H) * (4 + 4 * H + H * H) = 2 + a^H * a^H * a * a + 3 * a^H * a (6)
16 + 32 * H + H * H * H * H + 8 * H * H * H + 24 * H * H = 2 + a^H * a^H * a * a + 3 * a^H * a
= 3 + a^H * a^H * a * a + 3 * a^H * a
'''.strip())
def test_unicode_equation():
"""Test printing of the Eq class"""
eq_1 = Eq(lhs=OperatorSymbol('H', hs=0), rhs=Create(hs=0) * Destroy(hs=0))
# fmt: off
eq = (eq_1.apply_to_lhs(lambda expr: expr + 1).apply_to_rhs(
lambda expr: expr + 1).apply_to_rhs(lambda expr: expr**2).tag(
3).transform(lambda eq: eq + 1).tag(4).apply_to_rhs('expand').
apply_to_lhs(lambda expr: expr**2).tag(5).apply(
'expand').apply_to_lhs(lambda expr: expr**2).tag(6).apply_to_lhs(
'expand').apply_to_rhs(lambda expr: expr + 1))
# fmt: on
assert unicode(eq_1) == 'Ĥ⁽⁰⁾ = â^(0)† â⁽⁰⁾'
assert unicode(eq_1.tag(1)) == 'Ĥ⁽⁰⁾ = â^(0)† â⁽⁰⁾ (1)'
unicode_lines = unicode(eq, show_hs_label=False).split("\n")
expected = [
' Ĥ = â^† â',
' 𝟙 + Ĥ = â^† â',
' = 𝟙 + â^† â',
' = (𝟙 + â^† â) (𝟙 + â^† â) (3)',
' 2 + Ĥ = 𝟙 + (𝟙 + â^† â) (𝟙 + â^† â) (4)',
' = 2 + â^† â^† â â + 3 â^† â',
' (2 + Ĥ) (2 + Ĥ) = 2 + â^† â^† â â + 3 â^† â (5)',
' 4 + 4 Ĥ + Ĥ Ĥ = 2 + â^† â^† â â + 3 â^† â',
' (4 + 4 Ĥ + Ĥ Ĥ) (4 + 4 Ĥ + Ĥ Ĥ) = 2 + â^† â^† â â + 3 â^† â (6)',
'16 + 32 Ĥ + Ĥ Ĥ Ĥ Ĥ + 8 Ĥ Ĥ Ĥ + 24 Ĥ Ĥ = 2 + â^† â^† â â + 3 â^† â',
' = 3 + â^† â^† â â + 3 â^† â',
]
for i, line in enumerate(unicode_lines):
assert line == expected[i]
eq = Eq(OperatorSymbol('H', hs=0), 0, eq_sym_str='→')
assert unicode(eq, show_hs_label=False) == 'Ĥ → 0'
def test_eq_copy():
H_0 = OperatorSymbol('H_0', hs=0)
ω, E0 = sympy.symbols('omega, E_0')
eq0 = Eq(H_0, ω * Create(hs=0) * Destroy(hs=0) + E0, tag='0')
eq = eq0.copy()
assert eq == eq0
assert eq is not eq0
def test_repr_latex():
H_0 = OperatorSymbol('H_0', hs=0)
ω, E0 = sympy.symbols('omega, E_0')
Eq.latex_renderer = staticmethod(latex)
eq0 = Eq(H_0, ω * Create(hs=0) * Destroy(hs=0) + E0, tag='0')
repr1 = eq0._repr_latex_()
repr2 = latex(eq0)
assert repr1 == repr2
def test_apply_to_lhs():
H_0 = OperatorSymbol('H_0', hs=0)
ω, E0 = sympy.symbols('omega, E_0')
eq0 = Eq(H_0, ω * Create(hs=0) * Destroy(hs=0) + E0, tag='0')
eq = eq0.apply_to_lhs(lambda expr: expr + E0).tag('new')
assert eq.lhs == H_0 + E0
assert eq.rhs == eq0.rhs
assert eq._tag == 'new'
def test_eq_mult_const():
H_0 = OperatorSymbol('H_0', hs=0)
ω, E0 = sympy.symbols('omega, E_0')
eq0 = Eq(H_0, ω * Create(hs=0) * Destroy(hs=0) + E0, tag='0')
eq = 2 * eq0
assert eq == eq0 * 2
assert eq.lhs == 2 * eq0.lhs
assert eq.rhs == 2 * eq0.rhs
assert eq._tag is None
def test_create_on_fock_expansion():
"""Test ``Create * sum_i alpha_i |i> = sqrt(i+1) * alpha_i * |i+1>``"""
i = IdxSym('i')
alpha = IndexedBase('alpha')
hs = LocalSpace('0', dimension=3)
expr = Create(hs=hs) * KetIndexedSum(
alpha[i] * BasisKet(FockIndex(i), hs=hs),
ranges=IndexOverFockSpace(i, hs),
)
assert expr == KetIndexedSum(
sympy.sqrt(i + 1) * alpha[i] * BasisKet(FockIndex(i + 1), hs=hs),
ranges=IndexOverFockSpace(i, hs),
)
assert expr.doit() == (alpha[0] * BasisKet(1, hs=hs) +
sympy.sqrt(2) * alpha[1] * BasisKet(2, hs=hs))
def test_quantum_symbols_with_indexedhs():
"""Test the free_symbols method for objects that have a Hilbert space with a
sybmolic label, for the example of an OperatorSymbol"""
i, j = symbols('i, j', cls=IdxSym)
hs_i = LocalSpace(StrLabel(i))
hs_j = LocalSpace(StrLabel(j))
A = OperatorSymbol("A", hs=hs_i * hs_j)
assert A.free_symbols == {i, j}
expr = Create(hs=hs_i) * Destroy(hs=hs_i)
assert expr.free_symbols == {
i,
}
def test_unchanged_apply():
H_0 = OperatorSymbol('H_0', hs=0)
ω, E0 = sympy.symbols('omega, E_0')
eq0 = Eq(H_0, ω * Create(hs=0) * Destroy(hs=0) + E0, tag='0')
assert eq0.apply(lambda s: s.expand()).reset() == eq0
assert eq0.apply(lambda s: s.expand()) == eq0
assert eq0.apply(lambda s: s.expand())._lhs is None
assert eq0.apply('expand').reset() == eq0
assert eq0.apply('expand') == eq0
assert eq0.apply('expand')._lhs is None
def test_unicode_operator_operations():
"""Test the unicode representation of operator algebra operations"""
hs1 = LocalSpace('q_1', dimension=2)
hs2 = LocalSpace('q_2', dimension=2)
A = OperatorSymbol("A", hs=hs1)
B = OperatorSymbol("B", hs=hs1)
C = OperatorSymbol("C", hs=hs2)
psi = KetSymbol('Psi', hs=hs1)
gamma = symbols('gamma', positive=True)
assert unicode(A + B) == 'A\u0302^(q\u2081) + B\u0302^(q\u2081)'
# Â^(q₁) + B̂^(q₁)
assert unicode(A * B) == 'A\u0302^(q\u2081) B\u0302^(q\u2081)'
# Â^(q₁) B̂^(q₁)
assert unicode(A * C) == 'A\u0302^(q\u2081) C\u0302^(q\u2082)'
# Â^(q₁) Ĉ^(q₂)
assert unicode(2 * A) == '2 A\u0302^(q\u2081)' # 2 Â^(q₁)
assert unicode(2j * A) == '2j A\u0302^(q\u2081)'
# 2j Â^(q₁)
assert unicode((1 + 2j) * A) == '(1+2j) A\u0302^(q\u2081)'
# (1+2j) Â^(q₁)
assert unicode(gamma**2 * A) == '\u03b3\xb2 A\u0302^(q\u2081)'
# γ² Â^(q₁)
assert unicode(-(gamma**2) / 2 * A) == '-\u03b3\xb2/2 A\u0302^(q\u2081)'
# -γ²/2 Â^(q₁)
assert (unicode(tr(
A * C,
over_space=hs2)) == 'tr_(q\u2082)[C\u0302^(q\u2082)] A\u0302^(q\u2081)'
)
# tr_(q₂)[Ĉ^(q₂)] Â^(q₁)
assert unicode(Adjoint(A)) == 'A\u0302^(q\u2081)\u2020'
# Â^(q₁)†
assert unicode(Adjoint(Create(hs=1))) == 'a\u0302\u207d\xb9\u207e'
# â⁽¹⁾
assert unicode(PseudoInverse(A)) == '(A\u0302^(q\u2081))^+'
# (Â^(q₁))^+
assert unicode(NullSpaceProjector(A)) == 'P\u0302_Ker(A\u0302^(q\u2081))'
# P̂_Ker(Â^(q₁))
assert unicode(A - B) == 'A\u0302^(q\u2081) - B\u0302^(q\u2081)'
# Â^(q₁) - B̂^(q₁)
assert unicode(2 * A - sqrt(gamma) * (B + C)) in [
'2 A\u0302^(q\u2081) - \u221a\u03b3 (B\u0302^(q\u2081) '
'+ C\u0302^(q\u2082))',
'2 A\u0302^(q\u2081) - sqrt(\u03b3) (B\u0302^(q\u2081) '
'+ C\u0302^(q\u2082))',
]
# 2 Â^(q₁) - √γ (B̂^(q₁) + Ĉ^(q₂))
assert (unicode(Commutator(A,
B)) == '[A\u0302^(q\u2081), B\u0302^(q\u2081)]')
# [Â^(q₁), B̂^(q₁)]
expr = (Commutator(A, B) * psi).dag()
assert unicode(expr, show_hs_label=False) == r'⟨Ψ| [Â, B̂]^†'
def test_tex_operator_operations():
"""Test the tex representation of operator algebra operations"""
hs1 = LocalSpace('q_1', dimension=2)
hs2 = LocalSpace('q_2', dimension=2)
A = OperatorSymbol("A", hs=hs1)
B = OperatorSymbol("B", hs=hs1)
C = OperatorSymbol("C", hs=hs2)
psi = KetSymbol('Psi', hs=hs1)
gamma = symbols('gamma', positive=True)
assert latex(A.dag()) == r'\hat{A}^{(q_{1})\dagger}'
assert latex(A + B) == r'\hat{A}^{(q_{1})} + \hat{B}^{(q_{1})}'
assert latex(A * B) == r'\hat{A}^{(q_{1})} \hat{B}^{(q_{1})}'
assert latex(A * C) == r'\hat{A}^{(q_{1})} \hat{C}^{(q_{2})}'
assert latex(2 * A) == r'2 \hat{A}^{(q_{1})}'
assert latex(2j * A) == r'2i \hat{A}^{(q_{1})}'
assert latex((1 + 2j) * A) == r'(1+2i) \hat{A}^{(q_{1})}'
assert latex(gamma**2 * A) == r'\gamma^{2} \hat{A}^{(q_{1})}'
assert (latex(-(gamma**2) / 2 *
A) == r'- \frac{\gamma^{2}}{2} \hat{A}^{(q_{1})}')
assert (latex(tr(
A * C,
over_space=hs2)) == r'{\rm tr}_{q_{2}}\left[\hat{C}^{(q_{2})}\right] '
r'\hat{A}^{(q_{1})}')
assert latex(Adjoint(A)) == r'\hat{A}^{(q_{1})\dagger}'
assert (latex(Adjoint(
A**2)) == r'\left(\hat{A}^{(q_{1})} \hat{A}^{(q_{1})}\right)^\dagger')
assert (latex(
Adjoint(A)**2) == r'\hat{A}^{(q_{1})\dagger} \hat{A}^{(q_{1})\dagger}')
assert latex(Adjoint(Create(hs=1))) == r'\hat{a}^{(1)}'
assert (latex(Adjoint(A + B)) ==
r'\left(\hat{A}^{(q_{1})} + \hat{B}^{(q_{1})}\right)^\dagger')
assert latex(PseudoInverse(A)) == r'\left(\hat{A}^{(q_{1})}\right)^+'
assert (latex(
PseudoInverse(A)**2
) == r'\left(\hat{A}^{(q_{1})}\right)^+ \left(\hat{A}^{(q_{1})}\right)^+')
assert (latex(NullSpaceProjector(A)) ==
r'\hat{P}_{Ker}\left(\hat{A}^{(q_{1})}\right)')
assert latex(A - B) == r'\hat{A}^{(q_{1})} - \hat{B}^{(q_{1})}'
assert (latex(A - B + C) ==
r'\hat{A}^{(q_{1})} - \hat{B}^{(q_{1})} + \hat{C}^{(q_{2})}')
assert (latex(2 * A - sqrt(gamma) * (B + C)) ==
r'2 \hat{A}^{(q_{1})} - \sqrt{\gamma} \left(\hat{B}^{(q_{1})} + '
r'\hat{C}^{(q_{2})}\right)')
assert (latex(Commutator(
A, B)) == r'\left[\hat{A}^{(q_{1})}, \hat{B}^{(q_{1})}\right]')
expr = (Commutator(A, B) * psi).dag()
assert (latex(expr, show_hs_label=False) ==
r'\left\langle \Psi \right\rvert \left[\hat{A}, '
r'\hat{B}\right]^{\dagger}')
def test_unicode_operator_elements():
"""Test the unicode representation of "atomic" operator algebra elements"""
hs1 = LocalSpace('q1', dimension=2)
hs2 = LocalSpace('q2', dimension=2)
alpha, beta = symbols('alpha, beta')
assert unicode(OperatorSymbol("A", hs=hs1)) == 'A\u0302^(q\u2081)'
# Â^(q₁)
assert (unicode(OperatorSymbol('A', hs=1),
show_hs_label='subscript') == 'A\u0302\u208d\u2081\u208e'
) # Â₍₁₎
assert (unicode(
OperatorSymbol("A", hs=hs1),
unicode_op_hats=False,
unicode_sub_super=False,
) == 'A^(q_1)')
assert (unicode(OperatorSymbol(
"A_1",
hs=hs1 * hs2)) == 'A\u0302_1^(q\u2081\u2297q\u2082)') # Â_1^(q₁⊗q₂)
assert (unicode(OperatorSymbol(
"Xi_2", hs=('q1', 'q2'))) == '\u039e\u0302_2^(q\u2081\u2297q\u2082)'
) # Ξ̂_2^(q₁⊗q₂)
assert unicode(OperatorSymbol("Xi", alpha, beta, hs=1)) == ('Ξ̂⁽¹⁾(α, β)')
assert unicode(IdentityOperator) == "𝟙"
assert unicode(ZeroOperator) == "0"
assert unicode(Create(hs=1)) == 'a\u0302^(1)\u2020' # â^(1)†
assert unicode(Destroy(hs=1)) == 'a\u0302\u207d\xb9\u207e' # â⁽¹⁾
assert unicode(Destroy(hs=1), unicode_sub_super=False) == 'a\u0302^(1)'
assert unicode(Destroy(hs=1), unicode_op_hats=False) == 'a\u207d\xb9\u207e'
assert (unicode(Destroy(hs=1),
unicode_op_hats=False,
unicode_sub_super=False) == 'a^(1)')
assert (unicode(Squeeze(Rational(1, 2),
hs=1)) == 'Squeeze\u207d\xb9\u207e(1/2)')
# Squeeze⁽¹⁾(1/2)
hs_tls = LocalSpace('1', basis=('g', 'e'))
sig_e_g = LocalSigma('e', 'g', hs=hs_tls)
assert unicode(sig_e_g) == '|e⟩⟨g|⁽¹⁾'
assert unicode(sig_e_g, unicode_sub_super=False) == '|e⟩⟨g|^(1)'
assert unicode(sig_e_g, show_hs_label=False) == '|e⟩⟨g|'
assert (unicode(sig_e_g, sig_as_ketbra=False) == '\u03c3\u0302_e,g^(1)'
) # σ̂_e,g^(1)
sig_e_e = LocalProjector('e', hs=hs_tls)
assert unicode(sig_e_e) == '|e⟩⟨e|⁽¹⁾'
assert (unicode(
sig_e_e,
sig_as_ketbra=False) == '\u03a0\u0302\u2091\u207d\xb9\u207e') # Π̂ₑ⁽¹⁾
assert (unicode(BasisKet(0, hs=1) * BasisKet(0, hs=2) *
BasisKet(0, hs=3)) == '|0,0,0⟩^(1⊗2⊗3)')
assert unicode(BasisKet(0, hs=hs1) * BasisKet(0, hs=hs2)) == '|00⟩^(q₁⊗q₂)'
def test_ascii_operator_operations():
"""Test the ascii representation of operator algebra operations"""
hs1 = LocalSpace('q_1', dimension=2)
hs2 = LocalSpace('q_2', dimension=2)
A = OperatorSymbol("A", hs=hs1)
B = OperatorSymbol("B", hs=hs1)
C = OperatorSymbol("C", hs=hs2)
D = OperatorSymbol("D", hs=hs1)
psi = KetSymbol('Psi', hs=hs1)
gamma = symbols('gamma', positive=True)
assert ascii(A + B) == 'A^(q_1) + B^(q_1)'
assert ascii(A * B) == 'A^(q_1) * B^(q_1)'
assert ascii(A * C) == 'A^(q_1) * C^(q_2)'
assert ascii(A * (B + D)) == 'A^(q_1) * (B^(q_1) + D^(q_1))'
assert ascii(A * (B - D)) == 'A^(q_1) * (B^(q_1) - D^(q_1))'
assert (ascii(
(A + B) *
(-2 * B - D)) == '(A^(q_1) + B^(q_1)) * (-D^(q_1) - 2 * B^(q_1))')
assert ascii(OperatorTimes(A, -B)) == 'A^(q_1) * (-B^(q_1))'
assert ascii(OperatorTimes(A, -B), show_hs_label=False) == 'A * (-B)'
assert ascii(2 * A) == '2 * A^(q_1)'
assert ascii(2j * A) == '2j * A^(q_1)'
assert ascii((1 + 2j) * A) == '(1+2j) * A^(q_1)'
assert ascii(gamma**2 * A) == 'gamma**2 * A^(q_1)'
assert ascii(-(gamma**2) / 2 * A) == '-gamma**2/2 * A^(q_1)'
assert ascii(tr(A * C, over_space=hs2)) == 'tr_(q_2)[C^(q_2)] * A^(q_1)'
expr = A + OperatorPlusMinusCC(B * D)
assert ascii(expr, show_hs_label=False) == 'A + (B * D + c.c.)'
expr = A + OperatorPlusMinusCC(B + D)
assert ascii(expr, show_hs_label=False) == 'A + (B + D + c.c.)'
expr = A * OperatorPlusMinusCC(B * D)
assert ascii(expr, show_hs_label=False) == 'A * (B * D + c.c.)'
assert ascii(Adjoint(A)) == 'A^(q_1)H'
assert ascii(Adjoint(Create(hs=1))) == 'a^(1)'
assert ascii(Adjoint(A + B)) == '(A^(q_1) + B^(q_1))^H'
assert ascii(PseudoInverse(A)) == '(A^(q_1))^+'
assert ascii(NullSpaceProjector(A)) == 'P_Ker(A^(q_1))'
assert ascii(A - B) == 'A^(q_1) - B^(q_1)'
assert ascii(A - B + C) == 'A^(q_1) - B^(q_1) + C^(q_2)'
expr = 2 * A - sqrt(gamma) * (B + C)
assert ascii(expr) == '2 * A^(q_1) - sqrt(gamma) * (B^(q_1) + C^(q_2))'
assert ascii(Commutator(A, B)) == r'[A^(q_1), B^(q_1)]'
expr = (Commutator(A, B) * psi).dag()
assert ascii(expr, show_hs_label=False) == r'<Psi| [A, B]^H'
def test_tex_equation():
"""Test printing of the Eq class"""
eq_1 = Eq(lhs=OperatorSymbol('H', hs=0), rhs=Create(hs=0) * Destroy(hs=0))
# fmt: off
eq = (eq_1.apply_to_lhs(lambda expr: expr + 1).apply_to_rhs(
lambda expr: expr + 1).apply_to_rhs(lambda expr: expr**2).tag(
3).transform(lambda eq: eq + 1).tag(4).apply_to_rhs('expand').
apply_to_lhs(lambda expr: expr**2).tag(5).apply(
'expand').apply_to_lhs(lambda expr: expr**2).tag(6).apply_to_lhs(
'expand').apply_to_rhs(lambda expr: expr + 1))
# fmt: on
assert latex(eq_1).split("\n") == [
r'\begin{equation}',
r' \hat{H}^{(0)} = \hat{a}^{(0)\dagger} \hat{a}^{(0)}',
r'\end{equation}',
'',
]
assert latex(eq_1.tag(1).reset()).split("\n") == [
r'\begin{equation}',
r' \hat{H}^{(0)} = \hat{a}^{(0)\dagger} \hat{a}^{(0)}',
r'\tag{1}\end{equation}',
'',
]
tex_lines = latex(eq, show_hs_label=False,
tex_op_macro=r'\Op{{{name}}}').split("\n")
expected = [
r'\begin{align}',
r' \Op{H} &= \Op{a}^{\dagger} \Op{a}\\',
r' \mathbb{1} + \Op{H} &= \Op{a}^{\dagger} \Op{a}\\',
r' &= \mathbb{1} + \Op{a}^{\dagger} \Op{a}\\',
r' &= \left(\mathbb{1} + \Op{a}^{\dagger} \Op{a}\right) \left(\mathbb{1} + \Op{a}^{\dagger} \Op{a}\right)\tag{3}\\',
r' 2 + \Op{H} &= \mathbb{1} + \left(\mathbb{1} + \Op{a}^{\dagger} \Op{a}\right) \left(\mathbb{1} + \Op{a}^{\dagger} \Op{a}\right)\tag{4}\\',
r' &= 2 + \Op{a}^{\dagger} \Op{a}^{\dagger} \Op{a} \Op{a} + 3 \Op{a}^{\dagger} \Op{a}\\',
r' \left(2 + \Op{H}\right) \left(2 + \Op{H}\right) &= 2 + \Op{a}^{\dagger} \Op{a}^{\dagger} \Op{a} \Op{a} + 3 \Op{a}^{\dagger} \Op{a}\tag{5}\\',
r' 4 + 4 \Op{H} + \Op{H} \Op{H} &= 2 + \Op{a}^{\dagger} \Op{a}^{\dagger} \Op{a} \Op{a} + 3 \Op{a}^{\dagger} \Op{a}\\',
r' \left(4 + 4 \Op{H} + \Op{H} \Op{H}\right) \left(4 + 4 \Op{H} + \Op{H} \Op{H}\right) &= 2 + \Op{a}^{\dagger} \Op{a}^{\dagger} \Op{a} \Op{a} + 3 \Op{a}^{\dagger} \Op{a}\tag{6}\\',
r' 16 + 32 \Op{H} + \Op{H} \Op{H} \Op{H} \Op{H} + 8 \Op{H} \Op{H} \Op{H} + 24 \Op{H} \Op{H} &= 2 + \Op{a}^{\dagger} \Op{a}^{\dagger} \Op{a} \Op{a} + 3 \Op{a}^{\dagger} \Op{a}\\',
r' &= 3 + \Op{a}^{\dagger} \Op{a}^{\dagger} \Op{a} \Op{a} + 3 \Op{a}^{\dagger} \Op{a}',
r'\end{align}',
r'',
]
for i, line in enumerate(tex_lines):
assert line == expected[i]
def test_eq_repr():
H_0 = OperatorSymbol('H_0', hs=0)
ω, E0 = sympy.symbols('omega, E_0')
eq0 = Eq(H_0, ω * Create(hs=0) * Destroy(hs=0) + E0, tag='0')
assert repr(eq0) == "%s = %s (0)" % (repr(eq0.lhs), repr(eq0.rhs))
def test_no_sympify():
H_0 = OperatorSymbol('H_0', hs=0)
ω, E0 = sympy.symbols('omega, E_0')
eq0 = Eq(H_0, ω * Create(hs=0) * Destroy(hs=0) + E0, tag='0')
with pytest.raises(SympifyError):
sympy.sympify(eq0)
def test_tex_operator_elements():
"""Test the tex representation of "atomic" operator algebra elements"""
hs1 = LocalSpace('q1', dimension=2)
hs2 = LocalSpace('q2', dimension=2)
alpha, beta = symbols('alpha, beta')
fock1 = LocalSpace(1,
local_identifiers={
'Create': 'b',
'Destroy': 'b',
'Phase': 'Phi'
})
spin1 = SpinSpace(1,
spin=1,
local_identifiers={
'Jz': 'Z',
'Jplus': 'Jp',
'Jminus': 'Jm'
})
assert latex(OperatorSymbol("A", hs=hs1)) == r'\hat{A}^{(q_{1})}'
assert (latex(OperatorSymbol(
"A_1", hs=hs1 * hs2)) == r'\hat{A}_{1}^{(q_{1} \otimes q_{2})}')
assert (latex(OperatorSymbol(
"Xi_2", hs=(r'q1', 'q2'))) == r'\hat{\Xi}_{2}^{(q_{1} \otimes q_{2})}')
assert (latex(OperatorSymbol("Xi_full",
hs=1)) == r'\hat{\Xi}_{\text{full}}^{(1)}')
assert latex(
OperatorSymbol("Xi", alpha, beta,
hs=1)) == (r'\hat{\Xi}^{(1)}\left(\alpha, \beta\right)')
assert latex(IdentityOperator) == r'\mathbb{1}'
assert latex(IdentityOperator, tex_identity_sym='I') == 'I'
assert latex(ZeroOperator) == r'\mathbb{0}'
assert latex(Create(hs=1)) == r'\hat{a}^{(1)\dagger}'
assert latex(Create(hs=fock1)) == r'\hat{b}^{(1)\dagger}'
assert latex(Destroy(hs=1)) == r'\hat{a}^{(1)}'
assert latex(Destroy(hs=fock1)) == r'\hat{b}^{(1)}'
assert latex(Jz(hs=SpinSpace(1, spin=1))) == r'\hat{J}_{z}^{(1)}'
assert latex(Jz(hs=spin1)) == r'\hat{Z}^{(1)}'
assert latex(Jplus(hs=SpinSpace(1, spin=1))) == r'\hat{J}_{+}^{(1)}'
assert latex(Jplus(hs=spin1)) == r'\text{Jp}^{(1)}'
assert latex(Jminus(hs=SpinSpace(1, spin=1))) == r'\hat{J}_{-}^{(1)}'
assert latex(Jminus(hs=spin1)) == r'\text{Jm}^{(1)}'
assert (latex(Phase(Rational(
1, 2), hs=1)) == r'\text{Phase}^{(1)}\left(\frac{1}{2}\right)')
assert latex(Phase(0.5, hs=1)) == r'\text{Phase}^{(1)}\left(0.5\right)'
assert latex(Phase(0.5, hs=fock1)) == r'\hat{\Phi}^{(1)}\left(0.5\right)'
assert latex(Displace(0.5, hs=1)) == r'\hat{D}^{(1)}\left(0.5\right)'
assert latex(Squeeze(0.5, hs=1)) == r'\text{Squeeze}^{(1)}\left(0.5\right)'
hs_tls = LocalSpace('1', basis=('g', 'e'))
sig_e_g = LocalSigma('e', 'g', hs=hs_tls)
assert latex(sig_e_g, sig_as_ketbra=False) == r'\hat{\sigma}_{e,g}^{(1)}'
assert (
latex(sig_e_g) ==
r'\left\lvert e \middle\rangle\!\middle\langle g \right\rvert^{(1)}')
hs_tls = LocalSpace('1', basis=('excited', 'ground'))
sig_excited_ground = LocalSigma('excited', 'ground', hs=hs_tls)
assert (latex(sig_excited_ground, sig_as_ketbra=False) ==
r'\hat{\sigma}_{\text{excited},\text{ground}}^{(1)}')
assert (latex(sig_excited_ground) ==
r'\left\lvert \text{excited} \middle\rangle\!'
r'\middle\langle \text{ground} \right\rvert^{(1)}')
hs_tls = LocalSpace('1', basis=('mu', 'nu'))
sig_mu_nu = LocalSigma('mu', 'nu', hs=hs_tls)
assert (latex(sig_mu_nu) == r'\left\lvert \mu \middle\rangle\!'
r'\middle\langle \nu \right\rvert^{(1)}')
hs_tls = LocalSpace('1', basis=('excited', 'ground'))
sig_excited_excited = LocalProjector('excited', hs=hs_tls)
assert (latex(sig_excited_excited,
sig_as_ketbra=False) == r'\hat{\Pi}_{\text{excited}}^{(1)}')
hs_tls = LocalSpace('1', basis=('g', 'e'))
sig_e_e = LocalProjector('e', hs=hs_tls)
assert latex(sig_e_e, sig_as_ketbra=False) == r'\hat{\Pi}_{e}^{(1)}'
