def test_one_qubit_commutators():
"""Test single qubit gate commutation relations."""
for g1 in (IdentityGate, X, Y, Z, H, T, S):
for g2 in (IdentityGate, X, Y, Z, H, T, S):
e = Commutator(g1(0),g2(0))
a = matrix_to_zero(represent(e, nqubits=1, format='sympy'))
b = matrix_to_zero(represent(e.doit(), nqubits=1, format='sympy'))
assert a == b
e = Commutator(g1(0),g2(1))
assert e.doit() == 0
def test_commutator_identities():
assert Comm(a*A,b*B) == a*b*Comm(A,B)
assert Comm(A, A) == 0
assert Comm(a, b) == 0
assert Comm(A,B) == -Comm(B,A)
assert Comm(A,B).doit() == A*B - B*A
assert Comm(A,B*C).expand(commutator=True) == Comm(A,B)*C + B*Comm(A,C)
assert Comm(A*B,C).expand(commutator=True) == A*Comm(B,C) + Comm(A,C)*B
assert Comm(A+B,C).expand(commutator=True) == Comm(A,C) + Comm(B,C)
assert Comm(A,B+C).expand(commutator=True) == Comm(A,B) + Comm(A,C)
e = Comm(A,Comm(B,C))+Comm(B,Comm(C,A))+Comm(C,Comm(A,B))
assert e.doit().expand() == 0
def test_commutator():
c = Comm(A, B)
assert c.is_commutative is False
assert isinstance(c, Comm)
assert c.subs(A, C) == Comm(C, B)
# Ket
(k, Avec),
(Dagger(k), Dagger(Avec)),
# Operator
(A, Amat),
(Dagger(A), Dagger(Amat)),
# OuterProduct
(OuterProduct(k, b), Avec * Avec.H),
# TensorProduct
(TensorProduct(A, B), matrix_tensor_product(Amat, Bmat)),
# Pow
(A**2, Amat**2),
# Add/Mul
(A * B + 2 * A, Amat * Bmat + 2 * Amat),
# Commutator
(Commutator(A, B), Amat * Bmat - Bmat * Amat),
# AntiCommutator
(AntiCommutator(A, B), Amat * Bmat + Bmat * Amat),
# InnerProduct
(InnerProduct(b, k), (Avec.H * Avec)[0])
]
def test_format_sympy():
for test in _tests:
lhs = represent(test[0], basis=A, format='sympy')
rhs = to_sympy(test[1])
assert lhs == rhs
def test_scalar_sympy():
def test_big_expr():
f = Function('f')
x = symbols('x')
e1 = Dagger(
AntiCommutator(
Operator('A') + Operator('B'),
Pow(DifferentialOperator(Derivative(f(x), x), f(x)), 3)) *
TensorProduct(Jz**2,
Operator('A') + Operator('B'))) * (JzBra(1, 0) + JzBra(
1, 1)) * (JzKet(0, 0) + JzKet(1, -1))
e2 = Commutator(Jz**2,
Operator('A') + Operator('B')) * AntiCommutator(
Dagger(Operator('C') * Operator('D')),
Operator('E').inv()**2) * Dagger(Commutator(Jz, J2))
e3 = Wigner3j(1, 2, 3, 4, 5, 6) * TensorProduct(
Commutator(
Operator('A') + Dagger(Operator('B')),
Operator('C') + Operator('D')), Jz - J2) * Dagger(
OuterProduct(Dagger(JzBra(1, 1)), JzBra(
1, 0))) * TensorProduct(
JzKetCoupled(1, 1,
(1, 1)) + JzKetCoupled(1, 0, (1, 1)),
JzKetCoupled(1, -1, (1, 1)))
e4 = (ComplexSpace(1) * ComplexSpace(2) +
FockSpace()**2) * (L2(Interval(0, oo)) + HilbertSpace())
assert str(
e1
) == '(Jz**2)x(Dagger(A) + Dagger(B))*{Dagger(DifferentialOperator(Derivative(f(x), x),f(x)))**3,Dagger(A) + Dagger(B)}*(<1,0| + <1,1|)*(|0,0> + |1,-1>)'
ascii_str = \
"""\
/ 3 \\ \n\
|/ +\\ | \n\
2 / + +\\ <| /d \\ | + +> \n\
/J \\ x \\A + B /*||DifferentialOperator|--(f(x)),f(x)| | ,A + B |*(<1,0| + <1,1|)*(|0,0> + |1,-1>)\n\
\\ z/ \\\\ \dx / / / \
"""
ucode_str = \
u("""\
⎧ 3 ⎫ \n\
⎪⎛ †⎞ ⎪ \n\
2 ⎛ † †⎞ ⎨⎜ ⎛d ⎞ ⎟ † †⎬ \n\
⎛J ⎞ ⨂ ⎝A + B ⎠⋅⎪⎜DifferentialOperator⎜──(f(x)),f(x)⎟ ⎟ ,A + B ⎪⋅(⟨1,0❘ + ⟨1,1❘)⋅(❘0,0⟩ + ❘1,-1⟩)\n\
⎝ z⎠ ⎩⎝ ⎝dx ⎠ ⎠ ⎭ \
""")
assert pretty(e1) == ascii_str
assert upretty(e1) == ucode_str
assert latex(e1) == \
r'{J_z^{2}}\otimes \left({A^{\dag} + B^{\dag}}\right) \left\{\left(DifferentialOperator\left(\frac{d}{d x} f{\left (x \right )},f{\left (x \right )}\right)^{\dag}\right)^{3},A^{\dag} + B^{\dag}\right\} \left({\left\langle 1,0\right|} + {\left\langle 1,1\right|}\right) \left({\left|0,0\right\rangle } + {\left|1,-1\right\rangle }\right)'
sT(
e1,
"Mul(TensorProduct(Pow(JzOp(Symbol('J')), Integer(2)), Add(Dagger(Operator(Symbol('A'))), Dagger(Operator(Symbol('B'))))), AntiCommutator(Pow(Dagger(DifferentialOperator(Derivative(Function('f')(Symbol('x')), Symbol('x')),Function('f')(Symbol('x')))), Integer(3)),Add(Dagger(Operator(Symbol('A'))), Dagger(Operator(Symbol('B'))))), Add(JzBra(Integer(1),Integer(0)), JzBra(Integer(1),Integer(1))), Add(JzKet(Integer(0),Integer(0)), JzKet(Integer(1),Integer(-1))))"
)
assert str(e2) == '[Jz**2,A + B]*{E**(-2),Dagger(D)*Dagger(C)}*[J2,Jz]'
ascii_str = \
"""\
[ 2 ] / -2 + +\\ [ 2 ]\n\
[/J \\ ,A + B]*<E ,D *C >*[J ,J ]\n\
[\\ z/ ] \\ / [ z]\
"""
ucode_str = \
u("""\
⎡ 2 ⎤ ⎧ -2 † †⎫ ⎡ 2 ⎤\n\
⎢⎛J ⎞ ,A + B⎥⋅⎨E ,D ⋅C ⎬⋅⎢J ,J ⎥\n\
⎣⎝ z⎠ ⎦ ⎩ ⎭ ⎣ z⎦\
""")
assert pretty(e2) == ascii_str
assert upretty(e2) == ucode_str
assert latex(e2) == \
r'\left[J_z^{2},A + B\right] \left\{E^{-2},D^{\dag} C^{\dag}\right\} \left[J^2,J_z\right]'
sT(
e2,
"Mul(Commutator(Pow(JzOp(Symbol('J')), Integer(2)),Add(Operator(Symbol('A')), Operator(Symbol('B')))), AntiCommutator(Pow(Operator(Symbol('E')), Integer(-2)),Mul(Dagger(Operator(Symbol('D'))), Dagger(Operator(Symbol('C'))))), Commutator(J2Op(Symbol('J')),JzOp(Symbol('J'))))"
)
assert str(e3) == \
"Wigner3j(1, 2, 3, 4, 5, 6)*[Dagger(B) + A,C + D]x(-J2 + Jz)*|1,0><1,1|*(|1,0,j1=1,j2=1> + |1,1,j1=1,j2=1>)x|1,-1,j1=1,j2=1>"
ascii_str = \
"""\
[ + ] / 2 \\ \n\
/1 3 5\\*[B + A,C + D]x |- J + J |*|1,0><1,1|*(|1,0,j1=1,j2=1> + |1,1,j1=1,j2=1>)x |1,-1,j1=1,j2=1>\n\
| | \\ z/ \n\
\\2 4 6/ \
"""
ucode_str = \
u("""\
⎡ † ⎤ ⎛ 2 ⎞ \n\
⎛1 3 5⎞⋅⎣B + A,C + D⎦⨂ ⎜- J + J ⎟⋅❘1,0⟩⟨1,1❘⋅(❘1,0,j₁=1,j₂=1⟩ + ❘1,1,j₁=1,j₂=1⟩)⨂ ❘1,-1,j₁=1,j₂=1⟩\n\
⎜ ⎟ ⎝ z⎠ \n\
⎝2 4 6⎠ \
""")
assert pretty(e3) == ascii_str
assert upretty(e3) == ucode_str
assert latex(e3) == \
r'\left(\begin{array}{ccc} 1 & 3 & 5 \\ 2 & 4 & 6 \end{array}\right) {\left[B^{\dag} + A,C + D\right]}\otimes \left({- J^2 + J_z}\right) {\left|1,0\right\rangle }{\left\langle 1,1\right|} \left({{\left|1,0,j_{1}=1,j_{2}=1\right\rangle } + {\left|1,1,j_{1}=1,j_{2}=1\right\rangle }}\right)\otimes {{\left|1,-1,j_{1}=1,j_{2}=1\right\rangle }}'
sT(
e3,
"Mul(Wigner3j(Integer(1), Integer(2), Integer(3), Integer(4), Integer(5), Integer(6)), TensorProduct(Commutator(Add(Dagger(Operator(Symbol('B'))), Operator(Symbol('A'))),Add(Operator(Symbol('C')), Operator(Symbol('D')))), Add(Mul(Integer(-1), J2Op(Symbol('J'))), JzOp(Symbol('J')))), OuterProduct(JzKet(Integer(1),Integer(0)),JzBra(Integer(1),Integer(1))), TensorProduct(Add(JzKetCoupled(Integer(1),Integer(0),Tuple(Integer(1), Integer(1)),Tuple(Tuple(Integer(1), Integer(2), Integer(1)))), JzKetCoupled(Integer(1),Integer(1),Tuple(Integer(1), Integer(1)),Tuple(Tuple(Integer(1), Integer(2), Integer(1))))), JzKetCoupled(Integer(1),Integer(-1),Tuple(Integer(1), Integer(1)),Tuple(Tuple(Integer(1), Integer(2), Integer(1))))))"
)
assert str(e4) == '(C(1)*C(2)+F**2)*(L2(Interval(0, oo, False, True))+H)'
ascii_str = \
"""\
// 1 2\\ x2\\ / 2 \\\n\
\\\\C x C / + F / x \L + H/\
"""
ucode_str = \
u("""\
⎛⎛ 1 2⎞ ⨂2⎞ ⎛ 2 ⎞\n\
⎝⎝C ⨂ C ⎠ ⊕ F ⎠ ⨂ ⎝L ⊕ H⎠\
""")
assert pretty(e4) == ascii_str
assert upretty(e4) == ucode_str
assert latex(e4) == \
r'\left(\left(\mathcal{C}^{1}\otimes \mathcal{C}^{2}\right)\oplus {\mathcal{F}}^{\otimes 2}\right)\otimes \left({\mathcal{L}^2}\left( \left[0, \infty\right) \right)\oplus \mathcal{H}\right)'
sT(
e4,
"TensorProductHilbertSpace((DirectSumHilbertSpace(TensorProductHilbertSpace(ComplexSpace(Integer(1)),ComplexSpace(Integer(2))),TensorPowerHilbertSpace(FockSpace(),Integer(2)))),(DirectSumHilbertSpace(L2(Interval(Integer(0), oo, S.false, S.true)),HilbertSpace())))"
)
def test_commutator():
c = Comm(A, B)
assert c.is_commutative is False
assert isinstance(c, Comm)
assert c.subs(A, C) == Comm(C, B)
def test_sympy__physics__secondquant__Commutator():
from sympy.physics.secondquant import Commutator
assert _test_args(Commutator(x, y))
def test_sympy__physics__quantum__commutator__Commutator():
from sympy.physics.quantum.commutator import Commutator
A, B = symbols('A,B', commutative=False)
assert _test_args(Commutator(A, B))
def test_commutator():
assert qapply(Commutator(Jx, Jy)*Jz*po) == I*hbar**3*po
assert qapply(Commutator(J2, Jz)*Jz*po) == 0
assert qapply(Commutator(Jz, Foo('F'))*po) == 0
assert qapply(Commutator(Foo('F'), Jz)*po) == 0
