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_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