Example #1
0
def test_doit():
    x, y = symbols('x y')
    d = Density([XKet(), 0.5], [PxKet(), 0.5])
    assert (0.5 * (PxKet() * Dagger(PxKet())) + 0.5 *
            (XKet() * Dagger(XKet()))) == d.doit()

    # check for kets with expr in them
    d_with_sym = Density([XKet(x * y), 0.5], [PxKet(x * y), 0.5])
    assert (0.5 * (PxKet(x * y) * Dagger(PxKet(x * y))) + 0.5 *
            (XKet(x * y) * Dagger(XKet(x * y)))) == d_with_sym.doit()
Example #2
0
def test_doit():
    x,y = symbols('x y')
    d = Density([XKet(),0.5], [PxKet(),0.5])
    assert (0.5*(PxKet()*Dagger(PxKet())) +
            0.5*(XKet()*Dagger(XKet()))) == d.doit()

    # check for kets with expr in them
    d_with_sym = Density([XKet(x*y),0.5], [PxKet(x*y),0.5])
    assert (0.5*(PxKet(x*y)*Dagger(PxKet(x*y))) +
            0.5*(XKet(x*y)*Dagger(XKet(x*y)))) == d_with_sym.doit()
Example #3
0
def test_eval_trace():
    up = JzKet(S(1)/2, S(1)/2)
    down = JzKet(S(1)/2, -S(1)/2)
    d = Density((up, 0.5), (down, 0.5))

    t = Tr(d)
    assert t.doit() == 1

    #test dummy time dependent states
    class TestTimeDepKet(TimeDepKet):
        def _eval_trace(self, bra, **options):
            return 1

    x, t = symbols('x t')
    k1 = TestTimeDepKet(0, 0.5)
    k2 = TestTimeDepKet(0, 1)
    d = Density([k1, 0.5], [k2, 0.5])
    assert d.doit() == (0.5 * OuterProduct(k1, k1.dual) +
                        0.5 * OuterProduct(k2, k2.dual))

    t = Tr(d)
    assert t.doit() == 1
Example #4
0
def test_eval_trace():
    up = JzKet(S(1) / 2, S(1) / 2)
    down = JzKet(S(1) / 2, -S(1) / 2)
    d = Density((up, 0.5), (down, 0.5))

    t = Tr(d)
    assert t.doit() == 1

    #test dummy time dependent states
    class TestTimeDepKet(TimeDepKet):
        def _eval_trace(self, bra, **options):
            return 1

    x, t = symbols('x t')
    k1 = TestTimeDepKet(0, 0.5)
    k2 = TestTimeDepKet(0, 1)
    d = Density([k1, 0.5], [k2, 0.5])
    assert d.doit() == (0.5 * OuterProduct(k1, k1.dual) +
                        0.5 * OuterProduct(k2, k2.dual))

    t = Tr(d)
    assert t.doit() == 1
Example #5
0
def test_doit():

    x, y = symbols('x y')
    A, B, C, D, E, F = symbols('A B C D E F', commutative=False)
    d = Density([XKet(), 0.5], [PxKet(), 0.5])
    assert (0.5*(PxKet()*Dagger(PxKet())) +
            0.5*(XKet()*Dagger(XKet()))) == d.doit()

    # check for kets with expr in them
    d_with_sym = Density([XKet(x*y), 0.5], [PxKet(x*y), 0.5])
    assert (0.5*(PxKet(x*y)*Dagger(PxKet(x*y))) +
            0.5*(XKet(x*y)*Dagger(XKet(x*y)))) == d_with_sym.doit()

    d = Density([(A + B)*C, 1.0])
    assert d.doit() == (1.0*A*C*Dagger(C)*Dagger(A) +
                        1.0*A*C*Dagger(C)*Dagger(B) +
                        1.0*B*C*Dagger(C)*Dagger(A) +
                        1.0*B*C*Dagger(C)*Dagger(B))

    #  With TensorProducts as args
    # Density with simple tensor products as args
    t = TensorProduct(A, B, C)
    d = Density([t, 1.0])
    assert d.doit() == \
        1.0 * TensorProduct(A*Dagger(A), B*Dagger(B), C*Dagger(C))

    # Density with multiple Tensorproducts as states
    t2 = TensorProduct(A, B)
    t3 = TensorProduct(C, D)

    d = Density([t2, 0.5], [t3, 0.5])
    assert d.doit() == (0.5 * TensorProduct(A*Dagger(A), B*Dagger(B)) +
                        0.5 * TensorProduct(C*Dagger(C), D*Dagger(D)))

    #Density with mixed states
    d = Density([t2 + t3, 1.0])
    assert d.doit() == (1.0 * TensorProduct(A*Dagger(A), B*Dagger(B)) +
                        1.0 * TensorProduct(A*Dagger(C), B*Dagger(D)) +
                        1.0 * TensorProduct(C*Dagger(A), D*Dagger(B)) +
                        1.0 * TensorProduct(C*Dagger(C), D*Dagger(D)))

    #Density operators with spin states
    tp1 = TensorProduct(JzKet(1, 1), JzKet(1, -1))
    d = Density([tp1, 1])

    # full trace
    t = Tr(d)
    assert t.doit() == 1

    #Partial trace on density operators with spin states
    t = Tr(d, [0])
    assert t.doit() == JzKet(1, -1) * Dagger(JzKet(1, -1))
    t = Tr(d, [1])
    assert t.doit() == JzKet(1, 1) * Dagger(JzKet(1, 1))

    # with another spin state
    tp2 = TensorProduct(JzKet(S(1)/2, S(1)/2), JzKet(S(1)/2, -S(1)/2))
    d = Density([tp2, 1])

    #full trace
    t = Tr(d)
    assert t.doit() == 1

    #Partial trace on density operators with spin states
    t = Tr(d, [0])
    assert t.doit() == JzKet(S(1)/2, -S(1)/2) * Dagger(JzKet(S(1)/2, -S(1)/2))
    t = Tr(d, [1])
    assert t.doit() == JzKet(S(1)/2, S(1)/2) * Dagger(JzKet(S(1)/2, S(1)/2))
Example #6
0
def test_doit():

    x, y = symbols('x y')
    A, B, C, D, E, F = symbols('A B C D E F', commutative=False)
    d = Density([XKet(), 0.5], [PxKet(), 0.5])
    assert (0.5 * (PxKet() * Dagger(PxKet())) + 0.5 *
            (XKet() * Dagger(XKet()))) == d.doit()

    # check for kets with expr in them
    d_with_sym = Density([XKet(x * y), 0.5], [PxKet(x * y), 0.5])
    assert (0.5 * (PxKet(x * y) * Dagger(PxKet(x * y))) + 0.5 *
            (XKet(x * y) * Dagger(XKet(x * y)))) == d_with_sym.doit()

    d = Density([(A + B) * C, 1.0])
    assert d.doit() == (1.0 * A * C * Dagger(C) * Dagger(A) +
                        1.0 * A * C * Dagger(C) * Dagger(B) +
                        1.0 * B * C * Dagger(C) * Dagger(A) +
                        1.0 * B * C * Dagger(C) * Dagger(B))

    #  With TensorProducts as args
    # Density with simple tensor products as args
    t = TensorProduct(A, B, C)
    d = Density([t, 1.0])
    assert d.doit() == \
        1.0 * TensorProduct(A*Dagger(A), B*Dagger(B), C*Dagger(C))

    # Density with multiple Tensorproducts as states
    t2 = TensorProduct(A, B)
    t3 = TensorProduct(C, D)

    d = Density([t2, 0.5], [t3, 0.5])
    assert d.doit() == (0.5 * TensorProduct(A * Dagger(A), B * Dagger(B)) +
                        0.5 * TensorProduct(C * Dagger(C), D * Dagger(D)))

    #Density with mixed states
    d = Density([t2 + t3, 1.0])
    assert d.doit() == (1.0 * TensorProduct(A * Dagger(A), B * Dagger(B)) +
                        1.0 * TensorProduct(A * Dagger(C), B * Dagger(D)) +
                        1.0 * TensorProduct(C * Dagger(A), D * Dagger(B)) +
                        1.0 * TensorProduct(C * Dagger(C), D * Dagger(D)))

    #Density operators with spin states
    tp1 = TensorProduct(JzKet(1, 1), JzKet(1, -1))
    d = Density([tp1, 1])

    # full trace
    t = Tr(d)
    assert t.doit() == 1

    #Partial trace on density operators with spin states
    t = Tr(d, [0])
    assert t.doit() == JzKet(1, -1) * Dagger(JzKet(1, -1))
    t = Tr(d, [1])
    assert t.doit() == JzKet(1, 1) * Dagger(JzKet(1, 1))

    # with another spin state
    tp2 = TensorProduct(JzKet(S(1) / 2, S(1) / 2), JzKet(S(1) / 2, -S(1) / 2))
    d = Density([tp2, 1])

    #full trace
    t = Tr(d)
    assert t.doit() == 1

    #Partial trace on density operators with spin states
    t = Tr(d, [0])
    assert t.doit() == JzKet(S(1) / 2, -S(1) / 2) * Dagger(
        JzKet(S(1) / 2, -S(1) / 2))
    t = Tr(d, [1])
    assert t.doit() == JzKet(S(1) / 2,
                             S(1) / 2) * Dagger(JzKet(S(1) / 2,
                                                      S(1) / 2))