コード例 #1
0
class QuadraticHamiltoniansTest(unittest.TestCase):
    def setUp(self):
        self.n_qubits = 5
        self.constant = 1.7
        self.chemical_potential = 2.

        # Obtain random Hermitian and antisymmetric matrices
        self.hermitian_mat = random_hermitian_matrix(self.n_qubits)
        self.antisymmetric_mat = random_antisymmetric_matrix(self.n_qubits)

        self.combined_hermitian = (
            self.hermitian_mat -
            self.chemical_potential * numpy.eye(self.n_qubits))

        # Initialize a particle-number-conserving Hamiltonian
        self.quad_ham_pc = QuadraticHamiltonian(
            self.constant, self.hermitian_mat)

        # Initialize a non-particle-number-conserving Hamiltonian
        self.quad_ham_npc = QuadraticHamiltonian(
            self.constant, self.hermitian_mat, self.antisymmetric_mat,
            self.chemical_potential)

        # Initialize the sparse operators and get their ground energies
        self.quad_ham_pc_sparse = get_sparse_operator(self.quad_ham_pc)
        self.quad_ham_npc_sparse = get_sparse_operator(self.quad_ham_npc)

        self.pc_ground_energy, self.pc_ground_state = get_ground_state(
            self.quad_ham_pc_sparse)
        self.npc_ground_energy, self.npc_ground_state = get_ground_state(
            self.quad_ham_npc_sparse)

    def test_combined_hermitian_part(self):
        """Test getting the combined Hermitian part."""
        combined_hermitian_part = self.quad_ham_pc.combined_hermitian_part
        for i in numpy.ndindex(combined_hermitian_part.shape):
            self.assertAlmostEqual(self.hermitian_mat[i],
                                   combined_hermitian_part[i])

        combined_hermitian_part = self.quad_ham_npc.combined_hermitian_part
        for i in numpy.ndindex(combined_hermitian_part.shape):
            self.assertAlmostEqual(self.combined_hermitian[i],
                                   combined_hermitian_part[i])

    def test_hermitian_part(self):
        """Test getting the Hermitian part."""
        hermitian_part = self.quad_ham_pc.hermitian_part
        for i in numpy.ndindex(hermitian_part.shape):
            self.assertAlmostEqual(self.hermitian_mat[i], hermitian_part[i])

        hermitian_part = self.quad_ham_npc.hermitian_part
        for i in numpy.ndindex(hermitian_part.shape):
            self.assertAlmostEqual(self.hermitian_mat[i], hermitian_part[i])

    def test_antisymmetric_part(self):
        """Test getting the antisymmetric part."""
        antisymmetric_part = self.quad_ham_pc.antisymmetric_part
        for i in numpy.ndindex(antisymmetric_part.shape):
            self.assertAlmostEqual(0., antisymmetric_part[i])

        antisymmetric_part = self.quad_ham_npc.antisymmetric_part
        for i in numpy.ndindex(antisymmetric_part.shape):
            self.assertAlmostEqual(self.antisymmetric_mat[i],
                                   antisymmetric_part[i])

    def test_conserves_particle_number(self):
        """Test checking whether Hamiltonian conserves particle number."""
        self.assertTrue(self.quad_ham_pc.conserves_particle_number)
        self.assertFalse(self.quad_ham_npc.conserves_particle_number)

    def test_add_chemical_potential(self):
        """Test adding a chemical potential."""
        self.quad_ham_npc.add_chemical_potential(2.4)

        combined_hermitian_part = self.quad_ham_npc.combined_hermitian_part
        hermitian_part = self.quad_ham_npc.hermitian_part

        want_combined = (self.combined_hermitian -
                         2.4 * numpy.eye(self.n_qubits))
        want_hermitian = self.hermitian_mat

        for i in numpy.ndindex(combined_hermitian_part.shape):
            self.assertAlmostEqual(combined_hermitian_part[i],
                                   want_combined[i])

        for i in numpy.ndindex(hermitian_part.shape):
            self.assertAlmostEqual(hermitian_part[i], want_hermitian[i])

        self.assertAlmostEqual(2.4 + self.chemical_potential,
                               self.quad_ham_npc.chemical_potential)

    def test_orbital_energies(self):
        """Test getting the orbital energies."""
        # Test the particle-number-conserving case
        orbital_energies, constant = self.quad_ham_pc.orbital_energies()
        # Test the ground energy
        energy = numpy.sum(
            orbital_energies[orbital_energies < -EQ_TOLERANCE]) + constant
        self.assertAlmostEqual(energy, self.pc_ground_energy)

        # Test the non-particle-number-conserving case
        orbital_energies, constant = self.quad_ham_npc.orbital_energies()
        # Test the ground energy
        energy = constant
        self.assertAlmostEqual(energy, self.npc_ground_energy)

    def test_ground_energy(self):
        """Test getting the ground energy."""
        # Test particle-number-conserving case
        energy = self.quad_ham_pc.ground_energy()
        self.assertAlmostEqual(energy, self.pc_ground_energy)
        # Test non-particle-number-conserving case
        energy = self.quad_ham_npc.ground_energy()
        self.assertAlmostEqual(energy, self.npc_ground_energy)

    def test_majorana_form(self):
        """Test getting the Majorana form."""
        majorana_matrix, majorana_constant = self.quad_ham_npc.majorana_form()
        # Convert the Majorana form to a FermionOperator
        majorana_op = FermionOperator((), majorana_constant)
        for i in range(2 * self.n_qubits):
            if i < self.n_qubits:
                left_op = majorana_operator((i, 1))
            else:
                left_op = majorana_operator((i - self.n_qubits, 0))
            for j in range(2 * self.n_qubits):
                if j < self.n_qubits:
                    right_op = majorana_operator((j, 1), majorana_matrix[i, j])
                else:
                    right_op = majorana_operator((j - self.n_qubits, 0),
                                                 majorana_matrix[i, j])
                majorana_op += .5j * left_op * right_op
        # Get FermionOperator for original Hamiltonian
        fermion_operator = normal_ordered(
            get_fermion_operator(self.quad_ham_npc))
        self.assertTrue(
            normal_ordered(majorana_op).isclose(fermion_operator))

    def test_diagonalizing_bogoliubov_transform(self):
        """Test getting the diagonalizing Bogoliubov transformation."""
        hermitian_part = self.quad_ham_npc.combined_hermitian_part
        antisymmetric_part = self.quad_ham_npc.antisymmetric_part
        block_matrix = numpy.zeros((2 * self.n_qubits, 2 * self.n_qubits),
                                   dtype=complex)
        block_matrix[:self.n_qubits, :self.n_qubits] = antisymmetric_part
        block_matrix[:self.n_qubits, self.n_qubits:] = hermitian_part
        block_matrix[self.n_qubits:, :self.n_qubits] = -hermitian_part.conj()
        block_matrix[self.n_qubits:, self.n_qubits:] = (
            -antisymmetric_part.conj())

        ferm_unitary = self.quad_ham_npc.diagonalizing_bogoliubov_transform()

        # Check that the transformation is diagonalizing
        majorana_matrix, majorana_constant = self.quad_ham_npc.majorana_form()
        canonical, orthogonal = antisymmetric_canonical_form(majorana_matrix)
        diagonalized = ferm_unitary.conj().dot(
            block_matrix.dot(ferm_unitary.T.conj()))
        for i in numpy.ndindex((2 * self.n_qubits, 2 * self.n_qubits)):
            self.assertAlmostEqual(diagonalized[i], canonical[i])

        lower_unitary = ferm_unitary[self.n_qubits:]
        lower_left = lower_unitary[:, :self.n_qubits]
        lower_right = lower_unitary[:, self.n_qubits:]

        # Check that lower_left and lower_right satisfy the constraints
        # necessary for the transformed fermionic operators to satisfy
        # the fermionic anticommutation relations
        constraint_matrix_1 = (lower_left.dot(lower_left.T.conj()) +
                               lower_right.dot(lower_right.T.conj()))
        constraint_matrix_2 = (lower_left.dot(lower_right.T) +
                               lower_right.dot(lower_left.T))

        identity = numpy.eye(self.n_qubits, dtype=complex)
        for i in numpy.ndindex((self.n_qubits, self.n_qubits)):
            self.assertAlmostEqual(identity[i], constraint_matrix_1[i])
            self.assertAlmostEqual(0., constraint_matrix_2[i])
コード例 #2
0
class QuadraticHamiltoniansTest(unittest.TestCase):

    def setUp(self):
        self.n_qubits = 5
        self.constant = 1.7
        self.chemical_potential = 2.

        # Obtain random Hermitian and antisymmetric matrices
        self.hermitian_mat = random_hermitian_matrix(self.n_qubits)
        self.antisymmetric_mat = random_antisymmetric_matrix(self.n_qubits)

        self.combined_hermitian = (
                self.hermitian_mat -
                self.chemical_potential * numpy.eye(self.n_qubits))

        # Initialize a particle-number-conserving Hamiltonian
        self.quad_ham_pc = QuadraticHamiltonian(
                self.constant, self.hermitian_mat)

        # Initialize a non-particle-number-conserving Hamiltonian
        self.quad_ham_npc = QuadraticHamiltonian(
                self.constant, self.hermitian_mat, self.antisymmetric_mat,
                self.chemical_potential)

    def test_combined_hermitian_part(self):
        """Test getting the combined Hermitian part."""
        combined_hermitian_part = self.quad_ham_pc.combined_hermitian_part
        for i in numpy.ndindex(combined_hermitian_part.shape):
            self.assertAlmostEqual(self.hermitian_mat[i],
                                   combined_hermitian_part[i])

        combined_hermitian_part = self.quad_ham_npc.combined_hermitian_part
        for i in numpy.ndindex(combined_hermitian_part.shape):
            self.assertAlmostEqual(self.combined_hermitian[i],
                                   combined_hermitian_part[i])

    def test_hermitian_part(self):
        """Test getting the Hermitian part."""
        hermitian_part = self.quad_ham_pc.hermitian_part
        for i in numpy.ndindex(hermitian_part.shape):
            self.assertAlmostEqual(self.hermitian_mat[i], hermitian_part[i])

        hermitian_part = self.quad_ham_npc.hermitian_part
        for i in numpy.ndindex(hermitian_part.shape):
            self.assertAlmostEqual(self.hermitian_mat[i], hermitian_part[i])

    def test_antisymmetric_part(self):
        """Test getting the antisymmetric part."""
        antisymmetric_part = self.quad_ham_pc.antisymmetric_part
        for i in numpy.ndindex(antisymmetric_part.shape):
            self.assertAlmostEqual(0., antisymmetric_part[i])

        antisymmetric_part = self.quad_ham_npc.antisymmetric_part
        for i in numpy.ndindex(antisymmetric_part.shape):
            self.assertAlmostEqual(self.antisymmetric_mat[i],
                                   antisymmetric_part[i])

    def test_conserves_particle_number(self):
        """Test checking whether Hamiltonian conserves particle number."""
        self.assertTrue(self.quad_ham_pc.conserves_particle_number)
        self.assertFalse(self.quad_ham_npc.conserves_particle_number)

    def test_add_chemical_potential(self):
        """Test adding a chemical potential."""
        self.quad_ham_npc.add_chemical_potential(2.4)

        combined_hermitian_part = self.quad_ham_npc.combined_hermitian_part
        hermitian_part = self.quad_ham_npc.hermitian_part

        want_combined = (self.combined_hermitian -
                         2.4 * numpy.eye(self.n_qubits))
        want_hermitian = self.hermitian_mat

        for i in numpy.ndindex(combined_hermitian_part.shape):
            self.assertAlmostEqual(combined_hermitian_part[i],
                                   want_combined[i])

        for i in numpy.ndindex(hermitian_part.shape):
            self.assertAlmostEqual(hermitian_part[i], want_hermitian[i])

        self.assertAlmostEqual(2.4 + self.chemical_potential,
                               self.quad_ham_npc.chemical_potential)

    def test_orbital_energies(self):
        """Test getting the orbital energies."""
        # Test the particle-number-conserving case
        orbital_energies, constant = self.quad_ham_pc.orbital_energies()
        # Test the ground energy
        energy = numpy.sum(
                orbital_energies[orbital_energies < -EQ_TOLERANCE]) + constant
        quad_ham_pc_sparse = get_sparse_operator(self.quad_ham_pc)
        ground_energy, ground_state = get_ground_state(quad_ham_pc_sparse)
        self.assertAlmostEqual(energy, ground_energy)

        # Test the non-particle-number-conserving case
        orbital_energies, constant = self.quad_ham_npc.orbital_energies()
        # Test the ground energy
        energy = constant
        quad_ham_npc_sparse = get_sparse_operator(self.quad_ham_npc)
        ground_energy, ground_state = get_ground_state(quad_ham_npc_sparse)
        self.assertAlmostEqual(energy, ground_energy)

    def test_majorana_form(self):
        """Test getting the Majorana form."""
        majorana_matrix, majorana_constant = self.quad_ham_npc.majorana_form()
        # Convert the Majorana form to a FermionOperator
        majorana_op = FermionOperator((), majorana_constant)
        for i in range(2 * self.n_qubits):
            if i < self.n_qubits:
                left_op = majorana_operator((i, 1))
            else:
                left_op = majorana_operator((i - self.n_qubits, 0))
            for j in range(2 * self.n_qubits):
                if j < self.n_qubits:
                    right_op = majorana_operator((j, 1), majorana_matrix[i, j])
                else:
                    right_op = majorana_operator((j - self.n_qubits, 0),
                                                 majorana_matrix[i, j])
                majorana_op += .5j * left_op * right_op
        # Get FermionOperator for original Hamiltonian
        fermion_operator = normal_ordered(
                get_fermion_operator(self.quad_ham_npc))
        self.assertTrue(
                normal_ordered(majorana_op).isclose(fermion_operator))
コード例 #3
0
class QuadraticHamiltoniansTest(unittest.TestCase):
    def setUp(self):
        self.n_qubits = 5
        self.constant = 1.7
        self.chemical_potential = 2.

        # Obtain random Hermitian and antisymmetric matrices
        rand_mat_A = numpy.random.randn(self.n_qubits, self.n_qubits)
        rand_mat_B = numpy.random.randn(self.n_qubits, self.n_qubits)
        rand_mat = rand_mat_A + 1.j * rand_mat_B
        self.hermitian_mat = rand_mat + rand_mat.T.conj()
        rand_mat_A = numpy.random.randn(self.n_qubits, self.n_qubits)
        rand_mat_B = numpy.random.randn(self.n_qubits, self.n_qubits)
        rand_mat = rand_mat_A + 1.j * rand_mat_B
        self.antisymmetric_mat = rand_mat - rand_mat.T

        self.combined_hermitian = (
            self.hermitian_mat -
            self.chemical_potential * numpy.eye(self.n_qubits))

        # Initialize a particle-number-conserving Hamiltonian
        self.quad_ham_pc = QuadraticHamiltonian(self.constant,
                                                self.hermitian_mat)

        # Initialize a non-particle-number-conserving Hamiltonian
        self.quad_ham_npc = QuadraticHamiltonian(self.constant,
                                                 self.hermitian_mat,
                                                 self.antisymmetric_mat,
                                                 self.chemical_potential)

    def test_combined_hermitian_part(self):
        """Test getting the combined Hermitian part."""
        combined_hermitian_part = self.quad_ham_pc.combined_hermitian_part()
        for i in numpy.ndindex(combined_hermitian_part.shape):
            self.assertAlmostEqual(self.hermitian_mat[i],
                                   combined_hermitian_part[i])

        combined_hermitian_part = self.quad_ham_npc.combined_hermitian_part()
        for i in numpy.ndindex(combined_hermitian_part.shape):
            self.assertAlmostEqual(self.combined_hermitian[i],
                                   combined_hermitian_part[i])

    def test_hermitian_part(self):
        """Test getting the Hermitian part."""
        hermitian_part = self.quad_ham_pc.hermitian_part()
        for i in numpy.ndindex(hermitian_part.shape):
            self.assertAlmostEqual(self.hermitian_mat[i], hermitian_part[i])

        hermitian_part = self.quad_ham_npc.hermitian_part()
        for i in numpy.ndindex(hermitian_part.shape):
            self.assertAlmostEqual(self.hermitian_mat[i], hermitian_part[i])

    def test_antisymmetric_part(self):
        """Test getting the antisymmetric part."""
        antisymmetric_part = self.quad_ham_pc.antisymmetric_part()
        for i in numpy.ndindex(antisymmetric_part.shape):
            self.assertAlmostEqual(0., antisymmetric_part[i])

        antisymmetric_part = self.quad_ham_npc.antisymmetric_part()
        for i in numpy.ndindex(antisymmetric_part.shape):
            self.assertAlmostEqual(self.antisymmetric_mat[i],
                                   antisymmetric_part[i])

    def test_conserves_particle_number(self):
        """Test checking whether Hamiltonian conserves particle number."""
        self.assertTrue(self.quad_ham_pc.conserves_particle_number())
        self.assertFalse(self.quad_ham_npc.conserves_particle_number())

    def test_majorana_form(self):
        """Test getting the Majorana form."""
        majorana_matrix, majorana_constant = self.quad_ham_npc.majorana_form()
        # Convert the Majorana form to a FermionOperator
        majorana_op = FermionOperator((), majorana_constant)
        for i in range(2 * self.n_qubits):
            if i < self.n_qubits:
                left_op = majorana_operator((i, 1))
            else:
                left_op = majorana_operator((i - self.n_qubits, 0))
            for j in range(2 * self.n_qubits):
                if j < self.n_qubits:
                    right_op = majorana_operator((j, 1), majorana_matrix[i, j])
                else:
                    right_op = majorana_operator((j - self.n_qubits, 0),
                                                 majorana_matrix[i, j])
                majorana_op += .5j * left_op * right_op
        # Get FermionOperator for original Hamiltonian
        fermion_operator = normal_ordered(
            get_fermion_operator(self.quad_ham_npc))
        self.assertTrue(normal_ordered(majorana_op).isclose(fermion_operator))
コード例 #4
0
class DiagonalizingFermionicUnitaryTest(unittest.TestCase):

    def setUp(self):
        self.n_qubits = 5
        self.constant = 1.7
        self.chemical_potential = 2.

        # Obtain random Hermitian and antisymmetric matrices
        self.hermitian_mat = random_hermitian_matrix(self.n_qubits)
        self.antisymmetric_mat = random_antisymmetric_matrix(self.n_qubits)

        # Initialize a non-particle-number-conserving Hamiltonian
        self.quad_ham_npc = QuadraticHamiltonian(
                self.constant, self.hermitian_mat, self.antisymmetric_mat,
                self.chemical_potential)

    def test_diagonalizes_quadratic_hamiltonian(self):
        """Test that the unitary returned indeed diagonalizes a
        quadratic Hamiltonian."""
        hermitian_part = self.quad_ham_npc.combined_hermitian_part
        antisymmetric_part = self.quad_ham_npc.antisymmetric_part
        block_matrix = numpy.zeros((2 * self.n_qubits, 2 * self.n_qubits),
                                   dtype=complex)
        block_matrix[:self.n_qubits, :self.n_qubits] = antisymmetric_part
        block_matrix[:self.n_qubits, self.n_qubits:] = hermitian_part
        block_matrix[self.n_qubits:, :self.n_qubits] = -hermitian_part.conj()
        block_matrix[self.n_qubits:, self.n_qubits:] = (
                -antisymmetric_part.conj())

        majorana_matrix, majorana_constant = self.quad_ham_npc.majorana_form()
        canonical, orthogonal = antisymmetric_canonical_form(majorana_matrix)
        ferm_unitary = diagonalizing_fermionic_unitary(majorana_matrix)
        diagonalized = ferm_unitary.conj().dot(
                block_matrix.dot(ferm_unitary.T.conj()))
        for i in numpy.ndindex((2 * self.n_qubits, 2 * self.n_qubits)):
            self.assertAlmostEqual(diagonalized[i], canonical[i])

    def test_bad_dimensions(self):
        n, p = (3, 4)
        ones_mat = numpy.ones((n, p))
        with self.assertRaises(ValueError):
            ferm_unitary = diagonalizing_fermionic_unitary(ones_mat)

    def test_not_antisymmetric(self):
        n = 4
        ones_mat = numpy.ones((n, n))
        with self.assertRaises(ValueError):
            ferm_unitary = diagonalizing_fermionic_unitary(ones_mat)

    def test_n_equals_3(self):
        n = 3
        # Obtain a random antisymmetric matrix
        rand_mat = numpy.random.randn(2 * n, 2 * n)
        antisymmetric_matrix = rand_mat - rand_mat.T

        # Get the diagonalizing fermionic unitary
        ferm_unitary = diagonalizing_fermionic_unitary(antisymmetric_matrix)
        lower_unitary = ferm_unitary[n:]
        lower_left = lower_unitary[:, :n]
        lower_right = lower_unitary[:, n:]

        # Check that lower_left and lower_right satisfy the constraints
        # necessary for the transformed fermionic operators to satisfy
        # the fermionic anticommutation relations
        constraint_matrix_1 = (lower_left.dot(lower_left.T.conj()) +
                               lower_right.dot(lower_right.T.conj()))
        constraint_matrix_2 = (lower_left.dot(lower_right.T) +
                               lower_right.dot(lower_left.T))

        identity = numpy.eye(n, dtype=complex)
        for i in numpy.ndindex((n, n)):
            self.assertAlmostEqual(identity[i], constraint_matrix_1[i])
            self.assertAlmostEqual(0., constraint_matrix_2[i])