def bogoliubov_trans(p, q, theta):
    r"""The 2-mode Bogoliubov transformation is mapped to two-qubit operations.
     We use the identity X S^\dag X S X = Y X S^\dag Y S X = X to transform
     the Hamiltonian XY+YX to XX+YY type. The time evolution of the XX + YY
     Hamiltonian can be expressed as a power of the iSWAP gate.

    Args:
        p: the first qubit
        q: the second qubit
        theta: The rotational angle that specifies the Bogoliubov
        transformation, which is a function of the kinetic energy and
        the superconducting gap.
    """

    # The iSWAP gate corresponds to evolve under the Hamiltonian XX+YY for
    # time -pi/4.
    expo = -4 * theta / np.pi

    yield cirq.X(p)
    yield cirq.S(p)
    yield cirq.ISWAP(p, q)**expo
    yield cirq.S(p) ** 1.5
    yield cirq.X(p)
def bogoliubov_trans ( p , q , theta ) : expo = - 4 * theta / np . pi yield cirq . X ( p ) yield cirq . S ( p ) yield cirq . ISWAP ( p , q ) ** expo yield cirq . S ( p ) ** 1.5 yield cirq . X ( p )
r"""The 2-mode Bogoliubov transformation is mapped to two-qubit operations.
     We use the identity X S^\dag X S X = Y X S^\dag Y S X = X to transform
     the Hamiltonian XY+YX to XX+YY type. The time evolution of the XX + YY
     Hamiltonian can be expressed as a power of the iSWAP gate.

    Args:
        p: the first qubit
        q: the second qubit
        theta: The rotational angle that specifies the Bogoliubov
        transformation, which is a function of the kinetic energy and
        the superconducting gap.