:py:mod:`state_metrics.helstrom_holevo` ======================================= .. py:module:: state_metrics.helstrom_holevo .. autoapi-nested-parse:: Helstrom-Holevo metric. Module Contents --------------- Functions ~~~~~~~~~ .. autoapisummary:: state_metrics.helstrom_holevo.helstrom_holevo .. py:function:: helstrom_holevo(rho, sigma) Compute the Helstrom-Holevo distance between density matrices :cite:`WikiHolevo`. In general, the best success probability to discriminate two mixed states represented by :math:`\rho` and :math:`\sigma` is given by :cite:`WikiHolevo`. .. math:: \frac{1}{2}+\frac{1}{2} \left(\frac{1}{2} \left|\rho - \sigma \right|_1\right). .. rubric:: Examples Consider the following Bell state .. math:: u = \frac{1}{\sqrt{2}} \left( |00 \rangle + |11 \rangle \right) \in \mathcal{X}. The corresponding density matrix of :math:`u` may be calculated by: .. math:: \rho = u u^* = \begin{pmatrix} 1 & 0 & 0 & 1 \\ 0 & 0 & 0 & 0 \\ 0 & 0 & 0 & 0 \\ 1 & 0 & 0 & 1 \end{pmatrix} \in \text{D}(\mathcal{X}). Calculating the Helstrom-Holevo distance of states that are identical yield a value of :math:`1/2`. This can be verified in :code:`toqito` as follows. >>> from toqito.states import basis >>> from toqito.state_metrics import helstrom_holevo >>> import numpy as np >>> e_0, e_1 = basis(2, 0), basis(2, 1) >>> e_00 = np.kron(e_0, e_0) >>> e_11 = np.kron(e_1, e_1) >>> >>> u_vec = 1 / np.sqrt(2) * (e_00 + e_11) >>> rho = u_vec * u_vec.conj().T >>> sigma = rho >>> >>> helstrom_holevo(rho, sigma) 0.5 .. rubric:: References .. bibliography:: :filter: docname in docnames :raises ValueError: If matrices are not density operators. :param rho: Density operator. :param sigma: Density operator. :return: The Helstrom-Holevo distance between :code:`rho` and :code:`sigma`.