Source code for toqito.state_metrics.helstrom_holevo

"""Helstrom-Holevo metric gives the bst success probability to distinguish two mixed states."""

import numpy as np

from toqito.matrix_props import is_density, trace_norm


[docs] def helstrom_holevo(rho: np.ndarray, sigma: np.ndarray) -> float | np.floating: r"""Compute the Helstrom-Holevo distance between density matrices [@WikiHolevo]. In general, the best success probability to discriminate two mixed states represented by \(\rho\) and \(\sigma\) is given by [@WikiHolevo]. \[ \frac{1}{2}+\frac{1}{2} \left(\frac{1}{2} \left|\rho - \sigma \right|_1\right). \] Examples: Consider the following Bell state \[ u = \frac{1}{\sqrt{2}} \left( |00 \rangle + |11 \rangle \right) \in \mathcal{X}. \] The corresponding density matrix of \(u\) may be calculated by: \[ \rho = u u^* = \begin{pmatrix} 1 & 0 & 0 & 1 \\ 0 & 0 & 0 & 0 \\ 0 & 0 & 0 & 0 \\ 1 & 0 & 0 & 1 \end{pmatrix} \in \text{D}(\mathcal{X}). \] Calculating the Helstrom-Holevo distance of states that are identical yield a value of \(1/2\). This can be verified in `|toqito⟩` as follows. ```python exec="1" source="above" import numpy as np from toqito.states import basis from toqito.state_metrics import helstrom_holevo 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 print(helstrom_holevo(rho, sigma)) ``` Raises: ValueError: If matrices are not density operators. Args: rho: Density operator. sigma: Density operator. Returns: The Helstrom-Holevo distance between `rho` and `sigma`. """ if not is_density(rho) or not is_density(sigma): raise ValueError("Helstrom-Holevo is only defined for density operators.") return 1 / 2 + 1 / 2 * (trace_norm(rho - sigma)) / 2