measurements.pretty_good_measurement¶
Compute the set of pretty good measurements from an ensemble.
Functions¶
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Return the set of pretty good measurements from a set of vectors and corresponding probabilities. |
Module Contents¶
- measurements.pretty_good_measurement.pretty_good_measurement(states, probs=None)¶
Return the set of pretty good measurements from a set of vectors and corresponding probabilities.
This computes the “pretty good measurement” as initially defined in [1].
The pretty good measurement (PGM) (also known as the “square root measurement”) is the set of POVMs \((G_1, \ldots, G_n)\) such that
\[G_i = P^{-1/2} \left(p_i \rho_i\right) P^{-1/2} \quad \text{where} \quad P = \sum_{i=1}^n p_i \rho_i.\]See also
pretty_bad_measurement
Examples
Consider the collection of trine states.
\[u_0 = |0\rangle, \quad u_1 = -\frac{1}{2}\left(|0\rangle + \sqrt{3}|1\rangle\right), \quad \text{and} \quad u_2 = -\frac{1}{2}\left(|0\rangle - \sqrt{3}|1\rangle\right).\]>>> from toqito.states import trine >>> from toqito.measurements import pretty_good_measurement >>> >>> states = trine() >>> probs = [1 / 3, 1 / 3, 1 / 3] >>> pgm = pretty_good_measurement(states, probs) >>> pgm [array([[0.66666667, 0. ], [0. , 0. ]]), array([[0.16666667, 0.28867513], [0.28867513, 0.5 ]]), array([[ 0.16666667, -0.28867513], [-0.28867513, 0.5 ]])]
References
[1]Lane P Hughston, Richard Jozsa, and William K Wootters. A complete classification of quantum ensembles having a given density matrix. Physics Letters A, 183(1):14–18, 1993.
- Raises:
ValueError – If number of vectors does not match number of probabilities.
ValueError – If probabilities do not sum to 1.
- Parameters:
states (list[numpy.ndarray]) – A collection of either states provided as either vectors or density matrices.
probs (list[float] | None) – A set of fixed probabilities for a given ensemble of quantum states. The function assumes a uniform probability distribution if the fixed probabilities for the input ensemble are not provided.
- Return type:
list[numpy.ndarray]