We exhibit an orthogonal set of product states of two separated three-state particles that nevertheless cannot be reliably distinguished by any sequence of local operations and classical communication between the separate observers. It is proved that there is a finite gap between the mutual information obtainable by a joint measurement on these states and a measurement in which only local actions are permitted. This result implies the existence of separable superoperators that cannot be implemented locally. A set of states are found involving three two-state particles which also appear to be non-measurable locally. These and other multipartite states are classified according to the entropy and entanglement costs of preparing and measuring t...
Entanglement appears under two different forms in quantum theory, namely, as a property of states of...
Activation of Bell nonlocality refers to the phenomenon that some entangled mixed states that admit ...
We prove that any three linearly independent pure quantum states can always be locally distinguished...
We exhibit an orthogonal set of product states of two three-state particles that nevertheless cannot...
We experimentally demonstrate the superior discrimination of separated, unentangled two-qubit correl...
It is shown that the ensemble $\{p (\alpha),|\alpha>|\alpha^*>\}$ where $p (\alpha)$ is a Gaussian d...
Nonlocality without entanglement is a rather counterintuitive phenomenon in which information may be...
We present a generic method to construct a product basis exhibiting Nonlocality Without Entanglement...
Bennett et al. Physical Review A, vol. 59, no. 2, p. 1070, 1999] identified a set of orthogonal prod...
An alternative proof for existence of ``quantum nonlocality without entanglement'', i.e. existence o...
We introduce an aspect of nonlocality which arises when the task of quantum states distinguishabilit...
Despite the success of quantum mechanics in predicting the outcomes of experiments in many branches ...
We present an experimental demonstration of quantum nonlocality without entanglement using single-ph...
Finding out conditions which tell whether a set of orthogonal multipartite quantum states can be dis...
We study the local indistinguishability problem of quantum states. By introducing an easily calculat...
Entanglement appears under two different forms in quantum theory, namely, as a property of states of...
Activation of Bell nonlocality refers to the phenomenon that some entangled mixed states that admit ...
We prove that any three linearly independent pure quantum states can always be locally distinguished...
We exhibit an orthogonal set of product states of two three-state particles that nevertheless cannot...
We experimentally demonstrate the superior discrimination of separated, unentangled two-qubit correl...
It is shown that the ensemble $\{p (\alpha),|\alpha>|\alpha^*>\}$ where $p (\alpha)$ is a Gaussian d...
Nonlocality without entanglement is a rather counterintuitive phenomenon in which information may be...
We present a generic method to construct a product basis exhibiting Nonlocality Without Entanglement...
Bennett et al. Physical Review A, vol. 59, no. 2, p. 1070, 1999] identified a set of orthogonal prod...
An alternative proof for existence of ``quantum nonlocality without entanglement'', i.e. existence o...
We introduce an aspect of nonlocality which arises when the task of quantum states distinguishabilit...
Despite the success of quantum mechanics in predicting the outcomes of experiments in many branches ...
We present an experimental demonstration of quantum nonlocality without entanglement using single-ph...
Finding out conditions which tell whether a set of orthogonal multipartite quantum states can be dis...
We study the local indistinguishability problem of quantum states. By introducing an easily calculat...
Entanglement appears under two different forms in quantum theory, namely, as a property of states of...
Activation of Bell nonlocality refers to the phenomenon that some entangled mixed states that admit ...
We prove that any three linearly independent pure quantum states can always be locally distinguished...