Please use this identifier to cite or link to this item: http://hdl.handle.net/10397/43976
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dc.contributorDepartment of Applied Mathematics-
dc.creatorHu, Sen_US
dc.creatorQi, Len_US
dc.creatorZhang, Gen_US
dc.date.accessioned2016-06-07T06:37:32Z-
dc.date.available2016-06-07T06:37:32Z-
dc.identifier.issn1050-2947en_US
dc.identifier.urihttp://hdl.handle.net/10397/43976-
dc.language.isoenen_US
dc.publisherAmerican Physical Societyen_US
dc.rights©2016 American Physical Societyen_US
dc.rightsThe following publication Hu, S., Qi, L., & Zhang, G. (2016). Computing the geometric measure of entanglement of multipartite pure states by means of non-negative tensors. Physical Review A, 93(1), 1012304-1-012304-7 is available at https://doi.org/10.1103/PhysRevA.93.012304.en_US
dc.titleComputing the geometric measure of entanglement of multipartite pure states by means of non-negative tensorsen_US
dc.typeJournal/Magazine Articleen_US
dc.identifier.spage012304-1en_US
dc.identifier.epage012304-7en_US
dc.identifier.volume93en_US
dc.identifier.issue1en_US
dc.identifier.doi10.1103/PhysRevA.93.012304en_US
dcterms.abstractThe geometric measure of entanglement for pure states has attracted much attention. On the other hand, the spectral theory of non-negative tensors (hypermatrices) has been developed rapidly. In this paper, we show how the spectral theory of non-negative tensors can be applied to the study of the geometric measure of entanglement for pure states. For symmetric pure multipartite qubit or qutrit states an elimination method is given. For symmetric pure multipartite qudit states, a numerical algorithm with randomization is presented. We also show that a nonsymmetric pure state can be augmented to a symmetric one whose amplitudes can be encoded in a non-negative symmetric tensor, so the geometric measure of entanglement can be calculated. Several examples, such as mGHZ states, W states, inverted W states, qudits, and nonsymmetric states, are used to demonstrate the power of the proposed methods. Given a pure state, one can always find a change of basis (a unitary transformation) so that all the probability amplitudes of the pure state are non-negative under the new basis. Therefore, the methods proposed here can be applied to a very wide class of multipartite pure states.-
dcterms.accessRightsopen accessen_US
dcterms.bibliographicCitationPhysical review. A, Atomic, molecular, and optical physics, Jan. 2016, v. 93, no. 1, 012304, p. 1012304-1-012304-7en_US
dcterms.isPartOfPhysical review. A, Atomic, molecular, and optical physicsen_US
dcterms.issued2016-01-
dc.identifier.isiWOS:000367659100002-
dc.identifier.scopus2-s2.0-84954547010-
dc.identifier.eissn1094-1622en_US
dc.identifier.rosgroupid2015000347-
dc.description.ros2015-2016 > Academic research: refereed > Publication in refereed journal-
dc.description.oaVersion of Recorden_US
dc.identifier.FolderNumbera0850-n29en_US
dc.identifier.SubFormID1760en_US
dc.description.fundingSourceRGCen_US
dc.description.fundingTextPolyU 502111, No. 501212, No. 501913, No. 531213, No. 15302114, and No. 15206915en_US
dc.description.pubStatusPublisheden_US
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