Direct determination of arbitrary dimensional entanglement monotones using statistical correlators and minimal complementary measurements. (1st October 2022)

• Record Type: Journal Article
• Authors: Ghosh, Debadrita; Jennewein, Thomas; Sinha, Urbasi
• Is Part Of: Quantum science and technology. Volume 7:Number 4(2022)
• Publication Date: 2022-10-01
• Subjects: higher dimensional quantum information processing -- entanglement measures -- entanglement monotones; Quantum theory -- Periodicals; Quantum theory; Periodicals; 530
• DOI: 10.1088/2058-9565/ac8e28
• Languages: English
• ISSNs: 2058-9565

Abstract

Abstract: Higher dimensional quantum systems (qudits) present a potentially more efficient means, compared to qubits, for implementing various information theoretic tasks. One of the ubiquitous resources in such explorations is entanglement. Entanglement monotones (EMs) are of key importance, particularly for assessing the efficacy of a given entangled state as a resource for information theoretic tasks. Till date, investigations towards determination of EMs have focused on providing their tighter lower bounds. There is yet no general scheme available for direct determination of the EMs. Consequently, an empirical determination of any EM has not yet been achieved for entangled qudit states. The present paper fills this gap, both theoretically as well as experimentally. First, we derive analytical relations between statistical correlation measures i.e. mutual predictability (MP), mutual information (MI) and Pearson correlation coefficient (PCC) and standard EMs i.e. negativity (N) and entanglement of formation (EOF) in arbitrary dimensions. As a proof of concept, we then experimentally measure MP, MI and PCC of two-qutrit pure states and determine their N and EOF using these derived relations. This is a useful addition to the experimenter's toolkit wherein by using a limited number of measurements (in this case 1 set of measurements), one can directly measure the EMs in a bipartite arbitrary dimensional system. We obtain the value of N for our bipartite qutrit to be 0.907 ± 0.013 and the EOF to be 1.323 ± 0.022. Since the present scheme enables determination of more than one EM by the same limited number of measurements, we argue that it can serve as a unique experimental platform for quantitatively comparing and contrasting the operational implications of EMs as well as showing their non-monotonicity for a given bipartite pure qudit state.