4.6 Article

Direct determination of arbitrary dimensional entanglement monotones using statistical correlators and minimal complementary measurements

期刊

QUANTUM SCIENCE AND TECHNOLOGY
卷 7, 期 4, 页码 -

出版社

IOP Publishing Ltd
DOI: 10.1088/20589565/ac8e28

关键词

higher dimensional quantum information processing; entanglement measures; entanglement monotones

资金

  1. Ministry of Electronics and Information Technology (MeitY), Government of India [4(7)/2020-ITEA, Q-97]
  2. QuEST-DST Project Q-97 of the Govt. of India

向作者/读者索取更多资源

This paper fills the gap in determining entanglement monotones (EMs) in entangled qudit states. Analytical relations between statistical correlation measures and standard EMs are derived, and experimentally measured for two-qutrit pure states. The results provide valuable insights into the operational implications and non-monotonicity of EMs in bipartite pure qudit states.
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.

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