2020
DOI: 10.1103/physrevresearch.2.022039
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Conserved quantities in parity-time symmetric systems

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Cited by 43 publications
(32 citation statements)
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“…A class of Hamiltonians with PT-symmetry, which commute with the joint operation parity P and time-reversal operator T , was found to be able to keep the eigenvalues of H real in the exact PT phase [ 23 ]. Since then, PT quantum mechanics has been extensively investigated theoretically [ 24 , 25 , 26 , 27 , 28 , 29 , 30 , 31 , 32 , 33 , 34 , 35 , 36 , 37 , 38 , 39 , 40 , 41 , 42 , 43 , 44 ] and experimentally [ 12 , 13 , 14 , 45 , 46 , 47 , 48 ]. In fact, P -pseudo-Hermiticity was pointed out to be a sufficient and necessary condition to keep the spectrum of a non-Hermitian Hamiltonian purely real [ 49 , 50 , 51 ], and both the theory and applications are developed further [ 52 , 53 , 54 , 55 , 56 , 57 ].…”
Section: Introductionmentioning
confidence: 99%
“…A class of Hamiltonians with PT-symmetry, which commute with the joint operation parity P and time-reversal operator T , was found to be able to keep the eigenvalues of H real in the exact PT phase [ 23 ]. Since then, PT quantum mechanics has been extensively investigated theoretically [ 24 , 25 , 26 , 27 , 28 , 29 , 30 , 31 , 32 , 33 , 34 , 35 , 36 , 37 , 38 , 39 , 40 , 41 , 42 , 43 , 44 ] and experimentally [ 12 , 13 , 14 , 45 , 46 , 47 , 48 ]. In fact, P -pseudo-Hermiticity was pointed out to be a sufficient and necessary condition to keep the spectrum of a non-Hermitian Hamiltonian purely real [ 49 , 50 , 51 ], and both the theory and applications are developed further [ 52 , 53 , 54 , 55 , 56 , 57 ].…”
Section: Introductionmentioning
confidence: 99%
“…However, the EP degeneracies also occur in dissipative systems with mode-selective losses. Such passive PT -symmetric systems have been realized in the quantum domain with lossy, single-photons [31][32][33][34][35][36][37][38], ultracold atoms [39], and a superconducting transmon [40]. These realizations are limited to effective twodimensional Hamiltonians with second-order EPs, and their quantum information studies are confined to global properties [34].…”
Section: Introductionmentioning
confidence: 99%
“…In order to achieve the maximal violation of CFFW inequality, we scan the whole permitted measurement strategies of Alice and Bob since the observables are unknown but keeping B 1 and B 2 mutually unbiased. In the experiment, we only need to add certain QWPs in the original measurement setup, namely, a combination of sandwich type QWP-HWP-QWP sequence [36][37][38], and a following PBS to realize the measurement operators. The coincidence counting of the APDs {D1, D3} represent the result a = b = 0, simultaneously.…”
Section: Experimental Demonstration and Resultsmentioning
confidence: 99%