Automatic hermiticity for mixed states

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Automatic hermiticity for mixed states. / Nagao, Keiichi; Nielsen, Holger Bech.

I: Progress of Theoretical and Experimental Physics, Bind 2023, Nr. 3, 031B01, 09.03.2023.

Publikation: Bidrag til tidsskriftTidsskriftartikelForskningfagfællebedømt

Harvard

Nagao, K & Nielsen, HB 2023, 'Automatic hermiticity for mixed states', Progress of Theoretical and Experimental Physics, bind 2023, nr. 3, 031B01. https://doi.org/10.1093/ptep/ptad025

APA

Nagao, K., & Nielsen, H. B. (2023). Automatic hermiticity for mixed states. Progress of Theoretical and Experimental Physics, 2023(3), [031B01]. https://doi.org/10.1093/ptep/ptad025

Vancouver

Nagao K, Nielsen HB. Automatic hermiticity for mixed states. Progress of Theoretical and Experimental Physics. 2023 mar. 9;2023(3). 031B01. https://doi.org/10.1093/ptep/ptad025

Author

Nagao, Keiichi ; Nielsen, Holger Bech. / Automatic hermiticity for mixed states. I: Progress of Theoretical and Experimental Physics. 2023 ; Bind 2023, Nr. 3.

Bibtex

@article{aeb34e09e79b4c0d9bd0c468afd64251,
title = "Automatic hermiticity for mixed states",
abstract = "We previously proposed a mechanism to effectively obtain, after a long time development, a Hamiltonian being Hermitian with regard to a modified inner product I-Q that makes a given non-normal Hamiltonian normal by using an appropriately chosen Hermitian operator Q. We studied it for pure states. In this letter we show that a similar mechanism also works for mixed states by introducing density matrices to describe them and investigating their properties explicitly both in the future-not-included and future-included theories. In particular, in the latter, where not only a past state at the initial time T-A but also a future state at the final time T-B is given, we study a couple of candidates for it, and introduce a {"}skew density matrix{"} composed of both ensembles of the future and past states such that the trace of the product of it and an operator O matches a normalized matrix element of O. We argue that the skew density matrix defined with I-Q at the present time t for large T-B - t and large t - T-A approximately corresponds to another density matrix composed of only an ensemble of past states and defined with another inner product I-QJ for large t - T-A.",
keywords = "PSEUDO-HERMITICITY, PT-SYMMETRY, FUTURE",
author = "Keiichi Nagao and Nielsen, {Holger Bech}",
year = "2023",
month = mar,
day = "9",
doi = "10.1093/ptep/ptad025",
language = "English",
volume = "2023",
journal = "Progress of Theoretical Physics Supplement",
issn = "2050-3911",
publisher = "Oxford University Press",
number = "3",

}

RIS

TY - JOUR

T1 - Automatic hermiticity for mixed states

AU - Nagao, Keiichi

AU - Nielsen, Holger Bech

PY - 2023/3/9

Y1 - 2023/3/9

N2 - We previously proposed a mechanism to effectively obtain, after a long time development, a Hamiltonian being Hermitian with regard to a modified inner product I-Q that makes a given non-normal Hamiltonian normal by using an appropriately chosen Hermitian operator Q. We studied it for pure states. In this letter we show that a similar mechanism also works for mixed states by introducing density matrices to describe them and investigating their properties explicitly both in the future-not-included and future-included theories. In particular, in the latter, where not only a past state at the initial time T-A but also a future state at the final time T-B is given, we study a couple of candidates for it, and introduce a "skew density matrix" composed of both ensembles of the future and past states such that the trace of the product of it and an operator O matches a normalized matrix element of O. We argue that the skew density matrix defined with I-Q at the present time t for large T-B - t and large t - T-A approximately corresponds to another density matrix composed of only an ensemble of past states and defined with another inner product I-QJ for large t - T-A.

AB - We previously proposed a mechanism to effectively obtain, after a long time development, a Hamiltonian being Hermitian with regard to a modified inner product I-Q that makes a given non-normal Hamiltonian normal by using an appropriately chosen Hermitian operator Q. We studied it for pure states. In this letter we show that a similar mechanism also works for mixed states by introducing density matrices to describe them and investigating their properties explicitly both in the future-not-included and future-included theories. In particular, in the latter, where not only a past state at the initial time T-A but also a future state at the final time T-B is given, we study a couple of candidates for it, and introduce a "skew density matrix" composed of both ensembles of the future and past states such that the trace of the product of it and an operator O matches a normalized matrix element of O. We argue that the skew density matrix defined with I-Q at the present time t for large T-B - t and large t - T-A approximately corresponds to another density matrix composed of only an ensemble of past states and defined with another inner product I-QJ for large t - T-A.

KW - PSEUDO-HERMITICITY

KW - PT-SYMMETRY

KW - FUTURE

U2 - 10.1093/ptep/ptad025

DO - 10.1093/ptep/ptad025

M3 - Journal article

VL - 2023

JO - Progress of Theoretical Physics Supplement

JF - Progress of Theoretical Physics Supplement

SN - 2050-3911

IS - 3

M1 - 031B01

ER -

ID: 341918991