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The Schmidt Decomposition for Entangled System and Nonadiabatic Berry Phases

Received: 16 July 2024     Accepted: 12 August 2024     Published: 31 October 2024
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Abstract

The time-dependent Hamiltonians are a very important portion in the modeling of real systems. In fact, the dynamic description of an entangled quantum systems is reflected in full coherence with the resolution of a wave function, solution of the Schrödinger equation throughout the entire study path. In this regard, we specify in this paper the system of two-site Bose-Hubbard model that obeys tunnel behavior, as two coupled harmonic oscillators, to examine quantum entanglement. The dynamics of such a system is described by the Schrödinger equation have introduced to the solution, the non-linear Ermakov equations as well as through a passage to the Heisenberg picture approach and the general Lewis and Riesenfeld invariant method compute between coupled harmonic oscillators and the coupled Caldirola Kanai oscillators. We prove that a time exponential increase in the mass of the system brings back to an exponential increase of entanglement and the Heisenberg picture approach is the most stable method to quantum entanglement because, this last has reached very large values. Also, we specify a cyclic time evolution, we find analytically the nonadiabatic Berry phases. In a particular case, such an entangled system acquired a nonadiabatic Berry phases that exhibits the same behavior as the Schmidt parameter.

Published in American Journal of Physics and Applications (Volume 12, Issue 2)
DOI 10.11648/j.ajpa.20241202.12
Page(s) 27-39
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This is an Open Access article, distributed under the terms of the Creative Commons Attribution 4.0 International License (http://creativecommons.org/licenses/by/4.0/), which permits unrestricted use, distribution and reproduction in any medium or format, provided the original work is properly cited.

Copyright

Copyright © The Author(s), 2024. Published by Science Publishing Group

Keywords

Two-site Bose-Hubbard Model, Schmidt Mode, Entanglement, Nonadiabatic Berry Phases

References
[1] H-P. Breuer, E-M. Laine, J. Piilo, B. Vacchini: Non-Markovian dynamics in open quantum systems, Rev. Mod. Phys. 88, 021002 (2016),
[2] W. W. Hu, R-G. Zhou, X. Li, P. Fan, C. Y. Tan: A novel dynamic quantum secret sharing in high-dimensional quantum system, Quant. Info. Proc. 20, 159 (2021),
[3] S-N. Sun, M. Motta, R. N. Tazhigulov, A. T. K. Tan, G. K-L Chan, A. J. Minnich: Quantum Computation of Finite-Temperature Static and Dynamical Properties of Spin Systems Using Quantum Imaginary Time Evolution, PRX Quant. 2, 010317 (2021),
[4] R. J. Lewis-Swan, A. Safavi-Naini, A. M. Kaufman, A. M. Rey: Dynamics of quantum information, Nat. Rev. Phys. 1, 627 − 634 (2019),
[5] A. Lerose, S. Pappalardi: Bridging entanglement dynamics and chaos in semiclassical systems, Phys. Rev. A. 102, 032404 (2020),
[6] A. Nahum, J. Ruhman, S. Vijay, J. Haah: Quantum Entanglement Growth under Random Unitary Dynamics, Phys. Rev. X. 7, 031016 (2017),
[7] M. Ippoliti, V. Khemani: Postselection-Free Entanglement Dynamics via Spacetime Duality, Phys. Rev. Lett. 126, 060501 (2021),
[8] P. Shor: in Proceedings of the 35th Annual Symposium on Foundations of Computer Science, IEEE Computer Society Press, Los Alamitos, CA, 116123 (1994),
[9] X.Liu, L.Yu, P.Hu: New entanglement-assisted quantum codes from k-Galois dual codes, Elsevier. 55, 21 − 32 (2019),
[10] A. K. Ekert: Quantum Cryptography Based on Bell’s Theorem, Phys. Rev. Lett. 126, 060501 (2021),
[11] F. Gao, S. Qin, W. Huang, Q. Wen: Quantum private query: A new kind of practical quantum cryptographic protocol, Sc. Chin. Phys, Mec. Ast, 62 70301 (2019),
[12] Z-H. Yan, J-L. Qin, Z-Z. Qin, X-L. Su, X-J. Jia, C- DeXie, K-C. Peng: Generation of non-classical states of light and their application in deterministic quantum teleportation, Phys. Rev. Lett. 1, 43 − 49 (2021),
[13] L. Gao, S. J Harris, M. Junge: Quantum Teleportation and Super-Dense Coding in Operator Algebras, Phys. Rev. Lett. 2021, 9146 − 9179 (2019),
[14] R. Requist, E. K. U. Gross: Approximate formula for the macroscopic polarization including quantum fluctuations, J. Phys. Chem. Lett. 9, 7045 (2018),
[15] R. Requist, E. K. U. Gross: Accurate Formula for the Macroscopic Polarization of Strongly Correlated Materials, J. Phys. Chem. Lett. 9, 24, 70457051 (2018),
[16] M. Kohmoto: Topological Invariant and the Quantization of the Hall Conductance, An. Phys. 160,, 343 − 354 (1985),
[17] B. Dey, P. Kapri, O. Pal, T. K. Ghosh: Unconventional phases in a Haldane model of dice lattice, Phys. Rev. B. 101, 235406 (2020),
[18] Y. Aharonov, J. Anandan: Phase change during a cyclic quantum evolution, Phys. Rev. Lett. 58, 1593 (1987),
[19] G. Dattoli, R. Mignani, A. Torre: Geometrical phase in the cyclic evolution of non-Hermitian systems, J. Phys. A: Math. Gen. 23, 5795 (1990),
[20] Y. Singhal, E. Martello, S. Agrawal, T. Ozawa, H. Price, B. Gadway: Measuring the Adiabatic Non- Hermitian Berry Phase in Feedback-Coupled Oscillators, arXiv preprint arXiv, cond-mat. 5, 3 (2023),
[21] S. Campbell, G. D. Chiara, M. Paternostro: Equilibration and nonclassicality of a double-well potential, Sc. Rep. 6, 19730 (2016),
[22] M. A. Lohe: Exact time dependence of solutions to the time-dependent Schrödinger equation, J. Phys. A: Math. Theor. 42, 035307 (2009),
[23] J. L. Reid: An exact solution of the nonlineair differential equation,Pro. Amer. Math. Soc. 27, 61 − 62 (1971),
[24] S. Ghosh, K. S. Gupta and Sh. C. L. Srivastava: Entanglement dynamics following a sudden quench: An exact solution, epl. 120, 5 (2017),
[25] D. Park: Dynamics of entanglement and uncertainty relation in coupled harmonic oscillator system: exact results, Quant Inf. Proc. 17, 147 (2018),
[26] E. Pinney: The nonlinear differential equation, Proc. Am. Math. Soc. 1, 681 (1950).
[27] A. Ekert, P. L. Knight: Entangled quantum systems and the Schmidt decomposition, Am. J. Phys. 63, 415 (1995),
[28] A. Acin, A. Andrianov, L. Costa, E. Jané, J. I. Latorre, R. Tarrach: Generalized Schmidt Decomposition and Classification of Three-Quantum- Bits States, Phys. Rev. Lett. 7, 85 (2000),
[29] D. N. Makarov: High Intensity Generation of Entangled Photons in a Two Mode Electromagnetic Field, Wiley- Vch. 529, 10(2017),
[30] D. N. Makarov: Coupled harmonic oscillators and their quantum entanglement, Phys. Rev. E. 97, 042203 (2018),
[31] D. N. Makarov: Quantum entanglement of a harmonic oscillator with an electromagnetic field, Sc. Rep. 8, 8204 (2018),
[32] D. M. Tong, E. Sjöqvist, L. C. Kwek, C. H. Oh, M. Ericsson: Relation between geometric phases of entangled bipartite systems and their subsystems, Phys. Rev. A. 68, 022106 (2003),
[33] H. Casini, M. Huerta: Entanglement entropy in free quantum field theory,. Phys. A: Math. Theor. 42, 504007 (2009),
[34] C. H. Bennett, H. J. Bernstein, S. Popescu, B. Schumacher: Concentrating partial entanglement by local operations, Phys. Rev. A. 4, 53 (1996),
[35] M. V. Fedorova, N. I. Miklinb: Schmidt modes and entanglement, Cont. Phys. 55, 94 − 109 (2014),
[36] A. Yu. Bogdanov, Yu. I. Bogdanov, K. A. Valiev: Schmidt Modes and Entanglement in Continuous- Variable Quantum Systems, Russ. Microelec. 35, 7-20 (2006),
[37] M. V. Berry: The quantum phase, five years after, Geometric phases in physics phas.ubc.ca. (1989).
[38] S. Oh, Z. Huang, U. Peskin, S. Kais: Entanglement, Berry phases, and level crossings for the atomic Breit- Rabi Hamiltonian, Phys. Rev. A. 78, 062106 (2008),
[39] S. Ryu, Y. Hatsugai: Entanglement entropy and the Berry phase in the solid state, Phys. Rev. B. 73, 245115 (2006),
[40] I. A. Pedrosa, G. P. Serra, I. Guedes: Wave functions of a time-dependent harmonic oscillator with and without a singular perturbation, Phys. Rev. A. 56, 5 (1997),
[41] J-Y. Ji, J. K. Kim, S. P. Kim, K-S Soh: Exact wave functions and nonadiabatic Berry phases of a time- dependent harmonic oscillator, Phys. Rev. A. 52, 3352 (1995),
[42] J-Y. Ji, J. K. Kim, S. P. Kim: Heisenberg-picture approach to the exact quantum motion of a time- dependent harmonic oscillator, Phys. Rev. A. 51, 4268 (1995),
[43] J. R. Ackerhalt, K. RzaZewski: Heisenberg-picture operator perturbation theory, Phys. Rev. A. 12, 2549 (1975),
[44] S. P Kim: A class of exactly solved time-dependent quantum harmonic oscillators, J. Phys. A: Math. Gen. 27, 3927 (1994),
[45] A. Abidi, A. Trabelsi, S. Krichene: Coupled harmonic oscillators and their application in the dynamics of entanglement and the nonadiabatic Berry phases, Can.J.Phys. 99, 10 (2021),
[46] A. Abidi, A. Trabelsi: Dynamics of entanglement in coherent states, entangled Schrödinger cat state and distribution function, Rep. Math. Phys. 90, 123 − 140 (2022),
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  • APA Style

    Abidi, A., Trabelsi, A. (2024). The Schmidt Decomposition for Entangled System and Nonadiabatic Berry Phases. American Journal of Physics and Applications, 12(2), 27-39. https://doi.org/10.11648/j.ajpa.20241202.12

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    ACS Style

    Abidi, A.; Trabelsi, A. The Schmidt Decomposition for Entangled System and Nonadiabatic Berry Phases. Am. J. Phys. Appl. 2024, 12(2), 27-39. doi: 10.11648/j.ajpa.20241202.12

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    AMA Style

    Abidi A, Trabelsi A. The Schmidt Decomposition for Entangled System and Nonadiabatic Berry Phases. Am J Phys Appl. 2024;12(2):27-39. doi: 10.11648/j.ajpa.20241202.12

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  • @article{10.11648/j.ajpa.20241202.12,
      author = {Ahlem Abidi and Adel Trabelsi},
      title = {The Schmidt Decomposition for Entangled System and Nonadiabatic Berry Phases},
      journal = {American Journal of Physics and Applications},
      volume = {12},
      number = {2},
      pages = {27-39},
      doi = {10.11648/j.ajpa.20241202.12},
      url = {https://doi.org/10.11648/j.ajpa.20241202.12},
      eprint = {https://article.sciencepublishinggroup.com/pdf/10.11648.j.ajpa.20241202.12},
      abstract = {The time-dependent Hamiltonians are a very important portion in the modeling of real systems. In fact, the dynamic description of an entangled quantum systems is reflected in full coherence with the resolution of a wave function, solution of the Schrödinger equation throughout the entire study path. In this regard, we specify in this paper the system of two-site Bose-Hubbard model that obeys tunnel behavior, as two coupled harmonic oscillators, to examine quantum entanglement. The dynamics of such a system is described by the Schrödinger equation have introduced to the solution, the non-linear Ermakov equations as well as through a passage to the Heisenberg picture approach and the general Lewis and Riesenfeld invariant method compute between coupled harmonic oscillators and the coupled Caldirola Kanai oscillators. We prove that a time exponential increase in the mass of the system brings back to an exponential increase of entanglement and the Heisenberg picture approach is the most stable method to quantum entanglement because, this last has reached very large values. Also, we specify a cyclic time evolution, we find analytically the nonadiabatic Berry phases. In a particular case, such an entangled system acquired a nonadiabatic Berry phases that exhibits the same behavior as the Schmidt parameter. },
     year = {2024}
    }
    

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  • TY  - JOUR
    T1  - The Schmidt Decomposition for Entangled System and Nonadiabatic Berry Phases
    AU  - Ahlem Abidi
    AU  - Adel Trabelsi
    Y1  - 2024/10/31
    PY  - 2024
    N1  - https://doi.org/10.11648/j.ajpa.20241202.12
    DO  - 10.11648/j.ajpa.20241202.12
    T2  - American Journal of Physics and Applications
    JF  - American Journal of Physics and Applications
    JO  - American Journal of Physics and Applications
    SP  - 27
    EP  - 39
    PB  - Science Publishing Group
    SN  - 2330-4308
    UR  - https://doi.org/10.11648/j.ajpa.20241202.12
    AB  - The time-dependent Hamiltonians are a very important portion in the modeling of real systems. In fact, the dynamic description of an entangled quantum systems is reflected in full coherence with the resolution of a wave function, solution of the Schrödinger equation throughout the entire study path. In this regard, we specify in this paper the system of two-site Bose-Hubbard model that obeys tunnel behavior, as two coupled harmonic oscillators, to examine quantum entanglement. The dynamics of such a system is described by the Schrödinger equation have introduced to the solution, the non-linear Ermakov equations as well as through a passage to the Heisenberg picture approach and the general Lewis and Riesenfeld invariant method compute between coupled harmonic oscillators and the coupled Caldirola Kanai oscillators. We prove that a time exponential increase in the mass of the system brings back to an exponential increase of entanglement and the Heisenberg picture approach is the most stable method to quantum entanglement because, this last has reached very large values. Also, we specify a cyclic time evolution, we find analytically the nonadiabatic Berry phases. In a particular case, such an entangled system acquired a nonadiabatic Berry phases that exhibits the same behavior as the Schmidt parameter. 
    VL  - 12
    IS  - 2
    ER  - 

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Author Information
  • National Higher School of Engineers of Tunis, Tunis University, Tunisia; Department of Physics, Faculty of Sciences of Tunis, Tunis El Manar University, Tunis, Tunisia

  • National Center for Nuclear Science and Technology Technological Pole, Sidi Thabet, Tunisia

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