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《中国物理C》(英文)编辑部
2024年10月30日

Classical mechanics in non-commutative phase space

  • In this paper the laws of motion of classical particles have been investigated in a non-commutative phase space. The corresponding non-commutative relations contain not only spatial non-commutativity but also momentum non-commutativity. First, new Poisson brackets have been defined in non-commutative phase space. They contain corrections due to the non-commutativity of coordinates and momenta. On the basis of this new Poisson brackets, a new modified second law of Newton has been obtained. For two cases, the free particle and the harmonic oscillator, the equations of motion are derived on basis of the modified second law of Newton and the linear transformation (Phys. Rev. D, 2005, 72: 025010). The consistency between both methods is demonstrated. It is shown that a free particle in commutative space is not a free particle with zero-acceleration in the non-commutative phase space, but it remains a free particle with zero-acceleration in non-commutative space if only the coordinates are non-commutative.

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  • [1] . LI K, WANG J H, CHEN C Y. Modern Physics Letter A,2005, 20: 342. Connes A, Douglas M R, Schwarz A. JHEP, 1998, 9802:003. hep-th/97111623. Douglas M R, Hull C M. JHEP, 1998, 9802: 008. hep-th/97111654. Ardalan F, Arfaei H, Sheikh-Jabbari M M. JHEP, 1999,9902: 016. hep-th/98100725. Seiberg N, Witten E. JHEP, 1999, 9909: 032. hep-th/99081426. CHU C S, Ho P M. Nucl. Phys. B, 1999, 550: 151.hep/98122197. CHU C S, Ho P M. Nucl. Phys. B, 2000, 568: 447.hep/99061928. Ardalan F, Arfaei H, Sheikh-Jabbari M M. Nucl. Phys. B,2000, 576: 578. hep/99061919. Ezawa Z F. Quantum Hall Effects: Field Theoretical Approach and Related Topics. Singapore: World Scientific,200010. Minwalla S, Raamsdonk M V, Seiberg N. JHEP, 2000,0002: 020. hep-th/991207211. LONG Z W, JING J. Phys. Lett. B, 2003, 560: 12812. Chaichain M, Sheikh-Jabbari M M, Tureanu A. Phys. Rev.Lett., 2001, 86: 271613. Bellucci S, Nersessian A, Sochichiu C. Phys. Lett. B, 2001,522: 34514. Romero J M, Santiago J A, Vergara J D. Phys. Lett. A,2003, 310: 915. Bertolami O, Rosa J G. Phys. Rev. D, 2005, 72: 02501016. ZHANG J Z. Phys. Lett. B, 2004, 597: 36217. Mirza B, Dehghani M. Commun. Theor. Phys., 2004, 42:18318. FEI S M, GUO H Y. J. Phys. A, 1991, 24: 119. CHANG Z, CHEN W, GUO H Y et al. J. Phys. A, 1991,24: 142720. CHANG Z, CHEN W, GUO H Y. J. Phys. A, 1990, 23:418521. CHANG Z, FEI S M, GUO H Y et al. J. Phys. A, 1991,23: 537122. CHANG Z, FEI S M, GUO H Y et al. J. Phys. A, 1991,24: 543523. CHANG Z. Phys. Rep., 1995, 262: 137
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Get Citation
WEI Gao-Feng, LONG Chao-Yun, LONG Zheng-Wen, QIN Shui-Jie and FU Qiang. Classical mechanics in non-commutative phase space[J]. Chinese Physics C, 2008, 32(5): 338-341. doi: 10.1088/1674-1137/32/5/002
WEI Gao-Feng, LONG Chao-Yun, LONG Zheng-Wen, QIN Shui-Jie and FU Qiang. Classical mechanics in non-commutative phase space[J]. Chinese Physics C, 2008, 32(5): 338-341.  doi: 10.1088/1674-1137/32/5/002 shu
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Received: 2007-06-29
Revised: 2007-09-26
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Classical mechanics in non-commutative phase space

    Corresponding author: WEI Gao-Feng,

Abstract: 

In this paper the laws of motion of classical particles have been investigated in a non-commutative phase space. The corresponding non-commutative relations contain not only spatial non-commutativity but also momentum non-commutativity. First, new Poisson brackets have been defined in non-commutative phase space. They contain corrections due to the non-commutativity of coordinates and momenta. On the basis of this new Poisson brackets, a new modified second law of Newton has been obtained. For two cases, the free particle and the harmonic oscillator, the equations of motion are derived on basis of the modified second law of Newton and the linear transformation (Phys. Rev. D, 2005, 72: 025010). The consistency between both methods is demonstrated. It is shown that a free particle in commutative space is not a free particle with zero-acceleration in the non-commutative phase space, but it remains a free particle with zero-acceleration in non-commutative space if only the coordinates are non-commutative.

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