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2024年10月30日

From geometry to non-geometry via T-duality

  • Reconsideration of the T-duality of the open string allows us to introduce some geometric features in non-geometric theories. First, we have found what symmetry is T-dual to the local gauge transformations. It includes transformations of background fields but does not include transformations of the coordinates. According to this we have introduced a new, up to now missing term, with additional gauge field AiD (D denotes components with Dirichlet boundary conditions). It compensates non-fulfilment of the invariance under such transformations on the end-points of an open string, and the standard gauge field AaN (N denotes components with Neumann boundary conditions) compensates non-fulfilment of the gauge invariance. Using a generalized procedure we will perform T-duality of vector fields linear in coordinates. We show that gauge fields AaN and AiD are T-dual to ADa and ANi respectively. We introduce the field strength of T-dual non-geometric theories as derivatives of T-dual gauge fields along both T-dual variable yμ and its double ȳμ. This definition allows us to obtain gauge transformation of non-geometric theories which leaves the T-dual field strength invariant. Therefore, we introduce some new features of non-geometric theories where field strength has both antisymmetric and symmetric parts. This allows us to define new kinds of truly non-geometric theories.
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  • [1] S. Hellerman, J. McGreevy, and B. Williams, JHEP, 01:024 (2004)
    [2] A. Dabholkar and C. Hull, JHEP, 09:054 (2003)
    [3] J. Shelton, W. Taylor, and B. Wecht, JHEP, 10:085 (2005)
    [4] Hull, JHEP, 065:0510 (2005)
    [5] Lj. Davidovic and B. Sazdovic, Eur. Phys. J. C, 74:2683 (2014)
    [6] Lj. Davidovic and B. Sazdovic, JHEP, 11:119 (2015)
    [7] Lj. Davidovic, B. Nikolic, and B. Sazdovic, Eur. Phys. J. C, 74:2734 (2014)
    [8] Lj. Davidovic, B. Nikolic, and B. Sazdovic, Eur. Phys. J. C, 75:576 (2015)
    [9] Seiber and Witten, JHEP, 032:9909 (1999)
    [10] R. J. Szabo, Int. J. Mod. Phys. A, 19:1837 (2004)
    [11] D. Lust, JHEP, 12:084 (2010)
    [12] R. Blumenhagen, A. Deser, D. Lst, E. Plauschinn, and F. Rennecke, J. Phys. A, 44:385401 (2011)
    [13] R. J. Szabo, Class. Quant. Grav., 23:R199 (2006)
    [14] B. Zwiebach, A First Course in String Theory, Second edition (Cambridge University Press, 2002), p. 673
    [15] R. G. Leigh, Mod. Phys. Lett. A, 4:2767 (1989)
    [16] J. Polchinski, String theory, Volume I, First edition (Cambridge University Press, 1998), p. 402
    [17] T. Buscher, Phys. Lett. B, 194:51 (1987); 201:466 (1988)
    [18] M. Evans and B. A Ovrut, Phys. Rev. D, 39:3016 (1989)
    [19] M. Evans and B. A Ovrut, Phys. Rev. D, 41:3149 (1990)
    [20] Lj. Davidovic and B. Sazdovic, arXiv:1806.03138
    [21] P. Bouwknegt, K. Hannabuss, and V. Mathai, Commun. Math. Phys., 264:41 (2006)
    [22] J. Brodzki, V. Mathai, J. Rosenberg, and R. J. Szabo, Commun. Math. Phys., 277:643 (2008)
    [23] R. Blumenhagen and E. Plauschinn, J. Phys. A, 44:015401 (2011).
    [24] K. Becker, M. Becker and J. Schwarz, String Theory and MTheory:A Modern Introduction, First edition (Cambridge University Press, 2007), p. 739
    [25] H. Dorn and H.-J. Otto, Phys. Lett. B, 381:81 (1996)
    [26] E. Alvarez, J. L. F. Barbon, and J. Borlaf, Nucl. Phys. B, 479:218 (1996)
    [27] A. Chatzistavrakidis, L. Jonke, and O. Leehtenfeld, JHEP, 11:182 (2015)
    [28] B. Sazdovic, Eur. Phys. J. C, 77:634 (2017)
    [29] B. Sazdovic, JHEP, 08:055 (2015)
    [30] C. Hull and B. Zwiebach, JHEP, 09:099 (2009); JHEP, 09:090 (2009)
    [31] O. Hohm, C. Hull, and B. Zwiebach, JHEP, 08:008 (2010)
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Get Citation
B. Sazdovi?. From geometry to non-geometry via T-duality[J]. Chinese Physics C, 2018, 42(8): 083106. doi: 10.1088/1674-1137/42/8/083106
B. Sazdovi?. From geometry to non-geometry via T-duality[J]. Chinese Physics C, 2018, 42(8): 083106.  doi: 10.1088/1674-1137/42/8/083106 shu
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Received: 2018-02-12
Revised: 2018-05-24
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    Supported by the Serbian Ministry of Education and Science (171031)

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From geometry to non-geometry via T-duality

Fund Project:  Supported by the Serbian Ministry of Education and Science (171031)

Abstract: Reconsideration of the T-duality of the open string allows us to introduce some geometric features in non-geometric theories. First, we have found what symmetry is T-dual to the local gauge transformations. It includes transformations of background fields but does not include transformations of the coordinates. According to this we have introduced a new, up to now missing term, with additional gauge field AiD (D denotes components with Dirichlet boundary conditions). It compensates non-fulfilment of the invariance under such transformations on the end-points of an open string, and the standard gauge field AaN (N denotes components with Neumann boundary conditions) compensates non-fulfilment of the gauge invariance. Using a generalized procedure we will perform T-duality of vector fields linear in coordinates. We show that gauge fields AaN and AiD are T-dual to ADa and ANi respectively. We introduce the field strength of T-dual non-geometric theories as derivatives of T-dual gauge fields along both T-dual variable yμ and its double ȳμ. This definition allows us to obtain gauge transformation of non-geometric theories which leaves the T-dual field strength invariant. Therefore, we introduce some new features of non-geometric theories where field strength has both antisymmetric and symmetric parts. This allows us to define new kinds of truly non-geometric theories.

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