2009
DOI: 10.1088/1126-6708/2009/10/019
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Strings on the deformedT1,1: giant magnon and single spike solutions

Abstract: In this paper we have found giant magnon and single spike string solutions in a sector of the gamma-deformed conifold. We examined the dispersion relations and find a behavior analogous to the undeformed case. The transcendental functional relations between the conserved charges are shifted by a certain gamma-dependent term. The latter is proportional to the total momentum and thus qualitatively different from known cases.

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Cited by 10 publications
(16 citation statements)
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“…We refer to this equation as the pulsating condition. For Z we have the solution 40) which shows that Z is a constant, as it should be, due to the ansatz (3.37). The equation for θ becomes…”
Section: )mentioning
confidence: 99%
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“…We refer to this equation as the pulsating condition. For Z we have the solution 40) which shows that Z is a constant, as it should be, due to the ansatz (3.37). The equation for θ becomes…”
Section: )mentioning
confidence: 99%
“…Pulsating strings were first introduced in [29] and later on were generalized by [30][31][32]. Since then there have been further examples of pulsating strings, both in AdS and non-AdS backgrounds [33][34][35][36][37][38][39][40][41][42][43][44][45][46]. In this section we give a brief review on the pulsating string solution obtained in [29].…”
Section: Pulsating Strings In Ads/cft Correspondencementioning
confidence: 99%
“…In [9] we considered the case of infinite charges. In contrast to this case the finite size corrections originate from the expression…”
Section: Finite Size Analysis Setupmentioning
confidence: 99%
“…Since we assume ǫ ≪ 1 and thus the energy density E being very large, we see that the coefficient ∆ E produces the leading part of the correction and the ∆ 1 the subleading one. Expressing ∆ − 1 2 (J φ + J ψ ) γ from (25) in a concise form [9] we obtain…”
Section: Giant Magnonmentioning
confidence: 99%
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