2006
DOI: 10.1088/1126-6708/2006/07/014
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On the Dynamics of finite-gap solutions in classical string theory

Abstract: We study the dynamics of finite-gap solutions in classical string theory on R × S 3 . Each solution is characterised by a spectral curve, Σ, of genus g and a divisor, γ, of degree g on the curve. We present a complete reconstruction of the general solution and identify the corresponding moduli-space, M (2g) R , as a real symplectic manifold of dimension 2g. The dynamics of the general solution is shown to be equivalent to a specific Hamiltonian integrable system with phase-space M (2g) R . The resulting descri… Show more

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Cited by 81 publications
(219 citation statements)
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“…This is the main idea of the Pohlmeyer reduction [59] which we rederive here as it applies to our particular problem. Similar considerations in the context of string theory are well-known, for example see [32][33][34][35][36][37][38][39][40][41][43][44][45][46][47][48][49][50][51][52][53][54][55][56][57] and [60].…”
Section: Jhep11(2014)065mentioning
confidence: 81%
See 1 more Smart Citation
“…This is the main idea of the Pohlmeyer reduction [59] which we rederive here as it applies to our particular problem. Similar considerations in the context of string theory are well-known, for example see [32][33][34][35][36][37][38][39][40][41][43][44][45][46][47][48][49][50][51][52][53][54][55][56][57] and [60].…”
Section: Jhep11(2014)065mentioning
confidence: 81%
“…To find solutions in all those cases it is important to exploit the integrability properties of the equations of motion which are the same as those of the closed string. Recently, in the case of closed, Euclidean, plane Wilson loops (with constant scalar) an infinite parameter family of analytical solutions was found using Riemann theta functions [28,29] following results from the mathematical literature [30,31] and from previous results for closed strings [32][33][34][35][36][37][38][39][40][41]. This integrability construction for the Wilson loop was further discussed in [42] and also in [43][44][45][46][47][48][49][50][51][52][53][54][55][56][57].…”
Section: Jhep11(2014)065mentioning
confidence: 99%
“…For the AdS 5 × S 5 [16,17,[63][64][65][66][67][68] and AdS 4 × CP 3 [21] backgrounds the finite-gap method yields a set of coupled integral equations, which on the one hand parameterize possible classical solutions of the sigmamodel and on the other hand can be regarded as the classical limit of the Bethe equations for the quantum spectrum of the string. We first describe the general scheme of finite-gap integration, as applied to the 4 cosets, and then specify the general construction to the case at hand, the sigma model on AdS 3 × S 3 × S 3 × S 1 .…”
Section: Jhep03(2010)058mentioning
confidence: 99%
“…We can define the current 14) which is invariant under the global symmetry and, under the local symmetry transform as…”
Section: Equations Of Motionmentioning
confidence: 99%