High Energy Physics - Theory · arXiv:hep-th/0508140 v2 · submitted 19 Aug 2005
New Integrable System of 2dim Fermions from Strings on AdS_5 x S^5
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“Finally we show that the Hamiltonian is integrable by explicitly constructing the corresponding Lax representation.”
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Abstract
We consider classical superstrings propagating on AdS_5 x S^5 space-time. We consistently truncate the superstring equations of motion to the so-called su(1|1) sector. By fixing the uniform gauge we show that physical excitations in this sector are described by two complex fermionic degrees of freedom and we obtain the corresponding Lagrangian. Remarkably, this Lagrangian can be cast in a two-dimensional Lorentz-invariant form. The kinetic part of the Lagrangian induces a non-trivial Poisson structure while the Hamiltonian is just the one of the massive Dirac fermion. We find a change of variables which brings the Poisson structure to the canonical form but makes the Hamiltonian nontrivial. The Hamiltonian is derived as an exact function of two parameters: the total S^5 angular momentum J and string tension \lambda; it is a polynomial in 1/J and in \sqrt{\lambda'} where \lambda'=\frac{\lambda}J^2 is the effective BMN coupling. We identify the string states dual to the gauge theory operators from the closed su(1|1) sector of N=4 SYM and show that the corresponding near-plane wave energy shift computed from our Hamiltonian perfectly agrees with that recently found in the literature. Finally we show that the Hamiltonian is integrable by explicitly constructing the corresponding Lax representation.
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abstract compiled · 2026-09-23 · no language-model review
How the main claim is stated: asserted 1.00
What the abstract itself states, as probabilities: claims first 0.06 · states limitation 0.13 · human participants 0.01 · controlled comparison 0.03 · randomized assignment 0.01 · states quantitative result 0.20 · compares with prior results 0.95 · mentions code or data availability 0.02
The abstract, sentence by sentence
This table labels the abstract only (arXiv listing abstract v2). The number is the probability the classifier gave the label.
| Sentence | Role | The authors' own work | States the main conclusion | Strength |
|---|---|---|---|---|
| We consider classical superstrings propagating on AdS_5 x S^5 space-time. | background 0.82 | 0.66 | 0.02 | asserted 0.82 |
| We consistently truncate the superstring equations of motion to the so-called su(1|1) sector. | method 0.92 | 0.95 | 0.03 | asserted 1.00 |
| By fixing the uniform gauge we show that physical excitations in this sector are described by two complex fermionic degrees of freedom and we obtain the corresponding Lagrangian. | result 0.46 | 0.96 | 0.09 | asserted 1.00 |
| Remarkably, this Lagrangian can be cast in a two-dimensional Lorentz-invariant form. | result 0.94 | 0.86 | 0.13 | asserted 0.99 |
| The kinetic part of the Lagrangian induces a non-trivial Poisson structure while the Hamiltonian is just the one of the massive Dirac fermion. | result 0.99 | 0.89 | 0.07 | asserted 1.00 |
| We find a change of variables which brings the Poisson structure to the canonical form but makes the Hamiltonian nontrivial. | method 0.41 | 0.96 | 0.06 | asserted 1.00 |
| The Hamiltonian is derived as an exact function of two parameters: the total S^5 angular momentum J and string tension \lambda; it is a polynomial in 1/J and in \sqrt{\lambda'} where \lambda'=\frac{\lambda}{J^2} is the effective BMN coupling. | result 0.98 | 0.96 | 0.15 | asserted 1.00 |
| We identify the string states dual to the gauge theory operators from the closed su(1|1) sector of N=4 SYM and show that the corresponding near-plane wave energy shift computed from our Hamiltonian perfectly agrees with that recently found in the literature. | result 0.95 | 0.90 | 0.21 | asserted 1.00 |
| Finally we show that the Hamiltonian is integrable by explicitly constructing the corresponding Lax representation. | result 0.87 | 0.97 | 0.50 | asserted 1.00 |
What kind of paper the classifier reports this is: theoretical result 1.00 · evidence from proof or derivation 1.00
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Compiled by classifier-1.13-20260917 via OpenRouter, question bank abstract-p1-20260923, 2026-09-23: 1 request, 7,024 input tokens, $0.0003 reported.
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Cited by 22 Pith papers
Reviewed papers on Pith that cite this one. The full citation record
- Bethe Ansatz in Stringy Sigma Models hep-th · Mar 2006
- The AdS_5xS^5 superstring worldsheet S-matrix and crossing symmetry hep-th · Mar 2006
- Superstrings on AdS_4 x CP^3 as a Coset Sigma-model hep-th · Jun 2008
- On String S-matrix, Bound States and TBA hep-th · Oct 2007
- The AdS5xS5 Superstring in Light-Cone Gauge and its Bethe Equations hep-th · Mar 2006
- TTbar deformation and the light-cone gauge hep-th · May 2019
- Integrable S matrix, mirror TBA and spectrum for the stringy $\text{AdS}_{3}\times\text{S}^3\times\text{S}^3\times\text{S}^1$ WZW model hep-th · Dec 2018
- Twisting the Mirror TBA hep-th · Sep 2010
- Semiclassical Quantization of Spinning Strings in AdS_4 x CP^3 hep-th · Jul 2008
- The S-matrix of String Bound States hep-th · Mar 2008
- The Zamolodchikov-Faddeev Algebra for AdS_5 x S^5 Superstring hep-th · Dec 2006
- The Off-shell Symmetry Algebra of the Light-cone AdS_5 x S^5 Superstring hep-th · Sep 2006
- Finite-size Effects from Giant Magnons hep-th · Jun 2006
- On AdS_5 x S^5 String S-matrix hep-th · Apr 2006
- Green-Schwarz Strings in TsT-transformed backgrounds hep-th · Dec 2005
- Uniform Light-Cone Gauge for Strings in AdS_5 x S^5: Solving su(1|1) Sector hep-th · Oct 2005
- Wrapping interactions and a new source of corrections to the spin-chain/string duality hep-th · Oct 2005
- $T{\overline T}$, $\widetilde JJ$, $JT$ and $\widetilde JT$ deformations hep-th · Jul 2019
- The SU(1|2) and SU(2|2) Sectors from Superstrings in AdS5 x S5 hep-th · Apr 2006
- On highest-energy state in the su(1|1) sector of N=4 super Yang-Mills theory hep-th · Mar 2006
- Foundations of the AdS_5 x S^5 Superstring. Part I hep-th · Jan 2009
- Integrability of the AdS_5 x S^5 superstring and its deformations hep-th · Oct 2013
How the literature uses it
16 arXiv papers cite this in 56 sentences
Papers citing it · 31 sentences without a confident label
Contests it 1 paper
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It is not difficult to see that this remarkable scheme of cancellations would have been completely ruined had we not corrected the factor of $1/2$ missed by [ref] and the overall sign difference in comparison with by [ref] , as they were paramount for the intricate fine-tuning between the interaction terms required for $S$-matrix factorization.
Quantum integrability of the Alday-Arutyunov-Frolov model · S-matrix factorization · contest 0.95
Compares with it 3 papers
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It is important to emphasize here a significant difference in the last interacting term of our Lagrangian ([ref]) when compared to the Lagrangian (5.5) of [ref] .
Quantum integrability of the Alday-Arutyunov-Frolov model · Overview of the Alday-Arutyunov-Frolov model · 0.84
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Interestingly, the emerging reduced model appears to be completely equivalent to an integrable system arising under the corresponding consistent truncation of the$$superstring [ref] .$
Fermionic reductions of the AdS4 x CP3 superstring · Introduction · 0.98
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Interestingly, a strikingly similar result was found in the context of $5/_4$ [ref] , and it would be interesting to investigate the similarities of these two set-ups further.
Integrable S matrix, mirror TBA and spectrum for the stringy $\text{AdS}_{3}\times\text{S}^3\times\text{S}^3\times\text{S}^1$ WZW model · All-loop S matrix and asymptotic Bethe ansatz · 1.00
Cites it as background 7 papers
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In this section we review the AAF model [ref] , which emerges as a result of the consistent truncation of the superstring sigma model on $AdS_5 ×S^5$ to the $𝔰𝔲(1|1)$ sector.
Quantum integrability of the Alday-Arutyunov-Frolov model · Overview of the Alday-Arutyunov-Frolov model · 0.99
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We give here only the main formulas and definitions, and refer the reader for complete technical details to the works [ref] .
Integrable theories and generalized graded Maillet algebras · Alday-Arutyunov-Frolov model: $𝔰𝔲(1|1)$ strings in uniform gauge · 0.97
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The Alday-Arutyunov-Frolov ($AAF$) model is a purely fermionic classical integrable model arising from the reduction of the $AdS_5 ×S^5$ superstring theory to the $𝔰𝔲(1|1)$ subsector in the uniform gauge [ref] .
On the quantization of continuous non-ultralocal integrable systems · Introduction · 0.96
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