[PDF] Top 20 Spinning strings in AdS(5) x S**5 and integrable systems
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Spinning strings in AdS(5) x S**5 and integrable systems
... The bosonic part of the classical string action is a combination of SO(2,4) and SO(6) sigma models. The O(n) (or O(p,q)) sigma models are known to be classically integrable [8], and the same should obviously be ... See full document
49
Exact computation of one-loop correction to the energy of folded spinning string in AdS(5) x S-5
... The analytic expressions for the fluctuation determinants permitted us to carry out improved expansions in the small and large spin limit; the latter allowed us to verify that the reciprocity relations continue to be ... See full document
54
The AdS(5) x S**5 superstring in light cone gauge and its Bethe equations
... and spinning strings lim- its Arutyunov, Staudacher and one of the present authors were able to write down a set of quantum string Bethe equations [24] which are structurally very similar to the gauge ... See full document
59
The Zamolodchikov Faddeev Algebra for AdS 5 x S^5 Superstring
... the S-matrix which shares most of the usual properties of S-matrices arising in relativistic two-dimensional massive integrable ...corresponding S- matrix would not obey the usual Yang-Baxter ... See full document
41
String hypothesis for the AdS 5 x S^5 mirror
... the so-called dressing factor [17]. Its functional form was conjectured in [17] by discretizing the integral equations [18] describing classical spinning strings [19, 20], and using insights from gauge ... See full document
20
On AdS(5) x S**5 String S matrix
... dressing factor. Being universal to all sectors, it cannot be fixed by psu(2, 2 | 4) symmetry and therefore is supposed to encode dynamical information about the model. The dressing factor depends on the coupling ... See full document
11
Uniform light cone gauge for strings in AdS(5) x s**5: Solving SU(1|1) sector
... by means of constructing the Lax (zero-curvature) representation for the superstring equations of motion. In [28] we have shown that this connection admits a consistent reduction to the fields describing excitations from ... See full document
27
A search for AdS(5) X S-2 IIB supergravity solutions dual to N=2 SCFTs
... [4, 5] which relates supersymmetric quantities of four-dimensional N = 2 SCFTs to correlators in two-dimensional SCFTs [6, ...of S-duality properties of general N = 2 SCFTs have led to a better ... See full document
23
Static gauge and energy spectrum of single mode strings in AdS(5) x S 5
... impressive 5-loop order ...hidden integrable system behind the spectral problem of this AdS/CFT duality pair (for a recent review see ...excited AdS 5 × S 5 strings ... See full document
24
Superstring holography and integrability in AdS_5 x S^5
... In the previous chapter we reviewed how the problem of computing operator dimen- sions in the planar limit of large-N N = 4 SYM theory maps to that of diagonalizing the Hamiltonian of certain quantum mechanical ... See full document
271
S matrix for strings on η deformed AdS5 × S 5
... explicit spinning string solutions of the η-deformed bosonic ...η-deformed AdS a particularly interesting solution to analyse would be the GKP string and its generalisation [29, ...of AdS, ... See full document
24
Perturbative computation of string one-loop corrections to Wilson loop minimal surfaces in AdS(5) x S-5
... the s = 0 limit in the zeta-functions, which, in contrast to the examples in the previous two subsections, does not cancel out in the sum of leading-order corrections to the ... See full document
33
Comparative Analysis of Compact Spun Yarns and Ring Spun Yarns
... Although this thesis is about 2 spinning methods, we cannot draw conclusions based on yarn performance alone. It is necessary to convert these yarns in to fabrics and see how the end product performs with each ... See full document
117
The Off shell Symmetry Algebra of the Light cone AdS(5) x S**5 Superstring
... string S-matrix [3, 4, ...world-sheet S-matrix particularly involved: standard constraints on the form of S-matrix arising from the requirement of Lorentz invariance cannot be directly implemented, ... See full document
31
Precision calculation of 1/4-BPS Wilson loops in AdS(5) x S-5
... We acknowledge useful discussions with Xinyi Chen-Lin, Amit Dekel, Sergey Frolov, Simone Giombi, Jaume Gomis, Thomas Klose, Shota Komatsu, Martin Kruczenski, Daniel Medina Rincon, Diego Trancanelli, Pedro Vieira, Leo ... See full document
41
Some cubic couplings in type IIB supergravity on AdS(5) x S(5) and three point functions in SYM(4) at large N
... However, these operators will require a further modifica- tion to be consistent with all n-point functions computed in the framework of the AdS-CFT correspondence. In general, an extended CPO is the sum of a CPO ... See full document
16
Open Spinning Strings
... [25] L. N. Lipatov, High-energy asymptotics of multicolor QCD and exactly solvable lat- tice models, JETP Lett. 59 (1994) 596 [Pisma Zh. Eksp. Teor. Fiz. 59 (1994) 571] [arXiv:hep-th/9311037]; L. D. Faddeev and G. P. ... See full document
24
Quantizing three spin string solution in AdS(5) xS**5
... While the Hamiltonian is always positive in the point-like case k = 0, it is not manifestly so for k > 0, i.e. there is a potential for an instability. In general, the conclusion about non-positivity and instability ... See full document
25
Antisymmetric tensor field on AdS(5)
... (p q ˙ − H(p, q) + total derivative). Here a choice of coordinates and momenta is dictated by the transformation properties of gravity fields under isometries of AdS. In the Hamiltonian formulation the total ... See full document
6
Strings on the lattice and AdS/CFT
... the AdS boundary, on a lightlike cusped Wilson loop ...to AdS/CFT, strong coupling information on the behaviour of several important observables in the dual gauge theory and has been explicitly performed up ... See full document
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