ADS(5) X S-5
On AdS(5) x S**5 String S matrix
... the S-matrix is not ...The S-matrix for the model can be determined by using the symmetry algebra (and choosing properly its representation) up to a scalar factor ...
11
Static gauge and energy spectrum of single mode strings in AdS(5) x S 5
... First we consider the static gauge approach to string dynamics in a generic static space-time. We use only a part of the constraints to exclude the time components of the canonical variables. This relates the energy ...
24
Perturbative computation of string one-loop corrections to Wilson loop minimal surfaces in AdS(5) x S-5
... Another example will be the 1-loop partition function for the surface ending on the k-wound circle that should be representing the k-fundamental circular Wilson loop [3, 46]. Here the gauge theory result is a ...
33
Exact computation of one-loop correction to the energy of folded spinning string in AdS(5) x S-5
... As we shall explicitly show in Section 5 below, the effective action in the static gauge given by the sum of (3.15) and (3.11) is indeed UV finite. Moreover, we shall also verify the relation (3.17), i.e. ...
54
Precision calculation of 1/4-BPS Wilson loops in AdS(5) x S-5
... other procedures (e.g. heat kernel [11]), this method of regularizing determinants effectively introduces a fictitious boundary for the worldsheet surface, besides the expected conformal one. We then proceed with the ...
41
The Off shell Symmetry Algebra of the Light cone AdS(5) x S**5 Superstring
... the off-shell theory by relaxing the level-matching condition and take the limit of infinite light-cone momentum, which decompactifies the string world-sheet. We fo- cus on the psu(2 | 2) ⊕ psu(2 | 2) subalgebra which ...
31
The AdS(5) x S**5 superstring in light cone gauge and its Bethe equations
... One can easily see that the uniform light-cone gauge quartic Hamiltonian (5.16) is considerably simpler than the quartic Hamiltonian obtained by Calan et. al.[19], though still rather involved. An important property of ...
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Scalar quartic couplings in type IIB supergravity on AdS(5) x S(5)
... It is obvious that the cubic couplings found in [6, 7] obey the consistency condition allowing therefore truncation to the fields from the massless multiplet at the level of the cubic action. In this paper we show that ...
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Some cubic couplings in type IIB supergravity on AdS(5) x S(5) and three point functions in SYM(4) at large N
... the s I -dependent quartic terms and all cubic terms that involve two scalar fields s I ...scalars s I with symmetric tensor fields of the second rank coming from the AdS 5 components ...
16
Superstrings on AdS 4 x CP^3 as a Coset Sigma model
... one can develop semiclassical quantization to verify whether classical integrability is preserved by leading quantum corrections. Then, the subalgebra su(2 | 2) of the global symmetry algebra OSP(2, 2 | 6) which leaves ...
29
Superstring holography and integrability in AdS_5 x S^5
... As noted above, the matching achieved by BMN should not be confined to the Penrose (or large-radius) limit of the bulk theory, or to the large R-charge limit of the CFT. When the Penrose limit is lifted, finite-radius ...
271
A search for AdS(5) X S-2 IIB supergravity solutions dual to N=2 SCFTs
... Finally, before moving onto the general case, we remark that multiple Killing directions also appeared in [33], and, in particular, the Lie derivative of a similar S 2 warp-factor with respect to one Killing ...
23
Uniform light cone gauge for strings in AdS(5) x s**5: Solving SU(1|1) sector
... We are grateful to F. Alday, N. Dorey, J. Plefka, M. Staudacher, A. Tseytlin and M. Zamaklar for many valuable discussions. G. A. would like to thank Emery Sokatchev and Laboratoire d’Annecy-Le-Vieux de Physique ...
27
Foundations of the AdS 5 x S^5 Superstring Part I
... fixed string sigma models are equivalent for different choices of a uniform gauge, i.e. for different values of a, provided the level-matching condition is satisfied. String configurations which violate the ...
164
Semiclassical quantization of rotating superstring in AdS(5) x S**5
... section 5 we have determined the Lagrangian for small fluctuations near the solution ...the S = 0, J 6 = 0 solution discussed in section 4 where the bosonic ...the AdS 5 rotating case, ...
36
Giant magnons in TsT transformed AdS 5 x S^5
... off-shell, that is if one does not impose the level-matching condition then the de- formed string model is indistinguishable from the undeformed one, and they share the same magnon dispersion relation [18], the su (2 | ...
21
String hypothesis for the AdS 5 x S^5 mirror
... w (α) k of the second and third levels of the nested Bethe ansatz, and α = 1, 2 because the scattering matrix is the tensor product of the two su(2 | 2)-invariant S-matrices. We will often refer to K’s as to ...
20
Quadratic action for type IIB supergravity on AdS(5) x S(5)
... The AdS/CFT correspondence has already been used in [10]-[24] to compute some two- and three-point Green functions up to normalization constants, and some preliminary results on four-point Green functions have ...
16
Spinning strings in AdS(5) x S**5 and integrable systems
... It would be very important to try to go beyond semiclassics and identify the string states and field-theoretic operators for small values of the spins and energy (dimension). One possible direction could be to develop a ...
49
Thermodynamic Bethe Ansatz for the AdS 5 x S^5 Mirror Model
... We also see a certain difference with the findings of [52]. First of all, none of the TBA kernels in [52] seem to contain the (square root) of the ratio x(u + i/gQ)/x(u − i/gQ), while our kernels K ± Qy do. ...
32