[PDF] Top 20 The AdS(5) x S**5 superstring in light cone gauge and its Bethe equations
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The AdS(5) x S**5 superstring in light cone gauge and its Bethe equations
... all-loop Bethe ansatz conjectures on the gauge theory side and aware of the obtained data in the plane wave, flat space and spinning strings lim- its Arutyunov, Staudacher and one of the present ... See full document
59
The Off shell Symmetry Algebra of the Light cone AdS(5) x S**5 Superstring
... string S-matrix [3, 4, ...world-sheet gauge choice is the so-called generalised uniform light-cone gauge [8, ...this gauge are closely related to the spin chain excitation ... See full document
31
Uniform light cone gauge for strings in AdS(5) x s**5: Solving SU(1|1) sector
... N gauge and string theories, and, in particular, into the AdS/CFT duality conjecture ...corresponding Bethe ansatz whose solutions encode the spectrum of the ...the Bethe equations can ... See full document
27
Exact computation of one-loop correction to the energy of folded spinning string in AdS(5) x S-5
... integral equations, having as guiding principle the gauge theory information implying a description in terms of an asymptotic Bethe Ansatz ...the Bethe Ansatz result for the 1-loop correction ... See full document
54
String hypothesis for the AdS 5 x S^5 mirror
... the light-cone string model is not Lorentz-invariant, the mirror theory is governed by a different Hamiltonian and therefore has very different ...the Bethe-Yang equations for fundamental ... See full document
20
Static gauge and energy spectrum of single mode strings in AdS(5) x S 5
... static gauge X 0 ∼ Eτ for the AdS-string is that the worldsheet Hamiltonian density is polynomial in the fields, independent of the worldsheet space coordinate σ and in fact proportional to the ... See full document
24
Simplified TBA equations of the AdS 5 x S^5 mirror model
... TBA equations for the ground state of the light-cone superstring were derived in ...and its general solution has been con- structed in ...(TBA-like) equations for excited states ... See full document
17
Thermodynamic Bethe Ansatz for the AdS 5 x S^5 Mirror Model
... with its mirror. The light-cone gauge string sigma model lacks two-dimensional Lorentz invariance and, for this reason, the corresponding mirror model is a new theory that requires a separate ... See full document
32
Giant magnons in TsT transformed AdS 5 x S^5
... the light-cone Hamiltonian on the deformation param- eters disappears because in this limit all physical fields must vanish at the space infinity 1 ...the light-cone gauge-fixed string ... See full document
21
On AdS(5) x S**5 String S matrix
... the Bethe equations should be abandoned for di- rect diagonalization of a short-range Hubbard type Hamiltonian ...string Bethe equations turn into the gauge theory asymptotic ... See full document
11
Quadratic action for type IIB supergravity on AdS(5) x S(5)
... covariant equations of motion for type IIB supergravity [1, 2, 3] can not be derived from any action because of the presence of a self-dual ...at equations of motion which are not manifestly covariant but ... See full document
16
Super spin chain coherent state actions and $AdS_5 \times S^5$ superstring
... IIB superstring action [8] and to show that a fermionic action equivalent to the one found from the spin chain in the previous section emerges from it in the “fast-string” limit, thus generalizing the observations ... See full document
34
Foundations of the AdS 5 x S^5 Superstring Part I
... the light-cone string sigma model is not Lorentz-invariant, the mirror model is governed by a different Hamiltonian and therefore has very different ...the Bethe- Yang equations for the mirror ... See full document
164
On regularizing the AdS superstring worldsheet
... conformal gauge with the so-called AdS lightcone gauge, where the light-cone is entirely in AdS ...the AdS lightcone gauge-fixed action derived via double ... See full document
26
Superstring holography and integrability in AdS_5 x S^5
... the Bethe ansatz) have proved useful in this context (for a general review of the Bethe ansatz method, see ...the Bethe ansatz. For three- or higher-impurity operators, however, the Bethe ... See full document
271
Perturbative computation of string one-loop corrections to Wilson loop minimal surfaces in AdS(5) x S-5
... Below we will also test our perturbative approach based on constructing heat kernels for 2d fluctuation operators in an expansion in a small parameter on two other examples. The first will be the near-BPS limit of the ... See full document
33
PP-Wave Light-Cone Superstring Field Theory
... Following earlier work on maximally supersymmetric solutions of eleven-dimensional supergrav- ity [1, 2, 3], a new maximally supersymmetric solution of Type IIB supergravity [4] was found. This paved the way for ... See full document
32
Scale invariance of the η deformed AdS<inf>5</inf>à S5 superstring, T duality and modified type II equations
... vectors X = Z + I and Y that these equations are satisfied by the ABF ...supergravity equations of the R–R fluxes that is “driven” by the special isometry vector I and which are satisfied by the ABF ... See full document
42
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
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
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