Abstract:We discuss possible phase factors for the S-matrix of planar N = 4 gauge theory, leading to modifications at four-loop order as compared to an earlier proposal. While these result in a four-loop breakdown of perturbative BMNscaling, Kotikov-Lipatov transcendentality in the universal scaling function for large-spin twist operators may be preserved. One particularly natural choice, unique up to one constant, modifies the overall contribution of all terms containing odd zeta functions in the earlier proposed scal… Show more
“…As shown in [23][24][25], this algebra is strong enough to completely determine the form of the Smatrix up to an overall multiplicative scalar factor. In Ref.…”
Section: The Centrally Extended Su(2|2) S-matrixmentioning
confidence: 97%
“…Firstly, the S-matrix (4)- (6) does not depend on the difference of the spectral parameters and in fact, it is equivalent to Shastry's R-matrix [24,27] embedding the one-dimensional Hubbard model [28]. This feature leads us to consider the approach proposed in [29,30] and subsequently considered by other authors [31].…”
Section: Double-row Transfer Matrix and Reflection Matricesmentioning
confidence: 99%
“…In this sense, the scattering of a particle with the boundaries is described by the so-called boundary S-matrices or reflection matrices, and compatibility between the boundary scattering and the bulk integrability demands the reflection matrices to satisfy reflection equations (11), (12). From the perspective of the AdS 5 × S 5 string theory, the scattering amplitudes of the world-sheet excitations are described by a S-matrix invariant relative to the centrally extended su(2|2) ⊗ su(2|2) superalgebra [23,24]. The corresponding S-matrix is fully constrained by this symmetry algebra, up to an overall multiplicative scalar factor, and it is explicitly given by…”
We derive the Bethe ansatz equations on the half line for particles interacting through factorized S-matrices invariant relative to the centrally extended su(2|2) Lie superalgebra and su(1|2) open boundaries. These equations may be of relevance for the study of the spectrum of open strings on AdS 5 × S 5 background attached to Y = 0 giant graviton branes. A one-dimensional spin chain Hamiltonian associated to this system is also derived.
“…As shown in [23][24][25], this algebra is strong enough to completely determine the form of the Smatrix up to an overall multiplicative scalar factor. In Ref.…”
Section: The Centrally Extended Su(2|2) S-matrixmentioning
confidence: 97%
“…Firstly, the S-matrix (4)- (6) does not depend on the difference of the spectral parameters and in fact, it is equivalent to Shastry's R-matrix [24,27] embedding the one-dimensional Hubbard model [28]. This feature leads us to consider the approach proposed in [29,30] and subsequently considered by other authors [31].…”
Section: Double-row Transfer Matrix and Reflection Matricesmentioning
confidence: 99%
“…In this sense, the scattering of a particle with the boundaries is described by the so-called boundary S-matrices or reflection matrices, and compatibility between the boundary scattering and the bulk integrability demands the reflection matrices to satisfy reflection equations (11), (12). From the perspective of the AdS 5 × S 5 string theory, the scattering amplitudes of the world-sheet excitations are described by a S-matrix invariant relative to the centrally extended su(2|2) ⊗ su(2|2) superalgebra [23,24]. The corresponding S-matrix is fully constrained by this symmetry algebra, up to an overall multiplicative scalar factor, and it is explicitly given by…”
We derive the Bethe ansatz equations on the half line for particles interacting through factorized S-matrices invariant relative to the centrally extended su(2|2) Lie superalgebra and su(1|2) open boundaries. These equations may be of relevance for the study of the spectrum of open strings on AdS 5 × S 5 background attached to Y = 0 giant graviton branes. A one-dimensional spin chain Hamiltonian associated to this system is also derived.
We consider the bosonic ×д¾µ sector of the maximally supersymmetric AE SYM model and show that anomalous dimension of the twist-3 single-trace composite operators built of scalar fields, recently calculated up to the four-loop order, can be generated by a compact reciprocity respecting evolution kernel.
“…Recently, using the crossing constraint [16] and transcendentality principles [17], the full form of the scalar factor was conjectured from the string [18] and gauge [19] theory points of view.…”
We prove the universality of the Hernandez-Lopez phase by deriving it from first principles. We find a very simple integral representation for the phase and discuss its possible origin from a nested Bethe ansatz structure. Hopefully, the same kind of derivation could be used to constrain higher orders of the full quantum dressing factor.
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