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We consider the action of the $q$-deformed Poincar\'e superalgebra on the massless non-relativistic R-matrix in ordinary (undeformed) integrable $AdS_2 \times S^2 \times T^6$ type IIB superstring theory. The boost generator acts…

High Energy Physics - Theory · Physics 2022-10-12 Andrea Fontanella , Alessandro Torrielli

All symmetric space $AdS_n$ solutions of type II supergravity have recently been found for $n>2$. For the supersymmetric solutions (and their T-duals) it is known that the Green-Schwarz string is classically integrable. We complete the…

High Energy Physics - Theory · Physics 2018-04-04 Linus Wulff

Modern on-shell methods allow us to construct both the classical and quantum S-matrix for a large class of theories, without utilizing knowledge of the interacting Lagrangian. It was recently shown that the same applies for chiral gauge…

High Energy Physics - Theory · Physics 2014-02-28 Wei-Ming Chen , Yu-tin Huang , David A. McGady

The possibility of adding an SU(2) horizontal symmetry to the 331 model is studied. It is found that simple, anomaly-free fermion assignments can be made which lead to plausible results for fermion masses and mixings. In particular, all…

High Energy Physics - Phenomenology · Physics 2009-10-31 M. B. Tully , G. C. Joshi

Yang Mills theory in 2+1 dimensions can be expressed as an array of coupled (1+1)-dimensional principal chiral sigma models. The $SU(N)\times SU(N)$ principal chiral sigma model in 1+1 dimensions is integrable, asymptotically free and has…

High Energy Physics - Theory · Physics 2014-10-01 Axel Cortés Cubero

$S$-matrices associated to the vector representations of the quantum groups for the classical Lie algebras are constructed. For the $a_{m-1}$ and $c_m$ algebras the complete $S$-matrix is found by an application of the bootstrap equations.…

High Energy Physics - Theory · Physics 2009-10-22 Timothy Hollowood

We investigate the perturbative integrability of two-dimensional massive quantum field theories with polynomial-like interactions and show that any theory of such class which is purely elastic at the tree level is also purely elastic at one…

High Energy Physics - Theory · Physics 2025-04-29 Matheus Fabri , Davide Polvara

The AdS3/CFT2 correspondence features massless non-relativistic modes on the string worldsheet in lightcone gauge. We study in detail these excitations and highlight how they naturally split between chiral (left-moving) and anti-chiral…

High Energy Physics - Theory · Physics 2023-03-29 Sergey Frolov , Alessandro Sfondrini

We point attention to the fact that in SO(10) models with non-canonical (type II) see-saw mechanism and exact b-tau unification the trace of the neutrino mass matrix is very small, in fact practically zero. This has the advantage of being a…

High Energy Physics - Phenomenology · Physics 2010-04-05 W. Rodejohann

A free boson on a lattice is the simplest field theory one can think of. Its partition function can be easily computed in momentum space. However, this straightforward solution hides its integrability properties. Here, we use the methods of…

Statistical Mechanics · Physics 2021-02-03 Manuel Campos , German Sierra , Esperanza Lopez

We consider the tree amplitudes of production of $n_2$ scalar particles by $n_1$ particles of another kind, where both initial and final particles are at rest and on mass shell, in a model of two scalar fields with $O(2)$ symmetric…

High Energy Physics - Phenomenology · Physics 2008-11-26 M. V. Libanov , V. A. Rubakov , S. V. Troitsky

The massless S-matrix of the pure RR AdS3 X S3 X T4 theory is very similar but not quite the same as Fendley-Intriligator's N=2 S-matrix, in turns related to Sine-Gordon taken at a special coupling. In this short note we review the reason…

High Energy Physics - Theory · Physics 2026-01-21 Alessandro Torrielli

We present a classification of the massless chiral matter representations that can arise locally in M-theory on G(2) through geometrically engineered singularities. We will find that several of the more exceptional singularities could have…

High Energy Physics - Theory · Physics 2008-05-27 Jacob L. Bourjaily , Sam Espahbodi

We characterize when a size-2 positive semidefinite (psd) factorization of a positive matrix of rank 3 and psd rank 2 is unique. The characterization is obtained using tools from rigidity theory. In the first step, we define…

Metric Geometry · Mathematics 2024-10-25 Kristen Dawson , Serkan Hoşten , Kaie Kubjas , Lilja Metsälampi

The unitary Critical Pomeron connects to a unique massless left-handed SU(5) theory that, remarkably, might provide an unconventional underlying unification for the Standard Model. Multi-regge theory suggests the existence of a {\it…

High Energy Physics - Phenomenology · Physics 2017-08-23 Alan. R. White

We analyze the complex analytic properties of Classical (tree-level) S-matrices for four scalar particles with s-t crossing symmetry, involving an infinite number of exchanges. Under suitable analytic conditions, we demonstrate that such…

High Energy Physics - Theory · Physics 2025-02-26 Abhijit Gadde , Shraiyance Jain

The exact factorisable quantum S-matrices are known for simply laced as well as non-simply laced affine Toda field theories. Non-simply laced theories are obtained from the affine Toda theories based on simply laced algebras by folding the…

High Energy Physics - Theory · Physics 2015-06-26 S. Pratik Khastgir

We find complete solutions of S-matrix bootstrap equations for the scatterings of massless particles in (1+1) dimensions with A_n symmetries. We show that only three types (minimal, diagonal, and saturated cases) of these S-matrices can…

High Energy Physics - Theory · Physics 2025-09-26 Changrim Ahn

The modern S-Matrix Bootstrap provides non-perturbative bounds on low-energy aspects of scattering amplitudes, leveraging the constraints of unitarity, analyticity and crossing. Typically, the solutions saturating such bounds also saturate…

High Energy Physics - Theory · Physics 2023-10-12 António Antunes , Miguel S. Costa , José Pereira

We study states of large charge density in integrable conformal coset models. For the O(2) coset, we consider two different S-matrices, one corresponding to a Thirring mass perturbation and the other to the continuation to O(2+epsilon). The…

High Energy Physics - Theory · Physics 2016-11-23 Nelia Mann , Joseph Polchinski
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