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Related papers: SO(5) Clebsch-Gordan coefficients involving the 14…

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We discuss supersymmetric defects in 6d $\mathcal{N}=(1,0)$ SCFTs with $\mathrm{SO}(N_c)$ gauge group and $N_c-8$ fundamental flavors. The codimension 2 and 4 defects are engineered by coupling the 6d gauge fields to charged free fields in…

High Energy Physics - Theory · Physics 2022-04-13 Jin Chen , Babak Haghighat , Hee-Cheol Kim , Kimyeong Lee , Marcus Sperling , Xin Wang

We determine the Clebsch-Gordan and Racah-Wigner coefficients for continuous series of representations of the quantum deformed algebras U_q(sl(2)) and U_q(osp(1|2)). While our results for the former algebra reproduce formulas by Ponsot and…

High Energy Physics - Theory · Physics 2015-06-16 Leszek Hadasz , Michal Pawelkiewicz , Volker Schomerus

We introduce simple variables for describing the AdS$_5\times S^5$ superspace, i. e. $\frac{PSU(2,2|4)}{SO(4,1)\times SO(5)}$. The idea is to embed the coset superspace into a space described by variables which are in linear (ray)…

High Energy Physics - Theory · Physics 2015-10-28 Hidehiko Shimada

The $N=4$ SU(2)$_k$ superconformal algebra has the global automorphism of SO(4) $\approx$ SU(2)$\times$SU(2) with the {\it left} factor as the Kac-Moody gauge symmetry. As a consequence, an infinite set of independent algebras labeled by…

High Energy Physics - Theory · Physics 2015-06-26 Satoshi Matsuda , Yukitaka Ishimoto

In this paper, we introduce a new theoretical framework built upon fractional Sobolev-type spaces involving Riemann-Liouville (RL) fractional integrals/derivatives, which is naturally arisen from exact representations of Chebyshev expansion…

Numerical Analysis · Mathematics 2019-05-28 Wenjie Liu , Li-Lian Wang , Huiyuan Li

Explicit expressions are given for the actions and radial matrix elements of basic radial observables on multi-dimensional spaces in a continuous sequence of orthonormal bases for unitary SU(1,1) irreps. Explicit expressions are also given…

Mathematical Physics · Physics 2009-11-11 D. J. Rowe

According to Wilson's theory of critical phenomena, critical exponents are universal functions of $d$, the dimension of space, and $n$, the dimension of the symmetry group. SO(5) theory of antiferromagnetism and superconductivity predicts a…

Superconductivity · Physics 2015-06-24 Jiang-Ping Hu , Shou-Cheng Zhang

We study representations of $U_q(su(1,1))$ that can be considered as quantum analogs of tensor products of irreducible *-representations of the Lie algebra $su(1,1)$. We determine the decomposition of these representations into irreducible…

Quantum Algebra · Mathematics 2011-08-10 Wolter Groenevelt

We prove a curvature-dimension criterion and obtain logarithmic Sobolev inequalities for generalised Cauchy measures with optimal weights and explicit constants. In the one-dimensional case, this constant is even optimal. From these…

Functional Analysis · Mathematics 2026-04-06 Baptiste Nicolas Huguet

The article is devoted to some ``strange'' phenomena of representation theory and their interrelations. Cross-projective representations of pairs of anticommutative algebras, alloys, their universal envelopping Lie algebras and their…

Representation Theory · Mathematics 2007-05-23 Denis V. Juriev

Let G be a finite subgroup of SL(n,C), then the quotient C^n/G has a Gorenstein canonical singularity. Bridgeland-King-Reid proved that the G-Hilbert scheme Hilb^G(C^3) gives a crepant resolution of the quotient C^3/G for any finite…

Algebraic Geometry · Mathematics 2019-06-04 Y. Sato

It is shown that the method of infinitesimal generators ("Racah's method") can be broadly and systematically formulated as a method applicable to the calculation of reduced coupling coefficients for a generic subalgebra chain G>H, provided…

Mathematical Physics · Physics 2011-02-11 M. A. Caprio , K. D. Sviratcheva , A. E. McCoy

Let $\pi$ be a group equipped with an action of a second group $G$ by automorphisms. We define the equivariant cohomological dimension ${\sf cd}_G(\pi)$, the equivariant geometric dimension ${\sf gd}_G(\pi)$, and the equivariant…

Algebraic Topology · Mathematics 2020-04-24 Mark Grant , Ehud Meir , Irakli Patchkoria

We provide a new tableau model from which one can easily deduce the characters of finite-dimensional irreducible polynomial representations of the special orthogonal group $SO_n(\mathbb{C})$. This model originates from the representation…

Combinatorics · Mathematics 2023-02-17 Hideya Watanabe

The effective dimension-5 operators can be induced by quantum gravity or inspired by string and M theories. They have important impacts on grand unified theories. We investigate the group theoretic nature of them for the well known E(6)…

High Energy Physics - Phenomenology · Physics 2015-06-18 Chao-Shang Huang

Highest weight representations of $U_q(su(1,1))$ with $q=\exp \pi i/N$ are investigated. The structures of the irreducible hieghesat weight modules are discussed in detail. The Clebsch-Gordan decomposition for the tensor product of two…

High Energy Physics - Theory · Physics 2009-10-22 Takashi Suzuki

We summarize some previous work on SU(4) describing hadron representations and transformations as well as its noncompact 'counterpart' SU$*$(4) being the complex embedding of SL(2,$\mathbb{H}$). So after having related the 16-dim Dirac…

General Physics · Physics 2017-05-09 Rolf Dahm

We give an explicit algebraic description of finite Lorentz transformations of vectors in 10-dimensional Minkowski space by means of a parameterization in terms of the octonions. The possible utility of these results for superstring theory…

High Energy Physics - Theory · Physics 2009-10-22 Corinne A. Manogue , Jörg Schray

We discuss the Klein-Gordon (KG) equation using a 5D space-time approach. We explicitly show that the KG equation in flat space-time admits a consistent probabilistic interpretation with positively defined probability density. However, the…

Quantum Physics · Physics 2015-06-19 Romulus Breban

We re-express the quantum Calogero-Sutherland model for the Lie algebra $E_6$ and the particular value of the coupling constant $\kappa=1$ by using the fundamental irreducible characters of the algebra as dynamical variables. For that, we…

Mathematical Physics · Physics 2015-06-26 J. Fernandez-Nunez , W. Garcia-Fuertes , A. M. Perelomov