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N=4 mechanics, WDVV equations and roots

N=4 superconformal n-particle quantum mechanics on the real line is governed by two prepotentials, U and F, which obey a system of partial nonlinear differential equations generalizing the Witten-Dijkgraaf-Verlinde-Verlinde (WDVV) equation. While F cannot vanish and triggers translation non-invarian...

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Autores principales: Galajinsky, Anton, Lechtenfeld, Olaf, Polovnikov, Kirill
Lenguaje:eng
Publicado: 2008
Materias:
Acceso en línea:https://dx.doi.org/10.1088/1126-6708/2009/03/113
http://cds.cern.ch/record/1092049
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author Galajinsky, Anton
Lechtenfeld, Olaf
Polovnikov, Kirill
author_facet Galajinsky, Anton
Lechtenfeld, Olaf
Polovnikov, Kirill
author_sort Galajinsky, Anton
collection CERN
description N=4 superconformal n-particle quantum mechanics on the real line is governed by two prepotentials, U and F, which obey a system of partial nonlinear differential equations generalizing the Witten-Dijkgraaf-Verlinde-Verlinde (WDVV) equation. While F cannot vanish and triggers translation non-invariance, U=0 yields a class of solutions (with vanishing central charge) which are encoded by the finite Coxeter systems. We extend previously known WDVV solutions in two ways: the A_n system is deformed n-parametrically to the edge set of a general orthocentric n-simplex, and the BCF-type systems form one-parameter families. A full classification strategy is proposed. The corresponding irreducible mechanics models admit a central-charge deformation (U\neq0) only for A_1 and in certain parts of the even dihedral systems I_2(2q). Thus, up to coordinate change and orthogonal composition, tunable couplings occur only in peculiar three-particle models, among which the one based on G_2+A_1 is the prime example. For vanishing central charge and any given F background, U may be constructed as a generalized hypergeometric function.
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spelling cern-10920492023-03-14T19:07:36Zdoi:10.1088/1126-6708/2009/03/113http://cds.cern.ch/record/1092049engGalajinsky, AntonLechtenfeld, OlafPolovnikov, KirillN=4 mechanics, WDVV equations and rootsParticle Physics - TheoryN=4 superconformal n-particle quantum mechanics on the real line is governed by two prepotentials, U and F, which obey a system of partial nonlinear differential equations generalizing the Witten-Dijkgraaf-Verlinde-Verlinde (WDVV) equation. While F cannot vanish and triggers translation non-invariance, U=0 yields a class of solutions (with vanishing central charge) which are encoded by the finite Coxeter systems. We extend previously known WDVV solutions in two ways: the A_n system is deformed n-parametrically to the edge set of a general orthocentric n-simplex, and the BCF-type systems form one-parameter families. A full classification strategy is proposed. The corresponding irreducible mechanics models admit a central-charge deformation (U\neq0) only for A_1 and in certain parts of the even dihedral systems I_2(2q). Thus, up to coordinate change and orthogonal composition, tunable couplings occur only in peculiar three-particle models, among which the one based on G_2+A_1 is the prime example. For vanishing central charge and any given F background, U may be constructed as a generalized hypergeometric function.N=4 superconformal n-particle quantum mechanics on the real line is governed by two prepotentials, U and F, which obey a system of partial nonlinear differential equations generalizing the Witten-Dijkgraaf-Verlinde-Verlinde (WDVV) equation. While F cannot vanish and triggers translation non-invariance, U=0 yields a class of solutions (with vanishing central charge) which are encoded by the finite Coxeter systems. We extend previously known WDVV solutions in two ways: the A_n system is deformed n-parametrically to the edge set of a general orthocentric n-simplex, and the BCF-type systems form one-parameter families. A full classification strategy is proposed. The corresponding irreducible mechanics models admit a central-charge deformation (U\neq0) only for A_1 and in certain parts of the even dihedral systems I_2(2q). Thus, up to coordinate change and orthogonal composition, tunable couplings occur only in peculiar three-particle models, among which the one based on G_2+A_1 is the prime example. For vanishing central charge and any given F background, U may be constructed as a generalized hypergeometric function.arXiv:0802.4386CERN-PH-TH-2008-041ITP-UH-04-08LMP-TPU-01-08CERN-PH-TH-2008-041ITP–UH–04-08LMP-TPU–01-08oai:cds.cern.ch:10920492008-03-03
spellingShingle Particle Physics - Theory
Galajinsky, Anton
Lechtenfeld, Olaf
Polovnikov, Kirill
N=4 mechanics, WDVV equations and roots
title N=4 mechanics, WDVV equations and roots
title_full N=4 mechanics, WDVV equations and roots
title_fullStr N=4 mechanics, WDVV equations and roots
title_full_unstemmed N=4 mechanics, WDVV equations and roots
title_short N=4 mechanics, WDVV equations and roots
title_sort n=4 mechanics, wdvv equations and roots
topic Particle Physics - Theory
url https://dx.doi.org/10.1088/1126-6708/2009/03/113
http://cds.cern.ch/record/1092049
work_keys_str_mv AT galajinskyanton n4mechanicswdvvequationsandroots
AT lechtenfeldolaf n4mechanicswdvvequationsandroots
AT polovnikovkirill n4mechanicswdvvequationsandroots