Leading low-energy effective action in 6D, N=(1,1) SYM theory; Journal of High Energy Physics; Vol. 2018, iss. 9
| Parent link: | Journal of High Energy Physics Vol. 2018, iss. 9.— 2018.— [39, 15 p.] |
|---|---|
| Autor principal: | |
| Autor Corporativo: | |
| Outros Autores: | , |
| Resumo: | Title screen We elaborate on the low-energy effective action of 6D, N=(1,1)N=(1,1) supersymmetric Yang-Mills (SYM) theory in the N=(1,0)N=(1,0) harmonic superspace formulation. The theory is described in terms of analytic N=(1,0)N=(1,0) gauge superfield V ++ and analytic ω-hypermultiplet, both in the adjoint representation of gauge group. The effective action is defined in the framework of the background superfield method ensuring the manifest gauge invariance along with manifest N=(1,0)N=(1,0) supersymmetry. We calculate leading contribution to the one-loop effective action using the on-shell background superfields corresponding to the option when gauge group SU(N) is broken to SU(N − 1) × ϒ(1) ⊂ SU(N). In the bosonic sector the effective action involves the structure ∼F2X2∼F2X2 , where F 4 is a monomial of the fourth degree in an abelian field strength FM N and X stands for the scalar fields from the ω-hypermultiplet. It is manifestly demonstrated that the expectation values of the hypermultiplet scalar fields play the role of a natural infrared cutoff. Режим доступа: по договору с организацией-держателем ресурса |
| Idioma: | inglês |
| Publicado em: |
2018
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| Assuntos: | |
| Acesso em linha: | https://doi.org/10.1007/JHEP09(2018)039 |
| Formato: | Recurso Electrónico Capítulo de Livro |
| KOHA link: | https://koha.lib.tpu.ru/cgi-bin/koha/opac-detail.pl?biblionumber=659955 |
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| 200 | 1 | |a Leading low-energy effective action in 6D, N=(1,1) SYM theory |f I. L. Bukhbinder, E. A. Ivanov, B. S. Merzlikin | |
| 203 | |a Text |c electronic | ||
| 300 | |a Title screen | ||
| 320 | |a [References: 53 tit.] | ||
| 330 | |a We elaborate on the low-energy effective action of 6D, N=(1,1)N=(1,1) supersymmetric Yang-Mills (SYM) theory in the N=(1,0)N=(1,0) harmonic superspace formulation. The theory is described in terms of analytic N=(1,0)N=(1,0) gauge superfield V ++ and analytic ω-hypermultiplet, both in the adjoint representation of gauge group. The effective action is defined in the framework of the background superfield method ensuring the manifest gauge invariance along with manifest N=(1,0)N=(1,0) supersymmetry. We calculate leading contribution to the one-loop effective action using the on-shell background superfields corresponding to the option when gauge group SU(N) is broken to SU(N − 1) × ϒ(1) ⊂ SU(N). In the bosonic sector the effective action involves the structure ∼F2X2∼F2X2 , where F 4 is a monomial of the fourth degree in an abelian field strength FM N and X stands for the scalar fields from the ω-hypermultiplet. It is manifestly demonstrated that the expectation values of the hypermultiplet scalar fields play the role of a natural infrared cutoff. | ||
| 333 | |a Режим доступа: по договору с организацией-держателем ресурса | ||
| 461 | |t Journal of High Energy Physics | ||
| 463 | |t Vol. 2018, iss. 9 |v [39, 15 p.] |d 2018 | ||
| 610 | 1 | |a электронный ресурс | |
| 610 | 1 | |a труды учёных ТПУ | |
| 610 | 1 | |a extended supersymmetry | |
| 610 | 1 | |a superspaces | |
| 610 | 1 | |a supersymmetric gauge theory | |
| 610 | 1 | |a суперпространство | |
| 610 | 1 | |a калибровочная теория | |
| 700 | 1 | |a Bukhbinder |b I. L. |g Iosif Lvovich | |
| 701 | 1 | |a Ivanov |b E. A. |g Evgenyi | |
| 701 | 1 | |a Merzlikin |b B. S. |c mathematician |c research engineer, Senior Lecturer of Tomsk Polytechnic University, candidate of physico-mathematical Sciences |f 1987- |g Boris Sergeevich |3 (RuTPU)RU\TPU\pers\30925 |9 15163 | |
| 712 | 0 | 2 | |a Национальный исследовательский Томский политехнический университет |b Инженерная школа ядерных технологий |b Отделение экспериментальной физики |3 (RuTPU)RU\TPU\col\23549 |
| 801 | 2 | |a RU |b 63413507 |c 20190409 |g RCR | |
| 856 | 4 | |u https://doi.org/10.1007/JHEP09(2018)039 | |
| 942 | |c CF | ||