Finite cutoff CFT's and composite operators
Recently a conformally invariant action describing the Wilson-Fisher fixed point in D=4−ϵ dimensions in the presence of a finite UV cutoff was constructed [44]. In the present paper we construct two composite operator perturbations of this action with definite scaling dimension also in the presence...
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2021
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oai:doaj.org-article:0d8d494bb95d40faaec17d6f475845ed2021-12-04T04:32:50ZFinite cutoff CFT's and composite operators0550-321310.1016/j.nuclphysb.2021.115574https://doaj.org/article/0d8d494bb95d40faaec17d6f475845ed2021-12-01T00:00:00Zhttp://www.sciencedirect.com/science/article/pii/S0550321321002716https://doaj.org/toc/0550-3213Recently a conformally invariant action describing the Wilson-Fisher fixed point in D=4−ϵ dimensions in the presence of a finite UV cutoff was constructed [44]. In the present paper we construct two composite operator perturbations of this action with definite scaling dimension also in the presence of a finite cutoff. Thus the operator (as well as the fixed point action) is well defined at all momenta 0≤p≤∞ and at low energies they reduce to ∫xϕ2 and ∫xϕ4 respectively. The construction includes terms up to O(ϵ2). In the presence of a finite cutoff they mix with higher order ∫xϕn operators. The dimensions are also calculated to this order and agree with known results.S. DuttaB. SathiapalanElsevierarticleNuclear and particle physics. Atomic energy. RadioactivityQC770-798ENNuclear Physics B, Vol 973, Iss , Pp 115574- (2021) |
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Nuclear and particle physics. Atomic energy. Radioactivity QC770-798 |
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Nuclear and particle physics. Atomic energy. Radioactivity QC770-798 S. Dutta B. Sathiapalan Finite cutoff CFT's and composite operators |
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Recently a conformally invariant action describing the Wilson-Fisher fixed point in D=4−ϵ dimensions in the presence of a finite UV cutoff was constructed [44]. In the present paper we construct two composite operator perturbations of this action with definite scaling dimension also in the presence of a finite cutoff. Thus the operator (as well as the fixed point action) is well defined at all momenta 0≤p≤∞ and at low energies they reduce to ∫xϕ2 and ∫xϕ4 respectively. The construction includes terms up to O(ϵ2). In the presence of a finite cutoff they mix with higher order ∫xϕn operators. The dimensions are also calculated to this order and agree with known results. |
format |
article |
author |
S. Dutta B. Sathiapalan |
author_facet |
S. Dutta B. Sathiapalan |
author_sort |
S. Dutta |
title |
Finite cutoff CFT's and composite operators |
title_short |
Finite cutoff CFT's and composite operators |
title_full |
Finite cutoff CFT's and composite operators |
title_fullStr |
Finite cutoff CFT's and composite operators |
title_full_unstemmed |
Finite cutoff CFT's and composite operators |
title_sort |
finite cutoff cft's and composite operators |
publisher |
Elsevier |
publishDate |
2021 |
url |
https://doaj.org/article/0d8d494bb95d40faaec17d6f475845ed |
work_keys_str_mv |
AT sdutta finitecutoffcftsandcompositeoperators AT bsathiapalan finitecutoffcftsandcompositeoperators |
_version_ |
1718373012577714176 |