Scale invariance vs. conformal invariance: holographic two-point functions in Horndeski gravity

Abstract We consider Einstein-Horndeski gravity with a negative bare constant as a holographic model to investigate whether a scale invariant quantum field theory can exist without the full conformal invariance. Einstein-Horndeski gravity can admit two different AdS vacua. One is conformal, and the...

Full description

Bibliographic Details
Main Authors: Yue-Zhou Li, H. Lü, Hao-Yu Zhang
Format: Article
Language:English
Published: SpringerOpen 2019-07-01
Series:European Physical Journal C: Particles and Fields
Online Access:http://link.springer.com/article/10.1140/epjc/s10052-019-7096-6
id doaj-80d7cd5e26ec4d56996e9cbb51aed431
record_format Article
spelling doaj-80d7cd5e26ec4d56996e9cbb51aed4312020-11-25T03:24:09ZengSpringerOpenEuropean Physical Journal C: Particles and Fields1434-60441434-60522019-07-0179711310.1140/epjc/s10052-019-7096-6Scale invariance vs. conformal invariance: holographic two-point functions in Horndeski gravityYue-Zhou Li0H. Lü1Hao-Yu Zhang2Center for Joint Quantum Studies and Department of Physics, School of Science, Tianjin UniversityCenter for Joint Quantum Studies and Department of Physics, School of Science, Tianjin UniversityDepartment of Physics, Shandong UniversityAbstract We consider Einstein-Horndeski gravity with a negative bare constant as a holographic model to investigate whether a scale invariant quantum field theory can exist without the full conformal invariance. Einstein-Horndeski gravity can admit two different AdS vacua. One is conformal, and the holographic two-point functions of the boundary energy-momentum tensor are the same as the ones obtained in Einstein gravity. The other AdS vacuum, which arises at some critical point of the coupling constants, preserves the scale invariance but not the special conformal invariance due to the logarithmic radial dependence of the Horndeski scalar. In addition to the transverse and traceless graviton modes, the theory admits an additional trace/scalar mode in the scale invariant vacuum. We obtain the two-point functions of the corresponding boundary operators. We find that the trace/scalar mode gives rise to an non-vanishing two-point function, which distinguishes the scale invariant theory from the conformal theory. The two-point function vanishes in $$d=2$$ d=2 , where the full conformal symmetry is restored. Our results indicate the strongly coupled scale invariant unitary quantum field theory may exist in $$d\ge 3$$ d≥3 without the full conformal symmetry. The operator that is dual to the bulk trace/scalar mode however violates the dominant energy condition.http://link.springer.com/article/10.1140/epjc/s10052-019-7096-6
collection DOAJ
language English
format Article
sources DOAJ
author Yue-Zhou Li
H. Lü
Hao-Yu Zhang
spellingShingle Yue-Zhou Li
H. Lü
Hao-Yu Zhang
Scale invariance vs. conformal invariance: holographic two-point functions in Horndeski gravity
European Physical Journal C: Particles and Fields
author_facet Yue-Zhou Li
H. Lü
Hao-Yu Zhang
author_sort Yue-Zhou Li
title Scale invariance vs. conformal invariance: holographic two-point functions in Horndeski gravity
title_short Scale invariance vs. conformal invariance: holographic two-point functions in Horndeski gravity
title_full Scale invariance vs. conformal invariance: holographic two-point functions in Horndeski gravity
title_fullStr Scale invariance vs. conformal invariance: holographic two-point functions in Horndeski gravity
title_full_unstemmed Scale invariance vs. conformal invariance: holographic two-point functions in Horndeski gravity
title_sort scale invariance vs. conformal invariance: holographic two-point functions in horndeski gravity
publisher SpringerOpen
series European Physical Journal C: Particles and Fields
issn 1434-6044
1434-6052
publishDate 2019-07-01
description Abstract We consider Einstein-Horndeski gravity with a negative bare constant as a holographic model to investigate whether a scale invariant quantum field theory can exist without the full conformal invariance. Einstein-Horndeski gravity can admit two different AdS vacua. One is conformal, and the holographic two-point functions of the boundary energy-momentum tensor are the same as the ones obtained in Einstein gravity. The other AdS vacuum, which arises at some critical point of the coupling constants, preserves the scale invariance but not the special conformal invariance due to the logarithmic radial dependence of the Horndeski scalar. In addition to the transverse and traceless graviton modes, the theory admits an additional trace/scalar mode in the scale invariant vacuum. We obtain the two-point functions of the corresponding boundary operators. We find that the trace/scalar mode gives rise to an non-vanishing two-point function, which distinguishes the scale invariant theory from the conformal theory. The two-point function vanishes in $$d=2$$ d=2 , where the full conformal symmetry is restored. Our results indicate the strongly coupled scale invariant unitary quantum field theory may exist in $$d\ge 3$$ d≥3 without the full conformal symmetry. The operator that is dual to the bulk trace/scalar mode however violates the dominant energy condition.
url http://link.springer.com/article/10.1140/epjc/s10052-019-7096-6
work_keys_str_mv AT yuezhouli scaleinvariancevsconformalinvarianceholographictwopointfunctionsinhorndeskigravity
AT hlu scaleinvariancevsconformalinvarianceholographictwopointfunctionsinhorndeskigravity
AT haoyuzhang scaleinvariancevsconformalinvarianceholographictwopointfunctionsinhorndeskigravity
_version_ 1724603025593466880