Non-metric geometry as the origin of mass in gauge theories of scale invariance

Abstract We discuss gauge theories of scale invariance beyond the Standard Model (SM) and Einstein gravity. A consequence of gauging this symmetry is that their underlying 4D geometry is non-metric ( $$\nabla _\mu g_{\alpha \beta }\!\not =\!0$$ ∇ μ g α β ≠ 0 ). Examples of such theories are Weyl’s o...

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Main Author: D. M. Ghilencea
Format: Article
Language:English
Published: SpringerOpen 2023-02-01
Series:European Physical Journal C: Particles and Fields
Online Access:https://doi.org/10.1140/epjc/s10052-023-11237-z
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author D. M. Ghilencea
author_facet D. M. Ghilencea
author_sort D. M. Ghilencea
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description Abstract We discuss gauge theories of scale invariance beyond the Standard Model (SM) and Einstein gravity. A consequence of gauging this symmetry is that their underlying 4D geometry is non-metric ( $$\nabla _\mu g_{\alpha \beta }\!\not =\!0$$ ∇ μ g α β ≠ 0 ). Examples of such theories are Weyl’s original quadratic gravity theory and its Palatini version. These theories have spontaneous breaking of the gauged scale symmetry to Einstein gravity. All mass scales have a geometric origin: the Planck scale ( $$M_p$$ M p ), cosmological constant ( $$\Lambda $$ Λ ) and the mass of the Weyl gauge boson ( $$\omega _\mu $$ ω μ ) of scale symmetry are proportional to a scalar field vev that has an origin in the (geometric) $${\tilde{R}}^2$$ R ~ 2 term in the action. With $$\omega _\mu $$ ω μ of non-metric geometry origin, the SM Higgs field also has a similar origin, generated by Weyl boson fusion in the early Universe. This appears as a microscopic realisation of “matter creation from geometry” discussed in the thermodynamics of open systems applied to cosmology. Unlike in local scale invariant theories (with no $$\omega _\mu $$ ω μ present) with an underlying pseudo-Riemannian geometry, in our case: (1) there are no ghosts and no additional fields beyond the SM and underlying Weyl or Palatini geometry, (2) the cosmological constant is positive and is small because gravity is weak, (3) the Weyl or Palatini connection shares the Weyl (gauge) symmetry of the action, and: (4) there exists a non-trivial, conserved Weyl current of this symmetry. An intuitive picture of non-metricity and its relation to mass generation is also provided from a solid state physics perspective where it is common and is associated with point defects (metric anomalies) of the crystalline structure.
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spelling doaj.art-d190b49796ce4541af55e67c746bc5802023-04-03T05:38:00ZengSpringerOpenEuropean Physical Journal C: Particles and Fields1434-60522023-02-0183211510.1140/epjc/s10052-023-11237-zNon-metric geometry as the origin of mass in gauge theories of scale invarianceD. M. Ghilencea0Department of Theoretical Physics, National Institute of Physics and Nuclear Engineering (IFIN)Abstract We discuss gauge theories of scale invariance beyond the Standard Model (SM) and Einstein gravity. A consequence of gauging this symmetry is that their underlying 4D geometry is non-metric ( $$\nabla _\mu g_{\alpha \beta }\!\not =\!0$$ ∇ μ g α β ≠ 0 ). Examples of such theories are Weyl’s original quadratic gravity theory and its Palatini version. These theories have spontaneous breaking of the gauged scale symmetry to Einstein gravity. All mass scales have a geometric origin: the Planck scale ( $$M_p$$ M p ), cosmological constant ( $$\Lambda $$ Λ ) and the mass of the Weyl gauge boson ( $$\omega _\mu $$ ω μ ) of scale symmetry are proportional to a scalar field vev that has an origin in the (geometric) $${\tilde{R}}^2$$ R ~ 2 term in the action. With $$\omega _\mu $$ ω μ of non-metric geometry origin, the SM Higgs field also has a similar origin, generated by Weyl boson fusion in the early Universe. This appears as a microscopic realisation of “matter creation from geometry” discussed in the thermodynamics of open systems applied to cosmology. Unlike in local scale invariant theories (with no $$\omega _\mu $$ ω μ present) with an underlying pseudo-Riemannian geometry, in our case: (1) there are no ghosts and no additional fields beyond the SM and underlying Weyl or Palatini geometry, (2) the cosmological constant is positive and is small because gravity is weak, (3) the Weyl or Palatini connection shares the Weyl (gauge) symmetry of the action, and: (4) there exists a non-trivial, conserved Weyl current of this symmetry. An intuitive picture of non-metricity and its relation to mass generation is also provided from a solid state physics perspective where it is common and is associated with point defects (metric anomalies) of the crystalline structure.https://doi.org/10.1140/epjc/s10052-023-11237-z
spellingShingle D. M. Ghilencea
Non-metric geometry as the origin of mass in gauge theories of scale invariance
European Physical Journal C: Particles and Fields
title Non-metric geometry as the origin of mass in gauge theories of scale invariance
title_full Non-metric geometry as the origin of mass in gauge theories of scale invariance
title_fullStr Non-metric geometry as the origin of mass in gauge theories of scale invariance
title_full_unstemmed Non-metric geometry as the origin of mass in gauge theories of scale invariance
title_short Non-metric geometry as the origin of mass in gauge theories of scale invariance
title_sort non metric geometry as the origin of mass in gauge theories of scale invariance
url https://doi.org/10.1140/epjc/s10052-023-11237-z
work_keys_str_mv AT dmghilencea nonmetricgeometryastheoriginofmassingaugetheoriesofscaleinvariance