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Hyperscaling relations in mass-deformed conformal gauge theories

Hyperscaling relations in mass-deformed conformal gauge theories
Hyperscaling relations in mass-deformed conformal gauge theories
We present a number of analytical results which should guide the interpretation of lattice data in theories with an infrared fixed point (IRFP) deformed by a mass term δL = -m q‾ q. From renormalization group (RG) arguments we obtain the leading scaling exponent, F ~ m ηF, for all decay constants of the lowest lying states other than the ones affected by the chiral anomaly and the tensor ones. These scaling relations provide a clear cut way to distinguish a theory with an IRFP from a confining theory with heavy fermions. Moreover, we present a derivation relating the scaling of ⟨q‾q⟩ ~ m ηq‾q   to the scaling of the density of eigenvalues of the massless Dirac operator ρ(λ) ~ λ ηq‾q. RG arguments yield ηq‾q  = (3-γ*)/(1+γ*) as a function of the mass anomalous dimension γ* at the IRFP. The arguments can be generalized to other condensates such as ⟨G2⟩ ~ m4/(1+γ*). We describe a heuristic derivation of the result on the condensates, which provides interesting connections between different approaches. Our results are compared with existing data from numerical studies of SU(2) with two adjoint Dirac fermions.
1550-7998
014502-[15pp]
Zwicky, Roman
e1972346-331c-45ba-b057-ddb9ce03c3de
Zwicky, Roman
e1972346-331c-45ba-b057-ddb9ce03c3de

Zwicky, Roman (2010) Hyperscaling relations in mass-deformed conformal gauge theories. Physical Review D, 82 (1), 014502-[15pp]. (doi:10.1103/PhysRevD.82.014502).

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Abstract

We present a number of analytical results which should guide the interpretation of lattice data in theories with an infrared fixed point (IRFP) deformed by a mass term δL = -m q‾ q. From renormalization group (RG) arguments we obtain the leading scaling exponent, F ~ m ηF, for all decay constants of the lowest lying states other than the ones affected by the chiral anomaly and the tensor ones. These scaling relations provide a clear cut way to distinguish a theory with an IRFP from a confining theory with heavy fermions. Moreover, we present a derivation relating the scaling of ⟨q‾q⟩ ~ m ηq‾q   to the scaling of the density of eigenvalues of the massless Dirac operator ρ(λ) ~ λ ηq‾q. RG arguments yield ηq‾q  = (3-γ*)/(1+γ*) as a function of the mass anomalous dimension γ* at the IRFP. The arguments can be generalized to other condensates such as ⟨G2⟩ ~ m4/(1+γ*). We describe a heuristic derivation of the result on the condensates, which provides interesting connections between different approaches. Our results are compared with existing data from numerical studies of SU(2) with two adjoint Dirac fermions.

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Published date: July 2010

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Local EPrints ID: 185775
URI: http://eprints.soton.ac.uk/id/eprint/185775
ISSN: 1550-7998
PURE UUID: f9bd5c0c-f855-4bb9-bfba-d68a9821a957

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Date deposited: 11 May 2011 08:19
Last modified: 14 Mar 2024 03:15

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Author: Roman Zwicky

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