Low energy properties of SU(2) gauge theory with Nf = 3/2 flavours of adjoint fermions
A bstract In this work we present the results of a numerical investigation of SU(2) gauge theory with N f = 3 / 2 flavours of fermions, corresponding to 3 Majorana fermions, which transform in the adjoint representation of the gauge group. At two values of the gauge coupling, the masses of bound sta...
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Published in | The journal of high energy physics Vol. 2018; no. 1; pp. 1 - 15 |
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Main Authors | , , , , , |
Format | Journal Article |
Language | English |
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01.01.2018
Springer Nature B.V SpringerOpen |
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Abstract | A
bstract
In this work we present the results of a numerical investigation of SU(2) gauge theory with
N
f
= 3
/
2 flavours of fermions, corresponding to 3 Majorana fermions, which transform in the adjoint representation of the gauge group. At two values of the gauge coupling, the masses of bound states are considered as a function of the fundamental fermion mass, represented by the PCAC quark mass. The scaling of bound states masses indicates an infrared conformal behaviour of the theory. We obtain estimates for the fixed-point value of the mass anomalous dimension
γ
∗
from the scaling of masses and from the scaling of the mode number of the Wilson-Dirac operator. The difference of the estimates at the two gauge couplings should be due to scaling violations and lattice spacing effects. The more reliable estimate at the smaller gauge coupling is
γ
∗
≈ 0
.
38(2). |
---|---|
AbstractList | In this work we present the results of a numerical investigation of SU(2) gauge theory with Nf = 3/2 flavours of fermions, corresponding to 3 Majorana fermions, which transform in the adjoint representation of the gauge group. At two values of the gauge coupling, the masses of bound states are considered as a function of the fundamental fermion mass, represented by the PCAC quark mass. The scaling of bound states masses indicates an infrared conformal behaviour of the theory. We obtain estimates for the fixed-point value of the mass anomalous dimension γ∗ from the scaling of masses and from the scaling of the mode number of the Wilson-Dirac operator. The difference of the estimates at the two gauge couplings should be due to scaling violations and lattice spacing effects. The more reliable estimate at the smaller gauge coupling is γ∗ ≈ 0.38(2). A bstract In this work we present the results of a numerical investigation of SU(2) gauge theory with N f = 3 / 2 flavours of fermions, corresponding to 3 Majorana fermions, which transform in the adjoint representation of the gauge group. At two values of the gauge coupling, the masses of bound states are considered as a function of the fundamental fermion mass, represented by the PCAC quark mass. The scaling of bound states masses indicates an infrared conformal behaviour of the theory. We obtain estimates for the fixed-point value of the mass anomalous dimension γ ∗ from the scaling of masses and from the scaling of the mode number of the Wilson-Dirac operator. The difference of the estimates at the two gauge couplings should be due to scaling violations and lattice spacing effects. The more reliable estimate at the smaller gauge coupling is γ ∗ ≈ 0 . 38(2). Abstract In this work we present the results of a numerical investigation of SU(2) gauge theory with N f = 3/2 flavours of fermions, corresponding to 3 Majorana fermions, which transform in the adjoint representation of the gauge group. At two values of the gauge coupling, the masses of bound states are considered as a function of the fundamental fermion mass, represented by the PCAC quark mass. The scaling of bound states masses indicates an infrared conformal behaviour of the theory. We obtain estimates for the fixed-point value of the mass anomalous dimension γ ∗ from the scaling of masses and from the scaling of the mode number of the Wilson-Dirac operator. The difference of the estimates at the two gauge couplings should be due to scaling violations and lattice spacing effects. The more reliable estimate at the smaller gauge coupling is γ ∗ ≈ 0.38(2). |
ArticleNumber | 119 |
Author | Montvay, Istvan Giudice, Pietro Scior, Philipp Piemonte, Stefano Bergner, Georg Münster, Gernot |
Author_xml | – sequence: 1 givenname: Georg surname: Bergner fullname: Bergner, Georg organization: University of Jena, Institute for Theoretical Physics – sequence: 2 givenname: Pietro orcidid: 0000-0002-4138-8860 surname: Giudice fullname: Giudice, Pietro organization: University of Münster, Institute for Theoretical Physics – sequence: 3 givenname: Gernot surname: Münster fullname: Münster, Gernot email: munsteg@uni-muenster.de organization: University of Münster, Institute for Theoretical Physics – sequence: 4 givenname: Philipp surname: Scior fullname: Scior, Philipp organization: University of Münster, Institute for Theoretical Physics – sequence: 5 givenname: Istvan surname: Montvay fullname: Montvay, Istvan organization: Deutsches Elektronen-Synchrotron DESY – sequence: 6 givenname: Stefano surname: Piemonte fullname: Piemonte, Stefano organization: University of Regensburg, Institute for Theoretical Physics |
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Cites_doi | 10.1088/1126-6708/2009/03/013 10.1103/PhysRevD.51.3745 10.1007/JHEP07(2013)061 10.1088/1126-6708/2009/04/050 10.1007/JHEP08(2014)127 10.1103/PhysRevD.86.025006 10.1016/0550-3213(82)90035-9 10.1016/j.physletb.2005.07.050 10.1103/PhysRevD.96.034504 10.1103/RevModPhys.88.015001 10.1103/PhysRevD.69.054501 10.1007/JHEP06(2016)114 10.1103/PhysRevD.82.014502 10.1103/PhysRevD.94.065026 10.1103/PhysRevD.75.085018 10.1103/PhysRevD.91.114508 |
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References_xml | – volume: D 24 start-page: 1441 year: 1981 ident: 7485_CR2 publication-title: Phys. Rev. contributor: fullname: B Holdom – ident: 7485_CR6 – volume: 03 start-page: 013 year: 2009 ident: 7485_CR16 publication-title: JHEP doi: 10.1088/1126-6708/2009/03/013 contributor: fullname: L Giusti – ident: 7485_CR22 doi: 10.1103/PhysRevD.51.3745 – ident: 7485_CR18 doi: 10.1007/JHEP07(2013)061 – volume: 04 start-page: 050 year: 2009 ident: 7485_CR13 publication-title: JHEP doi: 10.1088/1126-6708/2009/04/050 contributor: fullname: MA Luty – ident: 7485_CR20 doi: 10.1007/JHEP08(2014)127 – ident: 7485_CR17 doi: 10.1103/PhysRevD.86.025006 – ident: 7485_CR1 doi: 10.1016/0550-3213(82)90035-9 – ident: 7485_CR12 doi: 10.1016/j.physletb.2005.07.050 – ident: 7485_CR19 – ident: 7485_CR4 doi: 10.1103/PhysRevD.96.034504 – ident: 7485_CR5 doi: 10.1103/RevModPhys.88.015001 – ident: 7485_CR10 doi: 10.1103/PhysRevD.69.054501 – ident: 7485_CR15 doi: 10.1007/JHEP06(2016)114 – ident: 7485_CR14 doi: 10.1103/PhysRevD.82.014502 – ident: 7485_CR11 doi: 10.1103/PhysRevD.94.065026 – ident: 7485_CR21 – ident: 7485_CR3 doi: 10.1103/PhysRevD.75.085018 – ident: 7485_CR8 – ident: 7485_CR9 – ident: 7485_CR7 doi: 10.1103/PhysRevD.91.114508 |
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Snippet | A
bstract
In this work we present the results of a numerical investigation of SU(2) gauge theory with
N
f
= 3
/
2 flavours of fermions, corresponding to 3... In this work we present the results of a numerical investigation of SU(2) gauge theory with Nf = 3/2 flavours of fermions, corresponding to 3 Majorana... Abstract In this work we present the results of a numerical investigation of SU(2) gauge theory with N f = 3/2 flavours of fermions, corresponding to 3... |
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SubjectTerms | Classical and Quantum Gravitation Couplings Elementary Particles Fermions Flavor (particle physics) Gauge theory High energy physics Lattice Quantum Field Theory Physics Physics and Astronomy Quantum Field Theories Quantum Field Theory Quantum Physics Regular Article - Theoretical Physics Relativity Theory Renormalization Group Scaling String Theory |
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Title | Low energy properties of SU(2) gauge theory with Nf = 3/2 flavours of adjoint fermions |
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