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Dynamical symmetry breaking in curved spacetime -review-
High Energy Physics - Theory · Submitted 12 Nov 1997
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim It is also argued that the chiral symmetry broken by a weak magnetic field may be restored due to the presence of gravitational field.
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The paper's own sentences, arranged. Each label is drawn from a closed vocabulary; the number beside it is the probability the classifier gave that label. Numbers in the tables are the authors', checked by code. No sentence in this record was written by a model.
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The abstract, sentence by sentence
Four-fermion interaction models are considered to be prototype models for dynamical symmetry breaking.The present review deals with recent developments in the studies of dynamical symmetry breaking in the four-fermion interaction models and their extension in curved spacetime. Starting with the Minkowski spacetime in dimension $D$ ($2 \leq D \leq 4$) the effective potential in the leading order of $1/N$-expansion is calculated and the phase structure of the theory is investigated. In curved spacetime curvature-induced phase transitions are discussed in the circumstances where fermion masses are dynamically generated. Subsequently a possibility of curvature- and temperature-induced or curvature- and topology-induced phase transitions is discussed. It is also argued that the chiral symmetry broken by a weak magnetic field may be restored due to the presence of gravitational field. Finally some applications of four-fermion models in quantum gravity are briefly described.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | Four-fermion interaction models are considered to be prototype models for dynamical symmetry breaking.The present review deals with recent developments in the studies of dynamical symmetry breaking in the four-fermion interaction models and their extension in curved spacetime. | background 0.67 | 0.23 | 0.08 | asserted 0.99 |
| s1 | Starting with the Minkowski spacetime in dimension $D$ ($2 \leq D \leq 4$) the effective potential in the leading order of $1/N$-expansion is calculated and the phase structure of the theory is investigated. | method 0.73 | 0.58 | 0.05 | asserted 0.99 |
| s2 | In curved spacetime curvature-induced phase transitions are discussed in the circumstances where fermion masses are dynamically generated. | contribution 0.93 | 0.29 | 0.11 | asserted 0.87 |
| s3 | Subsequently a possibility of curvature- and temperature-induced or curvature- and topology-induced phase transitions is discussed. | contribution 0.97 | 0.38 | 0.07 | hedged possibility 0.89 |
| s4 | It is also argued that the chiral symmetry broken by a weak magnetic field may be restored due to the presence of gravitational field. | result 0.76 | 0.37 | 0.18 | hedged possibility 1.00 |
| s5 | Finally some applications of four-fermion models in quantum gravity are briefly described. | contribution 0.89 | 0.25 | 0.06 | asserted 0.85 |
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The paper
Original abstract
Four-fermion interaction models are considered to be prototype models for dynamical symmetry breaking.The present review deals with recent developments in the studies of dynamical symmetry breaking in the four-fermion interaction models and their extension in curved spacetime. Starting with the Minkowski spacetime in dimension $D$ ($2 \leq D \leq 4$) the effective potential in the leading order of $1/N$-expansion is calculated and the phase structure of the theory is investigated. In curved spacetime curvature-induced phase transitions are discussed in the circumstances where fermion masses are dynamically generated. Subsequently a possibility of curvature- and temperature-induced or curvature- and topology-induced phase transitions is discussed. It is also argued that the chiral symmetry broken by a weak magnetic field may be restored due to the presence of gravitational field. Finally some applications of four-fermion models in quantum gravity are briefly described.
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References
How the literature uses it
17 arXiv papers cite this in 27 sentences
Papers whose main result relates to this one's
States the same result 1 paper
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We show that the gravitational field may compensate the effect of the magnetic field what leads to restoration of chiral symmetry.
Nambu-Jona-Lasinio Model in Curved Spacetime with Magnetic Field · 0.96
Papers citing it · 17 sentences without a confident label
Uses its method or tool 2 papers
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Performing the path integrals of the fermion field, we obtain the effective potential in the leading order of the $1/N$ expansion [ref] , [equation] where $M$ is an arbitrary mass scale and the trace, $$, denotes the sum over the spinor indices.
Precise Phase Structure in Four-fermion Interaction Model on Torus · Four-fermion interaction model on torus · 0.91
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Integrating out of the fermion with the cut-off regularization, we obtain the one-loop corrected potential [ref] , [equation]
Neutron star in Logarithmic model of Cartan $F(R)$ gravity · Effective potential of scalaron · 0.82
Compares with it 1 paper
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The derived expressions for the effective potential reduce to the known results in the previous works at the periodic ($δ=0$) and anti-periodic ($δ=1$) boundary conditions [ref] .
Four-Fermion Interaction Model on $\mathcal{M}^{D-1} \otimes S^1$ · Conclusions · 0.98
Cites it as background 6 papers
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The phenomenon is known to occur generically in fermionic systems of any dimension for various negatively curved spacetimes even at the weakest fermionic attraction [ref] .
A curvature bound from gravitational catalysis · Introduction · 0.87
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It is known that the broken chiral symmetry is restored by the finite size effect for the anti-periodic boundary condition, $δ=1$ and the finite size effect enhances the chiral symmetry breaking for the periodic boundary condition, $δ=0$ [ref] .
Four-Fermion Interaction Model on $\mathcal{M}^{D-1} \otimes S^1$ · Four-fermion interaction model on $ℳ^D-1 ⊗S^1$ · 0.89
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One could also employ other external probes like the electric field $E$ [ref] , the isospin chemical potential $μ_iso$ [ref] , the scalar curvature $R$ [ref] , the rotational angular velocity $ω$ [ref] , and their mixtures [ref] .
Perturbative confinement in thermal Yang-Mills theories induced by imaginary angular velocity · Introduction · 0.90
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