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Flow of Hagedorn singularities and phase transitions in large $N$ gauge theories
High Energy Physics - Theory · Submitted 27 Oct 2019
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We identify two distinct mechanisms for the appearance of physical Hagedorn singularities and center-symmetry changing phase transitions at real positive $\beta$, inflow of singularities from the $\beta=0$ point, and collisions of complex conjugate pairs of singularities.
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The abstract, sentence by sentence
We investigate the singularity structure of the $(-1)^F$ graded partition function in QCD with $n_f \geq 1$ massive adjoint fermions in the large-$N$ limit. Here, $F$ is fermion number and $N$ is the number of colors. The large $N$ partition function is made reliably calculable by taking space to be a small three-sphere $S^3$. Singularites in the graded partition function are related to phase transitions and to Hagedorn behavior in the $(-1)^F$-graded density of states. We study the flow of the singularities in the complex "inverse temperature" $\beta$ plane as a function of the quark mass. This analysis is a generalization of the Lee-Yang-Fisher-type analysis for a theory which is always in the thermodynamic limit thanks to the large $N$ limit. We identify two distinct mechanisms for the appearance of physical Hagedorn singularities and center-symmetry changing phase transitions at real positive $\beta$, inflow of singularities from the $\beta=0$ point, and collisions of complex conjugate pairs of singularities.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We investigate the singularity structure of the $(-1)^F$ graded partition function in QCD with $n_f \geq 1$ massive adjoint fermions in the large-$N$ limit. | contribution 1.00 | 0.89 | 0.06 | asserted 0.91 |
| s1 | Here, $F$ is fermion number and $N$ is the number of colors. | background 1.00 | 0.10 | 0.02 | asserted 0.99 |
| s2 | The large $N$ partition function is made reliably calculable by taking space to be a small three-sphere $S^3$. | method 0.99 | 0.39 | 0.03 | asserted 1.00 |
| s3 | Singularites in the graded partition function are related to phase transitions and to Hagedorn behavior in the $(-1)^F$-graded density of states. | interpretation 0.51 | 0.42 | 0.27 | asserted 1.00 |
| s4 | We study the flow of the singularities in the complex "inverse temperature" $\beta$ plane as a function of the quark mass. | contribution 0.82 | 0.93 | 0.07 | asserted 0.98 |
| s5 | This analysis is a generalization of the Lee-Yang-Fisher-type analysis for a theory which is always in the thermodynamic limit thanks to the large $N$ limit. | background 0.41 | 0.37 | 0.06 | asserted 1.00 |
| s6 | We identify two distinct mechanisms for the appearance of physical Hagedorn singularities and center-symmetry changing phase transitions at real positive $\beta$, inflow of singularities from the $\beta=0$ point, and collisions of complex conjugate pairs of singularities. | result 0.99 | 0.95 | 0.79 | asserted 1.00 |
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Original abstract
We investigate the singularity structure of the $(-1)^F$ graded partition function in QCD with $n_f \geq 1$ massive adjoint fermions in the large-$N$ limit. Here, $F$ is fermion number and $N$ is the number of colors. The large $N$ partition function is made reliably calculable by taking space to be a small three-sphere $S^3$. Singularites in the graded partition function are related to phase transitions and to Hagedorn behavior in the $(-1)^F$-graded density of states. We study the flow of the singularities in the complex "inverse temperature" $\beta$ plane as a function of the quark mass. This analysis is a generalization of the Lee-Yang-Fisher-type analysis for a theory which is always in the thermodynamic limit thanks to the large $N$ limit. We identify two distinct mechanisms for the appearance of physical Hagedorn singularities and center-symmetry changing phase transitions at real positive $\beta$, inflow of singularities from the $\beta=0$ point, and collisions of complex conjugate pairs of singularities.
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References
How the literature uses it
2 arXiv papers cite this in 2 sentences
What it cites · 47 sentences without a confident label
Uses the method or tool of 4 papers
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We took advantage of the small $S^3$ limit $RΛ→0$ to study the partition function using perturbation theory, following Refs. [ref] .
Finite Volume Phases of Large N Gauge Theories with Massive Adjoint Fermions · Introduction · 0.98
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We took advantage of the small $S^3$ limit $RΛ→0$ to study the partition function using perturbation theory, following Refs. [ref] .
Gauge Fields and Space-Time · Introduction · 0.98
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We took advantage of the small $S^3$ limit $RΛ→0$ to study the partition function using perturbation theory, following Refs. [ref] .
The Hagedorn/Deconfinement Phase Transition in Weakly Coupled Large N Gauge Theories · Introduction · 0.98
Cites as background 24 papers
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Gauge theories in this limit were first studied in Refs. [ref] .
Gauge Fields and Space-Time · Introduction · 0.99
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Gauge theories in this limit were first studied in Refs. [ref] .
The Hagedorn/Deconfinement Phase Transition in Weakly Coupled Large N Gauge Theories · Introduction · 0.99
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Gauge theories in this limit were first studied in Refs. [ref] .
The Hagedorn Transition, Deconfinement and N=4 SYM Theory · Introduction · 0.99
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