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The finite-temperature chiral transition in QCD with adjoint fermions
High Energy Physics - Theory · Submitted 2 Dec 2004
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim The finite-temperature chiral transition in two-flavor aQCD can therefore be continuous; in this case its critical behavior is determined by this new SU(4)/SO(4) universality class.
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The abstract, sentence by sentence
We study the nature of the finite-temperature chiral transition in QCD with N_f light quarks in the adjoint representation (aQCD). Renormalization-group arguments show that the transition can be continuous if a stable fixed point exists in the renormalization-group flow of the corresponding three-dimensional Phi^4 theory with a complex 2N_f x 2N_f symmetric matrix field and symmetry-breaking pattern SU(2N_f)->SO(2N_f). This issue is investigated by exploiting two three-dimensional perturbative approaches, the massless minimal-subtraction scheme without epsilon expansion and a massive scheme in which correlation functions are renormalized at zero momentum. We compute the renormalization-group functions in the two schemes to five and six loops respectively, and determine their large-order behavior. The analyses of the series show the presence of a stable three-dimensional fixed point characterized by the symmetry-breaking pattern SU(4)->SO(4). This fixed point does not appear in an epsilon-expansion analysis and therefore does not exist close to four dimensions. The finite-temperature chiral transition in two-flavor aQCD can therefore be continuous; in this case its critical behavior is determined by this new SU(4)/SO(4) universality class. One-flavor aQCD may show a more complex phase diagram with two phase transitions. One of them, if continuous, should belong to the O(3) vector universality class.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We study the nature of the finite-temperature chiral transition in QCD with N_f light quarks in the adjoint representation (aQCD). | contribution 0.90 | 0.87 | 0.03 | asserted 0.53 |
| s1 | Renormalization-group arguments show that the transition can be continuous if a stable fixed point exists in the renormalization-group flow of the corresponding three-dimensional Phi^4 theory with a complex 2N_f x 2N_f symmetric matrix field and symmetry-breaking pattern SU(2N_f)->SO(2N_f). | background 0.98 | 0.17 | 0.09 | hedged possibility 0.75 |
| s2 | This issue is investigated by exploiting two three-dimensional perturbative approaches, the massless minimal-subtraction scheme without epsilon expansion and a massive scheme in which correlation functions are renormalized at zero momentum. | method 0.99 | 0.72 | 0.02 | asserted 0.97 |
| s3 | We compute the renormalization-group functions in the two schemes to five and six loops respectively, and determine their large-order behavior. | method 0.84 | 0.96 | 0.03 | asserted 1.00 |
| s4 | The analyses of the series show the presence of a stable three-dimensional fixed point characterized by the symmetry-breaking pattern SU(4)->SO(4). | result 1.00 | 0.92 | 0.48 | asserted 1.00 |
| s5 | This fixed point does not appear in an epsilon-expansion analysis and therefore does not exist close to four dimensions. | result 0.55 | 0.54 | 0.08 | asserted 1.00 |
| s6 | The finite-temperature chiral transition in two-flavor aQCD can therefore be continuous; in this case its critical behavior is determined by this new SU(4)/SO(4) universality class. | interpretation 0.85 | 0.79 | 0.80 | hedged possibility 0.60 |
| s7 | One-flavor aQCD may show a more complex phase diagram with two phase transitions. | result 0.65 | 0.41 | 0.04 | hedged possibility 1.00 |
| s8 | One of them, if continuous, should belong to the O(3) vector universality class. | interpretation 0.53 | 0.35 | 0.04 | hedged possibility 0.91 |
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Original abstract
We study the nature of the finite-temperature chiral transition in QCD with N_f light quarks in the adjoint representation (aQCD). Renormalization-group arguments show that the transition can be continuous if a stable fixed point exists in the renormalization-group flow of the corresponding three-dimensional Phi^4 theory with a complex 2N_f x 2N_f symmetric matrix field and symmetry-breaking pattern SU(2N_f)->SO(2N_f). This issue is investigated by exploiting two three-dimensional perturbative approaches, the massless minimal-subtraction scheme without epsilon expansion and a massive scheme in which correlation functions are renormalized at zero momentum. We compute the renormalization-group functions in the two schemes to five and six loops respectively, and determine their large-order behavior. The analyses of the series show the presence of a stable three-dimensional fixed point characterized by the symmetry-breaking pattern SU(4)->SO(4). This fixed point does not appear in an epsilon-expansion analysis and therefore does not exist close to four dimensions. The finite-temperature chiral transition in two-flavor aQCD can therefore be continuous; in this case its critical behavior is determined by this new SU(4)/SO(4) universality class. One-flavor aQCD may show a more complex phase diagram with two phase transitions. One of them, if continuous, should belong to the O(3) vector universality class.
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References
How the literature uses it
8 arXiv papers cite this in 20 sentences
Papers citing it · 17 sentences without a confident label
Compares with it 1 paper
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These conditions are the same as what is found in analyses of the single-irrep subsectors of the potential [ref] , and so irrep coupling does not seem to affect which $χ$SB pattern is realized.
Stability Analysis of the Chiral Transition in SU(4) Gauge Theory with Fermions in Multiple Representations · Constraints due to Vacuum Stability and $χ$SB Pattern · 0.83
Cites it as background 2 papers
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In Sec. [ref], we review the results of the calculation for the single-irrep subsectors of the theory, which have been examined previously [ref] and whose fixed points span a subset of the fixed points of the full theory (see Sec. [ref] for discussion).
Stability Analysis of the Chiral Transition in SU(4) Gauge Theory with Fermions in Multiple Representations · Introduction · 0.82
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This implies that, in the case of a continuous chiral transition (note however that the transition may be also first order independently of the symmetry breaking), the critical behavior belongs to different 3D universality classes in the two cases [ref] .
Theta dependence of 4D SU(N) gauge theories at finite temperature · Introduction · 0.84
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