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Silver Blaze Puzzle in 1/Nc Expansions of Cold and Dense QCD Matter
High Energy Physics - Theory · Submitted 10 Mar 2014
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We argue that the confining properties are responsible for the Silver Blaze in the region of m_pi/2 < mu_q < M_B/Nc.
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The abstract, sentence by sentence
We consider quantum chromodynamics (QCD) with Nc colors and Nf quark flavors at finite quark chemical potential mu_q or isospin chemical potential mu_I. We specifically address the nature of the ``Silver Blaze'' behavior in the framework of 1/Nc expansion. Starting with the QCD partition function, we implement Veneziano's Nf/Nc expansion to identify the density onset. We find the baryon mass M_B and the pion mass m_pi appearing from different order of Veneziano's expansion. We argue that the confining properties are responsible for the Silver Blaze in the region of m_pi/2 < mu_q < M_B/Nc. We point out, however, that Veneziano's expansion brings about a puzzling subtlety along the same line as the baryon problem in finite-density quenched simulations. We emphasize that the large-Nc limit can allow for the physical ordering of M_B and m_pi thanks to the similarity to the quenched approximation, while the unphysical ghost quarks contaminate the baryon sector if Nc is finite. We also discuss the ``orientifold'' large-Nc limit that does not quench quark loops.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We consider quantum chromodynamics (QCD) with Nc colors and Nf quark flavors at finite quark chemical potential mu_q or isospin chemical potential mu_I. | background 0.92 | 0.24 | 0.02 | asserted 0.80 |
| s1 | We specifically address the nature of the ``Silver Blaze'' behavior in the framework of 1/Nc expansion. | contribution 0.92 | 0.44 | 0.05 | asserted 0.52 |
| s2 | Starting with the QCD partition function, we implement Veneziano's Nf/Nc expansion to identify the density onset. | method 0.98 | 0.87 | 0.05 | asserted 0.96 |
| s3 | We find the baryon mass M_B and the pion mass m_pi appearing from different order of Veneziano's expansion. | result 0.98 | 0.92 | 0.10 | asserted 1.00 |
| s4 | We argue that the confining properties are responsible for the Silver Blaze in the region of m_pi/2 < mu_q < M_B/Nc. | interpretation 0.93 | 0.79 | 0.46 | asserted 0.86 |
| s5 | We point out, however, that Veneziano's expansion brings about a puzzling subtlety along the same line as the baryon problem in finite-density quenched simulations. | limitation 0.68 | 0.67 | 0.09 | asserted 0.97 |
| s6 | We emphasize that the large-Nc limit can allow for the physical ordering of M_B and m_pi thanks to the similarity to the quenched approximation, while the unphysical ghost quarks contaminate the baryon sector if Nc is finite. | interpretation 0.91 | 0.55 | 0.32 | asserted 0.78 |
| s7 | We also discuss the ``orientifold'' large-Nc limit that does not quench quark loops. | contribution 0.95 | 0.59 | 0.04 | asserted 0.56 |
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The paper
Original abstract
We consider quantum chromodynamics (QCD) with Nc colors and Nf quark flavors at finite quark chemical potential mu_q or isospin chemical potential mu_I. We specifically address the nature of the ``Silver Blaze'' behavior in the framework of 1/Nc expansion. Starting with the QCD partition function, we implement Veneziano's Nf/Nc expansion to identify the density onset. We find the baryon mass M_B and the pion mass m_pi appearing from different order of Veneziano's expansion. We argue that the confining properties are responsible for the Silver Blaze in the region of m_pi/2 < mu_q < M_B/Nc. We point out, however, that Veneziano's expansion brings about a puzzling subtlety along the same line as the baryon problem in finite-density quenched simulations. We emphasize that the large-Nc limit can allow for the physical ordering of M_B and m_pi thanks to the similarity to the quenched approximation, while the unphysical ghost quarks contaminate the baryon sector if Nc is finite. We also discuss the ``orientifold'' large-Nc limit that does not quench quark loops.
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References
How the literature uses it
1 arXiv paper cite this in 2 sentences
Papers citing it · 1 sentence without a confident label
Cites it as background 1 paper
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However, the dominance of the black holes mean also that the Silver Blaze property of QCD (see [ref] ) is lost.
Cool baryon and quark matter in holographic QCD · Asymptotics of $w(ł)$ and the phase structure · 0.88
What it cites · 10 sentences without a confident label
Uses the method or tool of 2 papers
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To this end we exploit the worldline formalism (or the canonical ensemble representation) in order to expand the Dirac determinant in powers of $/$ [ref] (see also arguments in Ref. [ref] ).
QCD With A Chemical Potential, Topology, And The 't Hooft 1/N Expansion · Introduction · 0.98
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To this end we exploit the worldline formalism (or the canonical ensemble representation) in order to expand the Dirac determinant in powers of $/$ [ref] (see also arguments in Ref. [ref] ).
Large-N spacetime reduction and the sign and silver-blaze problems of dense QCD · Introduction · 0.98
Cites as background 6 papers
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Unlike the case with $≪T$, lattice-QCD simulations based on the Monte-Carlo algorithm has a serious difficulty called the sign problem due to a fluctuating phase of the fermion (Dirac) determinant at $≠0$ [ref] .
Lattice QCD at Finite Density -- An introductory review · Introduction · 0.96
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There are several approaches to evade the sign problem; the Taylor expansion [ref] , the re-weighing method [ref] , the imaginary chemical potential [ref] , and the complex Langevin equation [ref] , but they are not yet well-developed to go beyond the small-$/T$ regime.
A new method to study lattice QCD at finite temperature and chemical potential · Introduction · 0.92
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There are several approaches to evade the sign problem; the Taylor expansion [ref] , the re-weighing method [ref] , the imaginary chemical potential [ref] , and the complex Langevin equation [ref] , but they are not yet well-developed to go beyond the small-$/T$ regime.
The QCD thermal phase transition in the presence of a small chemical potential · Introduction · 0.92
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