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1 vote
2 answers
240 views

Sufficient and Necessary Conditions for Chiral Symmetry Breaking

In their 2005 paper, the authors write (just below eq. 3.19) we see that a non-zero value of $F_0$ is a necessary and sufficient criterion for spontaneous chiral symmetry breaking. On the other ...
ersbygre1's user avatar
  • 2,648
2 votes
1 answer
260 views

Why is the approximate $\rm U(2)\times U(2)$ global symmetry of QCD that has a special importance?

I was looking at Peskin and Schroeder (Section 19.3, page $667-668$). They talk about $\rm U(2)\times U(2)$ symmetry for the QCD Lagrangian in the limit of massless $u$ and $d$ quarks. However, this ...
SRS's user avatar
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1 vote
1 answer
279 views

Group structure of QCD‘s chiral symmetry (breaking)

With $3$ flavors of massless quarks, the QCD Lagrangian is invariant under flavor transformations$$SU(3)_V\ \otimes\ SU(3)_A\ \otimes\ U(1)_V\ \otimes\ U(1)_A.$$ Now, this is equivalent to $$SU(3)_R\ \...
ersbygre1's user avatar
  • 2,648
1 vote
2 answers
379 views

Derivation of Casher-Banks relation

Consider two-point function $\langle \bar{\psi}\psi\rangle$ in a model with massive fermions $\psi$ and gauge field: $$ \langle \bar{\psi}\psi\rangle =\frac{1}{V}\sum_{n} \frac{1}{\lambda_{n} +im}, $$...
Name YYY's user avatar
  • 8,901
4 votes
1 answer
248 views

Simple explanation of the QCD VEV in terms of instantons

I've heard that instantons in QCD generate quark bilinear condensate $\langle \bar{q}_{L}q_{R}\rangle$ which is responsible for spontaneous symmetry breaking. Is there any clear and simple way to ...
Name YYY's user avatar
  • 8,901
2 votes
0 answers
86 views

No global monopoles in QCD

If a global symmetry gets both spontaneously and explicitly broken, the explicit symmetry breaking pattern is crucial for understanding the formation of topological defects. For example, in the axion ...
Thomas's user avatar
  • 1,783
1 vote
0 answers
46 views

Do hierarchical condensates yield instantaneous or sequential symmetry breaking?

I am wondering whether the formation of a hierarchical vacuum condensate yields an instantaneous or sequential symmetry breaking in a cosmological phase transition. Let me illustrate this question ...
Thomas's user avatar
  • 1,783
1 vote
2 answers
1k views

Breaking of $SU(3)$ symmetry by bi-fundamental representation

Are there any general theorems which fix the possible symmetry breaking patterns of Lie groups (such as $SU(3)$) by vacuum expectation values of fields in specific representations (such as the quark ...
Thomas's user avatar
  • 1,783
2 votes
1 answer
141 views

gauge-invariant 6-quark order parameter

In this Review paper in p.1462, bottom left: Rev.Mod.Phys.80:1455-1515,2008 -- Color superconductivity in dense quark matter It says that "There is an associated gauge-invariant 6-quark order ...
ann marie cœur's user avatar
0 votes
1 answer
147 views

chiral symmetry condensate and 2SC, CFL breaking C, P and T symmetry?

Because we know that chiral symmetry condensate causes the chiral symmetry breaking, and it produces Goldstone modes of pseudo-scalars, so I believe that chiral symmetry breaking also breaks the T ...
ann marie cœur's user avatar
8 votes
1 answer
2k views

Peccei-Quinn-symmetry and effective Lagrangian for the Axion field

To solve the strong CP-problem Peccei and Quinn suggested the use of a new $U(1)$-symmetry called the PQ-symmetry. For this symmetry they constructed an effective Lagrangian involving the Nambu-...
Alpha001's user avatar
  • 1,114
3 votes
1 answer
403 views

Scalar pseudo-Goldstones from hypothetical $SU(3)_V$ symmetry breaking in QCD

The eight light pseudoscalar mesons of QCD are the pseudo-Goldstone bosons of the spontaneously broken chiral (axial) $SU(3)_A$ quark flavor symmetry. If we consider the hypothetical case of also ...
Thomas's user avatar
  • 1,783
1 vote
0 answers
195 views

Why does the $U(2n)$ flavor symmetry break down to a $U(1)$ group and an $SU(2n)$ group?

I am studying quantum field theory using Srednicki's textbook. Problem 83.1 is: Suppose that the color group is $G_C=SO(3)$ rather than $SU(3)$, and that each quark flavor is represented by a Dirac ...
Shen's user avatar
  • 1,653
9 votes
1 answer
739 views

Why do we have a non-zero quark vacuum condensate even though the QCD coupling goes to zero in the deep infrared?

It is well-known that QCD has a Landau pole at $\Lambda_{\rm QCD}\sim 200$ MeV, which means that the perturbative QCD coupling becomes strong at this scale. Conventionally, this is claimed to be the ...
Thomas's user avatar
  • 1,783
4 votes
1 answer
2k views

Question about the linear sigma-model

Suppose the linear sigma-model lagrangian: $$ L = \bar{N}(i\gamma_{\mu}\partial^{\mu}-g_A \phi)N + |\partial_{\mu}\phi|^{2} - V(|\phi|) - c\sigma , $$ where $$ N = \begin{pmatrix} p \\ n\end{pmatrix}, ...
Name YYY's user avatar
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