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9 votes
2 answers
796 views

How is the pion related to spontaneous symmetry breaking in QCD?

In chapter 19 of An Introduction to Quantum Field Theory by Peskin & Schroeder, they discuss spontaneous symmetry breaking (SSB) at low energies in massless (or nearly massless) QCD, given by $$\...
Flynn Linton's user avatar
2 votes
0 answers
69 views

Goldstone bosons in 2 and 3 quark flavor symmetries [closed]

In my (undergraduate) advanced elementary particles class last semester, we learnt that for a 2 quark (u/d) model the symmetry of the Lagrangian is (and breaks as) $$ U(2)_L \otimes U(2)_R = SU(2)_L \...
Yaezir's user avatar
  • 23
3 votes
1 answer
170 views

$U(1)_A$ effects on the baryons?

We know that the axial $U(1)_A$ is anomalous thus not a global symmetry. Therefore there is no direct associated pseudo goldstone boson for $U(1)_A$. This makes the $\eta'$ much more massive than the ...
ann marie cœur's user avatar
8 votes
1 answer
476 views

Why do we think that the $U(1)$ problem is solved by instantons?

It is usually thought that the $U(1)$ problem is solved when 't Hooft realized that instantons induce additional symmetry breaking of the $U(1)_A$ symmetry aside from the non-vanishing quark masses. ...
Wein Eld's user avatar
  • 3,691
2 votes
1 answer
531 views

Peskin's treatment of Pions as Goldstone Bosons

After restoring the mass terms in the Lagrangian \begin{align} \mathcal{L}=\bar{u} i \not D u+\bar{d i} \not D d-m_{u} \bar{u} u-m_{d} \bar{d} d, \end{align} one obtains equations of motion for the ...
user4580791's user avatar
19 votes
1 answer
2k views

What's the real resolution of the $U(1)_A$ problem?

To recap the problem, consider QCD with three massless quark flavors. There is a symmetry $$SU(3)_L \times SU(3)_R \times U(1)_L \times U(1)_R$$ corresponding to independent rotations of the left-...
knzhou's user avatar
  • 103k
3 votes
1 answer
745 views

Is it the chiral anomaly which is solely responsible for having instanton effects (and therefore, the $\theta-$term) in the QCD action?

$\textbf{Fact 1}$ In principle, the QCD Lagrangian should contain a Lorentz invariant, gauge invariant, dimension-4 term $\sim\theta \text{Tr}[F^{\mu\nu}\tilde{F}_{\mu\nu}]$. This term, however, is ...
SRS's user avatar
  • 26.8k
4 votes
1 answer
611 views

Anomalies of QCD

I have come across the following statement: The anomalies of QCD cannot be reproduced by a collection of free fermions carrying $U(1)_V$, $SU(N_f)_L$ and $SU(N_f)_R$ quantum numbers. That is why ...
QGravity's user avatar
  • 699
3 votes
1 answer
206 views

Counting number of gluon fields in ABJ anomaly of QCD

In QCD, the axial singlet quark current $j_5$ is anomalous, which was found by Adler, Bell, and Jackiw (here is a review): \begin{equation} \partial_\mu j_5^\mu=G\tilde{G}, \end{equation} where $G$ ...
Thomas's user avatar
  • 1,783
3 votes
1 answer
430 views

Computation of theta-term from triangle diagram

The chiral $U(1)$ anomaly in QCD can be calculated exactly by one-loop Feynman diagrams, for example by the famous triangle diagram. I am currently performing the computation to get a better ...
Thomas's user avatar
  • 1,783