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Relation between the trace anomaly and the energy-momentum tensor being off-shell

Let's say we have a massless QED theory with a Lagrangian \begin{equation} L=i\bar{\psi}\not{D}\psi-\frac{1}{4}F_{\mu\nu}F^{\mu\nu} \end{equation} The symmetric energy-momentum tensor is \begin{...
P. C. Spaniel's user avatar
5 votes
0 answers
210 views

Is it possible to couple an odd number of Dirac fermions, at finite density, to a massless gauge field in 2+1d?

In a beautiful paper by A. N. Redlich (PRL $\bf{52}$, 18 (1984)) on the parity anomaly, the author indicates that an odd number of Dirac fermions can never be coupled to a massless gauge field in 2+1d ...
hursaido's user avatar
5 votes
0 answers
236 views

Where does chiral matter at conical singularities "come from" in M-theory?

It seems to be accepted that to produce chiral fermionic matter in a compactification $\mathbb{R}^4\times X$ of M-theory/11d SUGRA to four dimensions, we need the seven-manifold $X$ to have isolated (...
ACuriousMind's user avatar
  • 129k
4 votes
2 answers
594 views

Gravitational and gauge-gravitational anomalies in ${\cal N}=1$ $D=4$ supergravity coupled to a SUSY gauge theory with chiral matter

When people talk about the first superstring revolution they often mention the miraculous cancellation of anomalies via the Green-Schwarz mechanism. My question is whether such a string-theoretic ...
stringpheno's user avatar
4 votes
1 answer
328 views

Symmetries: from a classical field theory to quantum

My background about this argument: a) Let's consider a classical field theory, where $\mathcal{L}(\phi(x),\partial_{\mu}\phi_(x))$ is the lagrangian density. A symmetry is a transformation $\phi(x) \...
Antonio19932806's user avatar
4 votes
1 answer
201 views

Critical dimension of ${\cal N}=2$ strings

In "A tour through ${\cal N}=2$ strings" by Neil Marcus (https://arxiv.org/abs/hep-th/9211059) the following problem - among others - is noted: The critical dimension of the ${\cal N}=2$ ...
and008's user avatar
  • 232
4 votes
1 answer
326 views

What does $B+L$ anomaly have to do with a phase redefinition of the left-handed quark field?

According to this answer, the reason why $SU(2)_L$ weak theory does not have a theta vacuum is because any theta term can be reabsorbed with a phase redefinition of the left-handed quark field. ...
Nanashi No Gombe's user avatar
4 votes
1 answer
373 views

"The operators with nontrivial vacuum expectation values have to soak up the zero modes associated to the anomaly."

I was reading ref.1, where one can read (emphasis mine) ... the vacuum expectation value $\langle \mathcal O_{\phi_1}\cdots \mathcal O_{\phi_\ell}\rangle$ vanishes unless $$ \sum_{k=1}^\ell\...
AccidentalFourierTransform's user avatar
4 votes
1 answer
492 views

chiral anomaly and translation symmetry in 1+1D

A Luttinger liquid at low energies can be captured by Dirac fermions in 1+1D, where the two component fermion field is given by $$\Psi(x)=\left(\begin{array}{c}\psi_R(x)\\\psi_L(x)\end{array}\right),$$...
pathintegral's user avatar
  • 1,515
4 votes
1 answer
277 views

Anomalies and determinant bundle curvature

I heard that anomalies and curvature of determinant bundle are related. Namely, curvature of determinant bundle is related to Chern-Simons form (which are involved in description of gauge anomalies). ...
newt's user avatar
  • 546
4 votes
2 answers
1k views

Traces in different representation

I am actually working with Green-Schwarz anomaly cancellation mechanism in which I have came across a strange formula which relates trace in the adjoint representation (Tr) to trace in fundamental ...
user44895's user avatar
  • 672
4 votes
1 answer
201 views

Anomalous global symmetry in non-gauge theories

I’m a bit confused on the effects of anomalous global symmetries. So take for instance the following theory $$\mathscr{L}=\partial_\mu\phi\partial^\mu\phi^*+i\bar{\psi}\gamma_\mu\partial^\mu\psi-y \...
Tom Bouley's user avatar
4 votes
1 answer
219 views

Bosonic SPT phases with time reversal and a $Z_2$ symmetry

Consider a bosonic system with time reversal symmetry $\mathcal{T}$ and a unitary on-site $\mathbb{Z}_2$ symmetry. Suppose the symmetry is realized in a special way such that $$\mathcal{T}^2= (-1)^B$$ ...
user34104's user avatar
  • 417
4 votes
1 answer
520 views

Loop counting for determinants and anomalies

I am trying to understand an argument for why anomalies are one-loop exact, given by Bilal in Lectures on Anomalies. The relevant paragraph is reproduced here: Let us first explain why the anomaly ...
gmarocco's user avatar
  • 485
4 votes
1 answer
310 views

2D anomaly-free condition for a gauge theory

Take a $SU(2)$ gauge theory in 2d spacetime, say there are $n_1$ left-handed Weyl fermion in spin-1 written as $$ 1_L, $$ and $n_0$ left-handed Weyl fermion in spin-0 written as $$ 0_L . $$ and $n_{1/...
ann marie cœur's user avatar
4 votes
1 answer
264 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
  • 8,971
4 votes
1 answer
916 views

Why do we study anomalies with the triangle diagram?

This is a very basic question. Why do we study anomalies by means of the triangle diagram, i.e. the tree-point function of gauge/global currents and not with, for instance, a two point function? In ...
apt45's user avatar
  • 2,237
4 votes
1 answer
298 views

Regularization and renomalization in the lightcone quantization of bosonic string

This question relates to this link. But I still don't understand it >_< In Polchinski's string theory vol I, p. 22, there is a divergence term (when $\epsilon \rightarrow 0$) in the zero point ...
user26143's user avatar
  • 6,451
4 votes
1 answer
225 views

A critical step in Fujikawa's proof of the Atiyah Singer index theorem

If the Riemannian curvature is zero and $\mathrm{dim}(M)=n=2k$, the Atiyah-Singer index theorem for the twisted Dirac operator reduces to the following equation: \begin{equation}\tag{1} \mathrm{ind}(...
Filippo's user avatar
  • 1,911
4 votes
1 answer
162 views

Momentum replacement in the axial anomaly calculation in dimensional regularisation (‘t Hooft prescription)

I have been studying the axial anomaly and everywhere I see the calculation of the triangle loop using dimensional regularisation (see for example pages 661-664 of section 19.2 of Peskin). In the ‘t ...
Roberto Corral's user avatar
4 votes
1 answer
220 views

Can a gauge anomaly be *removed* by quantum corrections?

Consider a classical gauge field coupled to a vector field $j^\mu$. Gauge invariance requires that $\mathcal A_\mathrm{cl}:=\partial_\mu j^\mu$ vanishes: $$ \mathcal A_\mathrm{cl}\equiv 0 $$ In other ...
AccidentalFourierTransform's user avatar
4 votes
1 answer
650 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
  • 719
4 votes
1 answer
980 views

Axial anomaly in QCD VS axial anomaly in current algebra QCD

I would like to understand the distinction between an axial anomaly in QCD (Theta Vacuum: axion -> 2 gluons) and an axial anomaly in QCD of current (Chern–Simons term: pion->two photons, photon->three ...
illuminato's user avatar
4 votes
1 answer
1k views

Why are critical dimensions and central charge linkable?

From wikipedia: "In order for a string theory to be consistent, the worldsheet theory must be conformally invariant. The obstruction to conformal symmetry is known as the Weyl anomaly and is ...
C Worthington's user avatar
4 votes
1 answer
738 views

anomalous chiral symmetry and the $\bar\theta$ parameter

I am studying anomalous $U(1)$'s, related to the strong CP problem, and I have some trouble with the origin of the parameter $\bar{\theta}$. We start with the QCD Lagrangian with the topological ...
Bulkilol's user avatar
  • 609
4 votes
0 answers
47 views

Resources on Advanced Topics in Standard Model: nonperturbative phenomena, phase transitions, etc

I'm interested in some books on Standard Model physics that discuss advanced topics in quantum field theory. By this I mean topics such as instantons, sphalerons, and friends, the electroweak phase ...
4 votes
0 answers
57 views

Gauge Anomalies General scenario using Fujikawa Method

I would like to ask a question about Gauge Anomalies and how we can extract them through the Fujikawa method, without using the general triangle diagram as proposed by Weinberg Volume 2 Chapter 22.3. ...
Anthony1199's user avatar
4 votes
0 answers
141 views

Normalization of zero point energy in string theory

Following Joe Polchinski’s Little Book of String, page 12, he use the sum $$1+2+3+...=-1/12$$ to find the zero point energy of the bosonic string (and later used the result to argue that we must have ...
ziv's user avatar
  • 1,774
4 votes
0 answers
202 views

Stress tensor trace anomaly in two dimensions

I'm trying to calculate the expectation value of the stress tensor in 2D following the book "Quantum fields in curved space" (Birrell and Davies). In 2D the divergent contribution to the one-...
mat5teo's user avatar
  • 61
4 votes
0 answers
206 views

Why 't Hooft anomaly can be described by some characteristic class?

In some recent papers, such as Zohar PhysRevB.97.054418, Zohar arXiv:1705.04786, Metlitski PhysRevB.98.085140, the authors state that the anomaly inflow term/ topological action can be expressed in ...
ZJX's user avatar
  • 868
4 votes
0 answers
121 views

Why are there only two 496-dim. gauge groups $E_8\times E_8$ and $SO(32)$ allowed in string theory? Why not $E_8\times U(1)^{248}$ or $U(1)^{496}$?

While constructing anomaly-free string theories with $\mathcal N=1$ supersymmetry (16 supercharges constituting a Majorana-Weyl spinor), we learn that the gauge group must be 496-dimensional in order ...
Tevatron5's user avatar
4 votes
0 answers
256 views

’t Hooft anomaly matching and massless baryons

In Lectures on Gauge Theory by David Tong there is statement (section 5.6.3 The Vafa-Witten-Weingarten Theorems), that: To invoke the full power of ’t Hooft anomaly matching, we needed to assume that ...
Nikita's user avatar
  • 5,737
4 votes
0 answers
92 views

Anomalies depend on how they are calculated. How is this satisfactory?

If we have a set of linear symmetry currents $J^{\mu}_{\alpha}$ and attempt to find if they are anomalous, we find that if we change the regularization procedure, the anomaly will get mixed around the ...
fewfew4's user avatar
  • 3,544
4 votes
0 answers
312 views

How does the Weyl anomaly imply $\langle T^{\mu}_{\mu} \rangle \neq 0$?

I want to consider the case of euclidean field theory in 2 dimensions with the action $$S[\phi]=\int \! d^2\!x \sqrt{\det(g)}g^{\mu\nu}\partial_\mu\phi\partial_\nu\phi$$ which leads to a partition ...
Leonard's user avatar
  • 261
4 votes
0 answers
194 views

Mathematics of Anomalies in QFT [duplicate]

As a mathematics student interested in theoretical physics, I found it very hard to study about anomalies in QFT in standard physics texts. They concentrate on particular examples (like chiral anomaly)...
4 votes
0 answers
224 views

How can we find the consistent form of the anomaly from the Fujikawa method?

The Fujikawa method to find the chiral anomaly allows us to find for the axial current $$\partial_\mu j^\mu=-\frac{g^2}{16\pi^2}\epsilon^{\mu\nu\rho\sigma} Tr F_{\mu\nu}F_{\rho\sigma},$$ which is the ...
user121664's user avatar
4 votes
0 answers
137 views

The chemical potential as the zeroth component of a constant gauge field

The chemical potential $\mu$, is introduced in the action as the lagrange multiplier $$ \tag 1 S[Q_{0}] \to S[\mu] = S[Q_{0}]-\int dt \mu Q_{0}(t), $$ where $$ Q_{0}(t) = \int d^{3}\mathbf r J_{0}(\...
Name YYY's user avatar
  • 8,971
4 votes
0 answers
115 views

Inconsistency in regularization with parallel and perpendicular momenta

In deriving the axial anomaly Peskin and Schroeder use dimensional regularization, continuing loop momenta to $ 4 - \epsilon $ dimenstions. The loop momenta can now be split into pieces ``parallel'' ...
JeffDror's user avatar
  • 9,005
4 votes
0 answers
660 views

Effective field theories and gauge anomalies cancellation

Lets assume some theory which concludes sets of generations of fermions (lets call them $A$ and $B$). Fermions $A$ have some gauge group $G_{A}$ (for example, SM), while fermions $B$ are charged under ...
Name YYY's user avatar
  • 8,971
4 votes
0 answers
516 views

Anomaly for Majorana fermion?

In 4-spacetime dimension, is there U(1) gauge field chiral anomaly associated with Majorana fermion (or I am not sure if it is equivalent, majorana representation)? Besides, I have read from several ...
qc2014's user avatar
  • 531
4 votes
0 answers
187 views

Some fundamental results in QFTs [closed]

In quantum theory we have some principles that guides us, e.g. Pauli's principle. What I am after in this question is a list of fundamental results, be it equation or identities that must hold in a ...
Physics_maths's user avatar
3 votes
3 answers
1k views

Question on Conformal Field Theory

Since every question has to be asked in a seperate topic, I'm asking a question refering to the following topic: Beginners questions concerning Conformal Field Theory In particular I'm referring to ...
mr_conf's user avatar
  • 391
3 votes
1 answer
1k views

The non-abelian chiral anomaly and one-loop diagrams higher than the triangle one

Suppose chiral fermions $\psi$ interacting with gauge fields $A_{\mu,L/R}$. With $P_{L/R} \equiv \frac{1\mp\gamma_{5}}{2}$ and $t_{a,L/R}$ denoting the generators, the corresponding action reads $$ S =...
Name YYY's user avatar
  • 8,971
3 votes
1 answer
8k views

Why are there specifically 10, 11, or 26 dimensions in string theory? [duplicate]

I know that current string theories state that there are 10, 11, or 26 spacetime dimensions in superstring theory, M-theory, and bosonic string theory, respectively. But when I looked up why those ...
DimensionalExpo's user avatar
3 votes
1 answer
174 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
3 votes
2 answers
182 views

Reference request - derivation of $\mathrm{ind}\,D_+=-\frac{1}{8\pi^2}\int\text{tr}\,F\wedge F$

Let $D$ be the Dirac operator. The equation \begin{equation}\tag{1} \mathrm{ind}\,D_+=-\frac{1}{8\pi^2}\int_M\text{tr}\,F^2=-\frac{1}{8\pi^2}\int_MF^a\wedge F^b\ \mathrm{tr}(T_aT_b) \end{equation} is ...
3 votes
1 answer
135 views

If a regularization procedure respects a symmetry, is this symmetry unbroken in perturbation theory?

I read in this paper the statement that a proof that SUSY is preserved in perturbation theory would be the existence of a regularization procedure which respects SUSY (for a particular theory). Is ...
Dwagg's user avatar
  • 2,022
3 votes
1 answer
674 views

Hermiticity of Dirac Operator $\gamma^{\mu}D_{\mu}$ and Expansion in eigenmodes

I'm interested to know under what conditions $\gamma^{\mu}D_{\mu}$ is a hermitian operator. I am studying the Fujikawa method of anomalies and I see that many sources have different answers for this. ...
CStarAlgebra's user avatar
  • 2,816
3 votes
1 answer
776 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
  • 27.2k
3 votes
1 answer
137 views

How is the dimensionful renornalization scale $\mu$ related to break of scale invariance in String Theory?

In the $7.1.1$ of David Tong's String Theory notes it is said the following about regularization of Polyakov action in a curved target manifold: $$\tag{7.3} S= \frac{1}{4\pi \alpha'} \int d^2\sigma \ ...
Генивалдо's user avatar

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