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Questions tagged [gauge-invariance]

Invariance of a physical system (its action) under a continuous group of local transformations underlain by a global symmetry whose group parameters fixed in space-time have now been extended to vary in space-time instead. Use for buildup of the invariance, fixing the gauge, and accounting for the corresponding changes in the functional measure of the system.

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Suppose a theoretical physicist wants to construct a theory to explain some newly discovered phenomenon. The new theory is expected to follow certain rules or fundamental principles. There are four ...
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For the sake of context suppose a euclidean pure Yang Mills theory with gauge group SU(2) for the rest of this question. The terms large and small gauge transformations are used around in two ...
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In Henneaux & Teitelboim (Quantization of Gauge Systems, p. 30), they discuss the variation of a dynamical variable $$ \delta F = \int d^nx\, u(x)\,\{F, C(x)\}_{PB},\tag{1.62} $$ where $C(x)$ is a ...
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According to Wigner's classification, any massless particle (except for scalars) has 2 degrees of freedom i 4D. This reduction is usually understood in terms of gauge invariance. For instance, a ...
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In Special Relativity, is it mathematically possible for a local, gauge-invariant field theory to have only one vector field $A_\mu$ and to have $U(1)$ symmetry, assuming the vector field $A_\mu$ and/...
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The charge density $\rho(\mathbf{x},t)$ and current density $\mathbf{j}(\mathbf{x},t)$ due to a point charge $q$ following a trajectory $\mathbf{r}(t)$ with velocity $\mathbf{v}(t)=d\mathbf{r}/dt$ is ...
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In a previous question regarding large gauge transformations, one of the answers mentions that large gauge transformations are true redundancies for classical gauge theories, while they contain ...
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A typical opinion is that a gauge transformation doesn't change physical states, but a global transformation does. However, it's clear that global transformation is a subset of gauge transformation, ...
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As the title suggests I am trying to understand the idea behind these identities and in order to do so, I will describe below, an example provided to us in the lecture. Once I understand how these ...
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For the sake of generality, I am not considering any specific scenario or field theory in particular. Instead, if we consider some arbitrary field theory of choice and also global and local ...
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I was reading an article by Weinberg that introduced the unitary gauge ("General Theory of Broken Local Symmetries", 1) at the classical level for a lagrangian $L$ of standard model-type, ...
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I am reading Tong's notes about string theory, the second chapter, and I encountered this part that I don't know how is derived. We are considering the worldsheet $(\tau,\sigma)$ whose gauge we set to ...
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I'm taking at look at QED foundations, and started thinking about how it relates to Dirac's Equation. Dirac spinors are invariant under a global phase transformation $\psi(x)\mapsto e^{i\alpha}\psi(x)$...
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Consider the Lorenz gauge condition \begin{equation} \partial_\mu A^\mu = 0. \tag{1} \end{equation} Suppose there exists a field configuration $B^\mu$ that satisfies the Lorenz gauge, and another ...
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This question is related to different motivations for the need of gauge invariance in QFT. I was introduced to gauge invariance in the following way. Consider a vector field $A^\mu(x)$, with $x\equiv ...
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Summary: Equation of motion (EOM) for the electromagnetic 4-potential $A^\mu$ is non-invertible. Allegedly, this makes it impossible to determine the Green's function, and complicates quantisation of ...
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I am quoting the Aharonov-Bohm paper "We shall show that, contrary to the conclusions of classical mechanics, there exist effects of potentials on charged particles" Consider a region ...
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Schwartz shows in section 9.4 (on SCALAR QED) that the amplitude of diagram (9.41) is not gauge invariant on its own, but once we add the amplitude of (9.43) we get a gauge independent result. Now, ...
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In the NRQM'al theory of a charged particle, if we gauge transform the potentials using some arbitrary gauge function $\Lambda(\textbf{X},t)$ then Schrodinger's equation implies that the quantum state ...
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In particle physics, one checks the invariance of the Lagrangian under global transformations of the fields $\psi\rightarrow e^{i\alpha}\psi$ and local transformations $\psi\rightarrow e^{i\alpha(x)}\...
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In quantum mechanics, we know that: The global phase of a wavefunction does not have any physical effect, but the relative difference in phase ($\Delta \phi$) among different components of the same ...
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In page 109 of Weigand's QFT note (https://www.physics.umd.edu/grt/taj/624b/WeigandQFT.pdf), he defined a general polarization 4-vector $$ \zeta^\mu=\sum_{\lambda,\lambda'}\alpha_\lambda\eta_{\lambda\...
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I am reading a paper on gauge-invariant description of gauge theories on a lattice. In p.$564$ formula $(6.1)$ of the paper, a complete set of gauge-invariant composite fields for an $SU(2)$ theory ...
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The origin of Meissner effect is the Anderson Higgs mechanism (see page 82 https://www-thphys.physics.ox.ac.uk/people/SteveSimon/QCM2019/QuantumMatter.pdf), where the global $U(1)$ phase symmetry of ...
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I can't understand the heuristic proof of $Z_1 = Z_2$ in the beginning of section 19.5 in Schwartz's "QFT and the SM". Basically, he considered a theory with an electron and a quark: $$\!\!\!...
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So, in Weyl gauge (A^{0} = 0) all physical states must obey Gauss's law. But that even makes the vacuum state (which is the Dirac sea tensor with the free EM vacuum) unphysical. Then, how do you ...
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When looking at What, in simplest terms, is gauge invariance? question, the OP in the last paragraph asks this: In many high school physics calculations, you measure or calculate time, distance, ...
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I'm trying to get my head around derivations of the PN and PPN order metric and Lagrangian in GR. Especially concerning the coordinate transformations to switch between the different gauges. I know ...
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How would the mathematics of electromagnetism and physical interpretation change if the gauge used a difference instead of a sum? In other words, what would this gauge do: $$\frac{1}{c}\frac{\partial \...
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For a general Yang-Mills theory, we have the field strength $$F_{\mu\nu} = \partial_\mu A_\nu - \partial_\nu A_\mu - ig [A_\mu, A_\nu]$$ I now want to prove that it transforms as $$F_{\mu\nu} \...
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Suppose we are working in scalar QED with Lagrangian $$\mathscr{L} = (D_\mu \phi)(D^\mu \phi)^* - \frac{1}{4}F_{\mu\nu}F^{\mu\nu}.$$ I now want to find the form of the covariant derivative $D_\mu$ ...
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In Baumann's Cosmology, he discusses a few aspects of adiabatic perturbations on Sec. 6.2.2. He states (p. 229) Adiabatic perturbations can be created by starting with a homogeneous universe and ...
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The Witten anomaly restricts the number of fermion doublets in an $SU(2)$ theory. If we have a gauge group $SU(2)_1 \times SU(2)_2$ and have only one fermion fundamental $\psi = (2,2)$, is this theory ...
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QED and QFT take $U(1)$ gauge symmetry as fundamental and obtain extremely successful predictions at the scales and experiments physicists have been able to perform. This should not be taken lightly. ...
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If there are two symmetries of a Lagrangian, perhaps they are transformations, $A$ and $B$, and they don't commute $[A, B] \neq 0.$ Let this act on some field, then if $(BA)^{-1}AB$ does not return ...
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When dealing with quantum field theory in curved spacetime, a spin connection field is introduced as a result of the Lorentz symmetry. I'm wondering what would be intuitively considered as "...
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I'm currently reading the book Quantum Paradoxes: Quantum Theory for the Perplexed by Aharonov and Rohrlich and in chapter 4 they show the existence of AB effect. I'm already familiar with the ...
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So the rule is that if you change the field by multiplying it by a phase factor that varies you get a different equation, so to compensate for this you change the derivative operator to get rid of the ...
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Let $$L = \int \frac{J(a,b)}{2}\dot{x}^2-p(x_a^2+x_b^2-J(a,b)) da da$$ where $p$ is a Lagrange multiplier, $x=x(a,b,t)$ and $dx/dt = \dot{x}$. This Lagrangian corresponds to the following dynamics $$ ...
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From Polchinski's String Theory: Point-particle example Let us consider an example, the point particles. Expanding out the condensed notation above, the local symmetry is coordinate ...
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The basic definition of principal bundles involves free and transitive action of the group $G$. And, it is well-known that classical Yang-Mills are modelled on principal bundles, where $G$ corresponds ...
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Can we introduce a worldsheet gauge field in Polyakov action? In superstring theory we need to be careful about anomaly cancellation, supersymmetry which fix the field content of worldsheet. Is there ...
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In the book "String theory and M-theory" by Becker-Becker-Schwarz, the author says that "reparametrization invariance of the string sigma-model action $$S_{\sigma}=\frac{-T}{2}\int d^2 ...
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I'm a math student and I started studying physics last year. I'm sorry if this question has been asked before but I'm completely confused about it. In page 30 of the book "String theory and M-...
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As we all know, cutoff regularization doesn’t work for gauge theory. So won’t the traditional Wilson RG work in gauge theory since it involves explicit cutoff for the same reason.
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For Bloch electrons $\psi_{nk}=e^{ikr}u_{nk}$, with $k$ the crystal momentum and $n$ the band index, I would like to know if the integral ($m \neq n, k^\prime \neq k$) $$ \langle u_{nk}|u_{nk^\prime}\...
Xiaoming Wang's user avatar
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I'm trying to understand the algebraic method of formulating the Landau level problem better. I'm referring to David Tong's notes on the Quantum Hall effect for this (but not exactly following his ...
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In EM theory, we can find first-class primary constraint, $$\Pi^{0}(x) = 0\tag{1}$$ and first-class secondary constraint, $$\partial_{i} \Pi^{i}(x) = 0\tag{2}$$ with Lagrangian $$\mathcal{L} = -(1/4)F^...
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On page 298 in Peskin and Schroeder, the authors attempt to argue that the $S$-matrix should be independent of the $\xi$-gauge in QED. However, I don't understand their argument, in particular the ...
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Feynman makes an analogy between EM field and gravity field in his Feynman's Lectures on Gravitation. The vector field representing EM potential would couple to the current source(vector) in the ...
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