Category Archives: Blog

Although Feynman diagrams are often first encountered in statistical/quantum field theory contexts where they are employed in perturbative calculations of partition/correlation functions based on Wick’s theorem, there is a lot of “fluff” in these cases that obscures their underlying simplicity. … Continue reading →

Problem #\(1\): What is the Landau-Ginzburg free energy functional \(F[m]\) for the Ising model? Solution #\(1\): It is defined implicitly through: \[e^{-\beta F[m]}=\sum_{\{\sigma_i\}\to_{\text{c.g.}}m(\textbf x)}e^{-\beta E_{\{\sigma_i\}}}\] where \(E_{\sigma_i}=-E_{\text{ext}}\sum_{i=1}^N\sigma_i-E_{\text{int}}\sum_{\langle i,j\rangle}\sigma_i\sigma_j\) is the energy of a given spin microstate \(\{\sigma_i\}\) and “\(\text{c.g.}\)” is … Continue reading →

Problem #\(1\): Define the Poincaré group. Solution #\(1\): In words, the Poincaré group is the isometry group of Minkowski spacetime \(\textbf R^{1,3}\). Mathematically, it is the semidirect product \(\textbf R^{1,3}⋊O(1,3)\) of the normal subgroup \(\textbf R^{1,3}\) of spacetime translations with … Continue reading →

Problem #\(1\): Write down a general \(\phi\)-dependent perturbation to the Klein-Gordon Lagrangian density \(\mathcal L\) for a real scalar field \(\phi\), and explain why in practice only the first \(2\) terms of such a perturbation need to be considered. Solution … Continue reading →

The purpose of this post is to explain what the toric code is, and its potential use as a fault-tolerant quantum error correcting stabilizer surface code for topological quantum computing. To begin, consider an \(N\times N\) square lattice \(\Lambda\) with … Continue reading →

The purpose of this post is to explain why, experimentally, one only observes \(4\) electric dipole transitions in the IR spectrum of buckminsterfullerene, also known as \(\text C_{60}\) or informally as the buckyball: Buckyball Basics The simplest conceptual way to … Continue reading →

The purpose of this post is to explain several techniques for laser cooling and laser trapping of atoms. In order to better emphasize key conceptual points, it will take the approach of posing problems, followed immediately by their solutions. Problem … Continue reading →

The purpose of this post is to review the theory behind several standard amplitude-splitting interferometers. Michelson Interferometer The simplest possible version of a Michelson interferometer is the following: For now, consider for simplicity a monochromatic light source of frequency \(\omega=ck=nvk=n’v’k=n^{\prime\prime}v^{\prime\prime}k\). … Continue reading →

The purpose of this post is to review several mechanisms that broaden the shape of spectral lines, whether these be absorption or emission spectra (it seems that there are no such things as “narrowing mechanisms” for spectral lines). Roughly speaking, … Continue reading →

The purpose of this post is to explain how Boltzmann’s equation in kinetic theory arises. Problem #\(1\): Write down Liouville’s equation from classical Hamiltonian mechanics governing the incompressible phase space flow (i.e. time evolution) of the joint probability density function … Continue reading →