Category Archives: Blog

Problem: Distinguish between the terms “intrinsic semiconductor” and “extrinsic semiconductor“. Solution: An intrinsic semiconductor is pretty much what it sounds like, i.e. a “pure” semiconductor material like \(\text{Si}\) that is undoped with any impurity dopants. An extrinsic semiconductor is then … Continue reading →

Problem: A vibrating string with displacement profile \(y(x,t)\) has non-uniform mass per unit length \(\mu(x)\) and non-uniform tension \(T(x)\) experiences both an internal restoring force due to \(T(x)\) but also a linear “Hooke’s law” restoring force \(-k(x)y(x)\) everywhere so that … Continue reading →

Learning physics is hard. The purpose of this post is to collect a bunch of techniques that can help to make the process of learning (and remembering!) new concepts easier. Trick #\(1\): Avoid always simplifying formulas as much as possible, … Continue reading →

The purpose of this post is to lay the foundations for what any experimental physicist should know when it comes to analyzing their experimental data in a rigorous and thoughtful manner. Problem: How does on reduce random error? How does … Continue reading →

Just as the fundamental theorem of single-variable calculus \(\int_{x_1}^{x_2}f'(x)dx=f(x_2)-f(x_1)\) is the key insight on which the entire subject of single-variable calculus rests, there is an analogous sense in which one can consider a fundamental theorem of classical computing to be … Continue reading →

Problem #\(1\): Given a linear operator \(H\) on some Hilbert space, define the resolvent operator associated to \(H\). Solution #\(1\): The resolvent \(G_H(E)\) of \(H\) is the operator-valued Mobius-like transformation of a complex variable \(E\in\textbf C\) defined by the matrix … Continue reading →

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 →