Lecture Notes – Topological Moiré Bands, Fractional Chern Insulators, and Advanced Topics

Collected from 2026 Summer School and various workshops

Posted by Maggie on July 19, 2026

This page collects lecture notes from Prof. Fengcheng Wu (Wuhan University), Prof. K.T. Law, and additional contributors on topics including topological moiré bands, fractional Chern insulators, quantum Monte Carlo sign problems, higher‑form symmetries, quantum anomalies, conformal field theory, BCS superconductivity, quantum geometry, Anderson localization, and Friedel oscillations. All PDFs are stored in the PPTX/ folder.

I. Topological Moiré Bands & Fractional Chern Insulators

Lecture notes from Prof. Fengcheng Wu's series at the 2026 Greater Bay Area Quantum Science Summer School. Topics include topological moiré bands, integer and fractional quantum anomalous Hall effects, collective excitations, and non‑Abelian fractional quantum states.

📘 Lecture 2.2 – Topological Moiré Bands

Theory of topological bands in moiré superlattices, including continuum models, layer‑pseudospin skyrmions, quantum geometry, and Wilson loop methods.

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📘 Lecture 3.1 – Integer Chern Insulators & Competing States in tMoTe₂

Quantum anomalous Hall insulators based on the Kane‑Mele‑Hubbard model, Hartree‑Fock approximation, and phase diagrams with competing orders in tMoTe₂.

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📘 Lecture 3.2 – Collective Excitations

Collective excitations in integer QAHIs: excitonic optical response (Bethe‑Salpeter equation) and topological magnons, plus spin models and domain walls.

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📘 Lecture 4 – Abelian & Non‑Abelian Fractional Chern Insulators in tMoTe₂

Lattice analogs of fractional quantum Hall effects: skyrmion picture, generalized Landau levels, ideal vs. nonideal quantum geometry, and Abelian (Jain sequences) as well as non‑Abelian (\(\nu = 5/2\)) fractional states.

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II. Supplementary Lecture Notes

Additional notes from various sources, covering quantum Monte Carlo sign problems, higher‑form symmetries, quantum anomalies, and conformal field theory.

II-A. Quantum Monte Carlo & The Sign Problem

A comprehensive review of the fermion sign problem in QMC, its origin, mitigation strategies, and complexity‑theoretic limits.

📘 The Sign Problem in Quantum Monte Carlo

Author: Xiao Yan Xu

Pedagogical exposition covering negative/complex weights in SSE, world‑line, and DQMC; average sign and reweighting cost; structural cures (Marshall rotations, determinant pairing, fermion bags, merons, Majorana positivity); and fundamental limits (NP‑hardness, stoquastic‑basis search, topological obstructions).

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II-B. Higher‑Form Symmetry & Quantum Anomalies

Modern generalized symmetries and 't Hooft anomalies, illustrated via the compact boson, Maxwell theory, and a (0+1)‑dimensional Dirac fermion.

📘 Compact Boson, Duality, Gauging, and Anomalies

Source: Summer school handout

Self‑contained tour of 1+1D compact boson: momentum/winding \(\mathrm{U}(1)\) symmetries, mixed anomaly, T‑duality, discrete gauging, emergent dual symmetries, BF pairing, Kramers‑Wannier duality, and generalization to higher‑form symmetries in Maxwell theory (electric/magnetic 1‑form symmetries, Coulomb/Higgs/confined phases).

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📘 量子反常简介('t Hooft Anomaly)

Author: 姚元 (Yuan Yao)

Elementary introduction using a (0+1)‑dimensional Dirac fermion on a thermal circle. Shows the conflict between local \(\mathrm{U}(1)\) gauge invariance and global charge conjugation, leading to a mixed anomaly; demonstrates anomaly inflow and proves that anomalous symmetries imply ingappability.

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II-C. Conformal Field Theory

A pedagogical introduction to 2D CFT, from conformal transformations and the Virasoro algebra to unitary minimal models and the critical Ising model.

📘 Conformal Field Theory – From Basics to Minimal Models

Author: 朱伟 (Wei Zhu)

Self‑contained notes covering: conformal transformations in \(d\) dimensions, primary fields and correlation functions, holomorphic nature in 2D, Witt and Virasoro algebras, central charge, radial quantization, state‑operator correspondence, OPE, highest‑weight representations, Kac determinant, unitary minimal models, and the critical Ising model as a worked example (fusion rules, critical exponents).

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III. K.T. Law Lecture Series – Superconductivity, Quantum Geometry, and Disorder

Graduate lecture series by Prof. K.T. Law covering the microscopic theory of superconductivity (Cooper problem & BCS), quantum geometry in flat‑band superconductivity, Fermi‑velocity‑controlled length scales, Friedel oscillations, and Anderson localization in one dimension. Includes both Beamer slides and detailed lecture notes.

III-A. Cooper Problem & BCS Theory of Superconductivity

The two pillars of microscopic superconductivity: Cooper's instability and the BCS variational ground state.

📊 Beamer – The Cooper Problem

Type: Presentation slides

Introduction to the Cooper problem: physical setup, trial wavefunction, two‑body Schrödinger equation, model interaction, self‑consistency, and bound‑state energy \( \Delta = 2\hbar\omega_D e^{-2/N(0)V} \). Emphasizes the essential singularity and instability of the normal state.

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📊 Beamer – From the Cooper Pair Problem to the BCS Ground State

Type: Presentation slides

Bridge from single‑pair Cooper problem to full BCS many‑body state: reduced BCS Hamiltonian, variational wavefunction \( |\Psi_{\mathrm{BCS}}\rangle = \prod_k (u_k + v_k c_{k\uparrow}^\dagger c_{-k\downarrow}^\dagger)|0\rangle \), energy minimization, gap parameter, coherence factors, pair amplitude \( g_k \), gap equation, and condensation energy.

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📘 Lecture Note – The Cooper Problem (Concise)

Type: Lecture notes

Concise written derivation of the Cooper problem: motivation, trial wavefunction, amplitude equation, model interaction, bound‑state energy, and physical significance.

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📘 Lecture Note – Cooper Problem & BCS Theory (Full)

Type: Comprehensive lecture notes

Complete written version covering both Cooper problem and full BCS variational treatment: two‑body Schrödinger equation, model interaction, bound‑state energy, reduced BCS Hamiltonian, BCS trial wavefunction, energy minimization, coherence factors, pair amplitude, gap equation, and condensation energy.

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III-B. Quantum Geometry & Flat‑Band Superconductivity

How quantum geometry — the quantum metric of Bloch wavefunctions — sets the Cooper pair size in flat bands where \( v_F \to 0 \).

📊 Beamer – The Size of a Cooper Pair in a Flat Band

Type: Presentation slides

Resolves the paradox of flat‑band superconductivity: introduces the quantum metric \( g_{\mu\nu}(\mathbf{k}) \), derives \( \xi_{\mathrm{pair}}^2 = 2\langle \operatorname{tr} g \rangle_{\mathrm{BZ}} \), and proves the topological lower bound \( \xi_{\mathrm{pair}}^2 \gtrsim |C| a^2/\pi \) for Chern bands.

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📘 Lecture Note – The Size of a Cooper Pair in a Flat Band

Type: Comprehensive lecture notes

Self‑contained pedagogical introduction: conventional BCS coherence length, flat‑band Cooper problem with band projection, binding energy \( E_b = -U/N_{\mathrm{orb}} \), quantum geometric tensor \( Q_{\mu\nu} = g_{\mu\nu} - \frac{i}{2}\Omega_{\mu\nu} \), pair size \( \xi_{\mathrm{pair}}^2 = 2\langle \operatorname{tr} g \rangle_{\mathrm{BZ}} \), topological lower bound, and equivalence to Wannier spread.

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III-C. Fermi‑Velocity‑Controlled Length Scales in Solids

The master formula \( L_E \sim \hbar v_F / E \) unifying thermal length, BCS coherence, Kondo cloud, mean free path, and localization.

📊 Beamer – Fermi-Velocity-Controlled Length Scales in Solids

Type: Presentation slides

Unified framework: \( L_T = \hbar v_F/2\pi k_B T \), \( \xi_0 = \hbar v_F/\pi\Delta \), \( \xi_K = \hbar v_F/k_B T_K \), \( \ell = v_F\tau \), diffusive generalization \( L_E \to \sqrt{\hbar D/E} \), and Thouless energy \( E_{\mathrm{Th}} = \hbar D/L^2 \).

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📘 Lecture Note – Fermi-Velocity-Controlled Length Scales in Solids

Type: Comprehensive lecture notes

Full derivations: linearization at Fermi surface, three readings of \( L_E = \hbar v_F/E \), thermal length via Matsubara poles, SNS Josephson decay, BCS coherence from pair wavefunction, Kondo cloud from Yosida variational state, mean free path and 1D localization, diffusive generalization, and Thouless energy.

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III-D. Friedel Oscillations in One Dimension

Green's function / \( T \)-matrix derivation of the \( 2k_F \) density oscillation and its thermal cutoff.

📊 Beamer – Friedel Oscillations in One Dimension

Type: Presentation slides

Green's function derivation: Lehmann representation, free Green's function \( G_0^R(x,x';E) = -\dfrac{i}{\hbar v_E} e^{ik_E|x-x'|} \), Dyson equation, separable \( T \)-matrix \( t(E) = u/(1 + iu/\hbar v_E) \), zero‑temperature result \( \delta n(x) \sim -\dfrac{u\nu_F}{2}\dfrac{\cos(2k_F x)}{|x|} \), and finite‑temperature thermal length \( \xi_T = \hbar v_F/2\pi k_B T \).

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📘 Lecture Note – Friedel Oscillations in One Dimension

Type: Detailed lecture notes

Six‑section written note: physical setup, Lehmann representation and spectral function, free Green's function, Dyson equation and separable \( T \)-matrix, charge density from Green's function, zero‑temperature result, and finite‑temperature thermal envelope \( (x/\xi_T)/\sinh(x/\xi_T) \).

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III-E. Anderson Localization in One Dimension

Transfer‑matrix derivation of exponential localization, Lyapunov exponent, and the Thouless formula.

📊 Beamer – Anderson Localization in One Dimension

Type: Presentation slides

1D Anderson model: tight‑binding Hamiltonian, three‑term recurrence, transfer matrix \( T_n \in \mathrm{SL}(2,\mathbb{R}) \), Lyapunov exponent \( \gamma(E) = \lim_{N\to\infty} \frac{1}{N}\ln\|\mathcal{M}_N\| \), localization length \( \xi(E) = 1/\gamma(E) \), clean‑chain limit, weak‑disorder Thouless formula \( \xi(E) = 2(4t^2 - E^2)/\sigma^2 \), Prüfer variables, and numerical QR re‑orthogonalization.

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📘 Lecture Note – Anderson Localization in One Dimension

Type: Detailed lecture notes

Complete written derivation: tight‑binding Hamiltonian, transfer matrix, Furstenberg and Oseledec theorems, clean‑chain limit, weak‑disorder expansion in Prüfer variables, Thouless formula, numerical implementation, and connection to scaling theory of localization.

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III-F. Solid‑State Length Scale Overview

A master overview of the hierarchy of length scales in solids, unifying the entire course.

📊 Beamer – Solid-State Length Scale Overview

Type: Presentation slides

High‑level summary: hierarchy of length scales from \( \lambda_F \) to \( \xi_K \), diffusive generalization, Thouless energy as the inverse dictionary, and limits of the framework (flat bands, non‑Fermi liquids, Dirac materials).

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