Harper equation
The Peierls phase converts the two-dimensional magnetic problem into a one-dimensional difference equation with a quasiperiodic potential.
Topological Matter 04 · magnetic Bloch bands
Diagonalize the Harper tight-binding Hamiltonian to build the fractal energy spectrum versus dimensionless flux. Park the probe near any rational flux, watch the magnetic unit cell expand into subbands, and label a selected gap with its Hall Chern number from the Diophantine equation.
Physics tutorial
BackgroundA two-dimensional lattice electron in perpendicular field feels both Bloch periodicity and cyclotron phase. At rational flux the periods combine into a magnetic unit cell.
Why it mattersThe Hofstadter spectrum unifies band theory, quantum Hall topology, and fractal self-similarity in one minimal model.
Start with the essentials
The Peierls phase converts the two-dimensional magnetic problem into a one-dimensional difference equation with a quasiperiodic potential.
is the single-electron flux quantum; the denominator sets magnetic-cell size.
For gap , the integer solution is the Hall Chern number of all occupied bands below it.
Typical misconceptionThe wings show the shape of electron motion in real space.
Better mental modelThe horizontal axis is flux and the vertical axis is allowed energy; every point is an eigenvalue of a different Hamiltonian.
Typical misconceptionA sufficiently large finite matrix displays every scale exactly.
Better mental modelEvery numerical plot has size and sampling cutoffs and can only approach the self-similar infinite-lattice spectrum layer by layer.
Select , , and in sequence.
What to observe: The right-hand flux slice gains structure as the magnetic-cell denominator grows.Hold and move the energy probe vertically.
What to observe: The nearest gap count changes and the Diophantine Chern label jumps.Choose the golden-ratio approximation and increase the Harper matrix size.
What to observe: The spatial eigenstate and local spectrum become more intricate, while the finite system still resolves only finite hierarchy.