HomeQuantum PhysicsMajorana Zero Modes in a Topological Nanowire

Majorana Zero Modes in a Topological Nanowire (2D)

Interactive Kitaev-chain simulator: tune chemical potential, pairing and hopping on a 1D topological superconducting wire, diagonalize its real Bogoliubov-de-Gennes Hamiltonian live, and watch the computed near-zero-energy mode localize at the wire's ends.

Quantum Physics2DAdvanced60 FPS📱 Mobile-adapted⇄ 3D version
2d-majorana-fermion-topological-qubit ↗ Open standalone

This 2D companion to the 3D Kitaev-chain simulator drops the lattice-graphics view in favor of showing the physics engine's raw output: the real 2N×2N Bogoliubov-de-Gennes Hamiltonian for the chain is assembled from the μ, Δ, t and N sliders and diagonalized in-browser with the classical Jacobi eigenvalue algorithm on every change — no analytic shortcut. The top strip plots all 2N computed eigenvalues (always exact ±E pairs, a live check of particle-hole symmetry); the bar chart below plots the real site-resolved probability density of the eigenvector nearest zero energy, so end-localization of the Majorana zero mode is something the diagonalization actually produces, not an animation cue. Live readouts track the numerically diagonalized near-zero energy, the analytic bulk gap, the end-mode localization length, and the topological winding invariant, and a parity-measurement button demonstrates how the two end modes encode one non-local, noise-resistant topological qubit.

⚙ Under the hood

Tune chemical potential, pairing and hopping on an interactive Kitaev chain and watch unpaired Majorana zero modes localize at the wire's ends, then measure the non-local fermion parity they encode as a topological qubit.

Majorana fermiontopological qubitKitaev chainquantum computingsuperconductivitycondensed matter

2D · HTML5 Canvas 2D · 60 FPS target · runs fully client-side, no install

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