The Kitaev chain is the minimal model of a 1D topological p-wave superconductor / spinless nanowire with proximity-induced pairing:
H = -μΣc_j†c_j - Σ[t(c_j†c_j+1+h.c.) + Δ(c_jc_j+1+h.c.)]
Writing each ordinary fermion as two Majorana operators, c_j = (γA,j+iγB,j)/2, the on-site term pairs γA,j with γB,j (strength ∝ μ) while hopping+pairing links γB,j to γA,j+1 of the next site (strength ∝ t+Δ). At the solvable point μ=0, Δ=t, every Majorana pairs with its neighbor across the site boundary, leaving γA,1 and γB,N completely unpaired — two spatially separated, exactly zero-energy Majorana modes.
More generally the chain is topological whenever |μ| < 2t (with Δ≠0). The end-mode decay is governed by the roots of
(t+Δ)λ² + μλ + (t-Δ) = 0
with localization length ξ = -1/ln|λdominant|; the bulk excitation gap is mink √[(2t cos k - μ)² + 4Δ²sin²k], plotted live above.
- μ, Δ, t sliders — tune the Hamiltonian; bond brightness in the 3D view directly shows the on-site (μ) vs inter-site (t+Δ) Majorana pairing strength computed from these values.
- N slider — chain length; a shorter wire lets the two end modes overlap and split away from exactly zero energy even in the topological phase.
- Measure fermion parity — the two far-separated end Majoranas combine into one non-local fermion d=(γL+iγR)/2. Its occupation number (0 or 1) is the topological qubit; measuring it collapses that single shared quantum number at both ends at once, illustrating why local noise can't dephase it.
This is the mechanism behind proposed topological qubits in InSb/InAs nanowires with induced superconductivity (Microsoft, Delft, and others) — information stored non-locally in Majorana zero modes is, in principle, protected from local perturbations.