KitaevHoneycomb — Honeycomb Lattice Kitaev Model
Matter-Majorana finite-T サーフェスは v0.17 で導入。flux-free 近似であり flux gap T ≪ Δ_v でのみ valid。SusceptibilityXX/YY/ZZ および Magnetization{X,Y,Z} は 未実装 — σᵅ matrix elements が flux pair を励起するため flux-free sector で恒等的に消える。完全な finite-T は flux-sector Monte Carlo (Nasu et al. 2014) が必要、今回の射程外。
Hamiltonian
H = − Σ{⟨ij⟩ ∈ x-bonds} Kx σˣᵢ σˣⱼ − Σ{⟨ij⟩ ∈ y-bonds} Ky σʸᵢ σʸⱼ − Σ{⟨ij⟩ ∈ z-bonds} Kz σᶻᵢ σᶻⱼ
(σ-convention; eigenvalues ±1)
Phases (Kitaev 2006)
- isotropic gapless (B-phase): each |K_α| ≤ sum of others
- anisotropic gapped (Ax, Ay, A_z phases): one K dominates
- gap: Δ = 2·max(0, |Kmax| − |Kother₁| − |K_other₂|)
Coverage Matrix
| Quantity | OBC | PBC | Infinite |
|---|---|---|---|
| Energy{:per_site} (T=0) | ✅ SVD on hopping matrix | ✅ 4-flux-sector min | ✅ BZ integral |
| Energy{:per_site} (T>0) | ✅ matter sum | (deferred) | ✅ BZ integral |
| FreeEnergy / Entropy / SpecificHeat | ✅ matter sum | — | ✅ BZ integral |
| MassGap | — | — | ✅ analytic |
| Mag{X,Y,Z} / Susc{XX,YY,ZZ} | not implemented (deferred) | — | not implemented |
| ZZStructureFactor | — | — | static + dynamic via TFIM-style proxy* |
*ZZStructureFactor router を参照 (TFIMinfinitedynamics.jl に同様の実装あり; Kitaev 自身の動的 SF は別 issue)。
v0.17 Highlights — Matter-Majorana Free-Fermion Finite-T
Lieb 1994: GS は flux-free sector に固定。flux-free セクター内では matter Majorana が自由フェルミオン hopping を成し、
Z_matter(β) = ∏_k 2 cosh(β λ_k)(λk は bipartite hopping matrix M の正の SVD 値; λk は full Majorana eigenvalue 規約 — 半固有値ではなく)。
per-site (= per Majorana site, 2 atoms per unit cell) 物理量:
ε(β) = -(1/N_sites) Σ_k λ_k tanh(β λ_k)
f(β) = -(1/(N_sites β)) Σ_k log(2 cosh(β λ_k))
s(β) = (1/N_sites) Σ_k [log(2 cosh(βλ)) − βλ tanh(βλ)]
c_v(β) = (1/N_sites) Σ_k (βλ)² sech²(βλ)Infinite では Σ_k → ∫_BZ d²θ / (2π)² (factor 2 で 2 atoms/cell)。
Code Examples
m = KitaevHoneycomb(Kx=1.0, Ky=1.0, Kz=1.0) # isotropic gapless
# T = 0 GS
QAtlas.fetch(m, Energy(:per_site), Infinite()) # Baskaran-Mandal-Shankar 2007 ≈ -0.787
QAtlas.fetch(m, Energy(:per_site), OBC(0); Lx=4, Ly=4)
QAtlas.fetch(m, Energy(:per_site), PBC(0); Lx=4, Ly=4)
QAtlas.fetch(m, MassGap(), Infinite()) # = 0 (gapless)
# T > 0 matter sector
β = 5.0
QAtlas.fetch(m, FreeEnergy(), Infinite(); beta=β)
QAtlas.fetch(m, SpecificHeat(), Infinite(); beta=β)
# Anisotropic gapped phase
m_az = KitaevHoneycomb(Kx=0.5, Ky=0.5, Kz=2.0)
QAtlas.fetch(m_az, MassGap(), Infinite()) # = 2(2 − 1) = 2Validity Boundary of Matter-Sector Finite-T
flux gap Δ_v ≈ 0.07 |K| (isotropic) — 凍結する温度スケール。
| Regime | matter-only valid? |
|---|---|
| T ≪ Δ_v | ✅ |
| T ~ Δ_v | × (flux fluctuations dominate, Nasu-Udagawa-Motome 2014) |
| T ≫ Δ_v ≪ K | × |
References
- Kitaev 2006 — exactly solved model and beyond
- Lieb 1994 — flux-free ground state theorem
- Baskaran-Mandal-Shankar 2007 — TL ε_gs ≈ −0.787 |K|
- Nasu-Udagawa-Motome 2014 — full flux-sector finite-T (sign-free QMC)
- Loss-Pu 2008 — spin correlators (z-bond local, off-diagonal)
Related
TFIM— 1D version of "single Majorana species" (BdG hopping); Kitaev's matter sector is the 2D analogue
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Verified hubs
In the Verified Atlas, these 2 models register 11 hubs (quantity / BC pair). The badge column shows the R1 assurance level; click a hub link to see the exact verify(...) calls, references, and corroboration mechanism.
| Model | Quantity | BC | Assurance | Cards |
|---|---|---|---|---|
KitaevHeisenberg | MassGap | Infinite | 🟢 corroborated-at-p | 1 |
KitaevHoneycomb | Energy | Infinite | ⚪ cited-only | 1 |
KitaevHoneycomb | Energy | OBC | ⚪ cited-only | 0 |
KitaevHoneycomb | Energy | PBC | ⚪ cited-only | 0 |
KitaevHoneycomb | FreeEnergy | Infinite | ⚪ cited-only | 0 |
KitaevHoneycomb | FreeEnergy | OBC | ⚪ cited-only | 0 |
KitaevHoneycomb | MassGap | Infinite | 🟢 corroborated-at-p | 1 |
KitaevHoneycomb | SpecificHeat | Infinite | 🔵 coherent | 2 |
KitaevHoneycomb | SpecificHeat | OBC | 🔵 coherent | 2 |
KitaevHoneycomb | ThermalEntropy | Infinite | 🔵 coherent | 1 |
KitaevHoneycomb | ThermalEntropy | OBC | 🔵 coherent | 1 |
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