|
gptkb:Edwards-Anderson_model
|
H = -∑_{⟨i,j⟩} J_{ij} S_i S_j
|
|
gptkb:complete_graph_K_{n+1}
|
yes
|
|
gptkb:(n+1)-cube_graph
|
true
|
|
gptkb:icosahedron_graph
|
true
|
|
gptkb:K_3
|
true
|
|
gptkb:hypercube_graph
|
true
|
|
gptkb:Potts_model
|
H = -J Σ δ(s_i, s_j)
|
|
gptkb:Ising_chain
|
H = -J Σ s_i s_{i+1} - h Σ s_i
|
|
gptkb:Hénon–Heiles_system
|
H = 1/2 (p_x^2 + p_y^2 + x^2 + y^2) + x^2 y - (1/3) y^3
|
|
gptkb:Franklin_graph
|
true
|
|
gptkb:Edwards–Anderson_model
|
sum over random couplings between spins
|
|
gptkb:XY_model
|
H = -J Σ cos(θ_i - θ_j)
|
|
gptkb:n-cube_graph
|
true
|
|
gptkb:Toda_lattice
|
sum of kinetic and exponential potential energies
|
|
gptkb:complete_graph_K_{2^n}
|
yes
|
|
gptkb:antiferromagnetic_Heisenberg_model
|
H = J Σ S_i · S_j, with J < 0
|
|
gptkb:XXZ_spin_chain
|
H = J ∑ (S_i^x S_{i+1}^x + S_i^y S_{i+1}^y + Δ S_i^z S_{i+1}^z)
|
|
gptkb:Ising_model
|
sum over spin interactions
|
|
gptkb:Heawood_graph
|
true
|
|
gptkb:2D_Ising_model
|
H = -J Σ⟨i,j⟩ s_i s_j - h Σ_i s_i
|