neuralqx.operators.computational.Euclidean3d.jax.vertex_TRC module¶
- class Euclidean3dVertexTRCOperatorJax(lqx, vertex, *, apply_lapse=False)¶
Bases:
ComputationalJaxOperatorSingle-vertex Thiemann-regularised Euclidean Hamiltonian constraint H_v for the 2+1 U(1)^3 WCL model as a JAX-compatible ComputationalOperator.
For each term t (constructed from LqxWCL3D._sum_terms and _epsilon) and each U(1) copy c=0,1,2, this emits one connection:
σ’_{t,c} = h_{α_t}^{(c)} σ
- with matrix element:
<σ’_{t,c}|H_v|σ> = N(v) w_t Δ_k^{(c)}(σ) Δ_l^{(c)}(σ)
- where:
Δ_s^{(c)}(σ) = sqrt(V_v(σ)) - sqrt(V_v(h_{s}^{(c)-1} σ)).
No Taylor expansions are used. sqrt(V_v) is evaluated directly from the 2+1 vertex volume kernel.
- property dtype¶
The dtype of the operator’s matrix elements ⟨σ|Ô|σ’⟩.
- tree_flatten()¶
- classmethod tree_unflatten(aux, leaves)¶
- class Euclidean3dVertexTRCAdjointOperatorJax(lqx, vertex, *, apply_lapse=False)¶
Bases:
Euclidean3dVertexTRCOperatorJaxAdjoint of Euclidean3dVertexTRCOperatorJax.
- Differences vs the ket-ordered operator:
segment differences use forward shifts (h_s) instead of inverse shifts (h_s^{-1}) i.e. we flip seg shifts: seg_shift -> -seg_shift
loop holonomy is daggered, i.e. loop shifts negated.
- ThiemannRegularisedVertexConstraint3dJax(lqx, vertex, *, apply_lapse=False, adjoint=False)¶