Diagonal #
Ported from scottnarmstrong/Superdiffusion at 7f20476385d4af418f110303085ad0740c9eba46. Module imports, support namespace and local option directives adapted for Lean Pool.
Block diagonality of the annealed cutoff block matrix #
ABK26, e.homs.defs.U.diag. Once the annealed coupling matrix vanishes
(e.annealed.khom.zero), the display records that bhom_m(U) = shom_m(U) and
that the annealed doubled matrix is block diagonal, bfAhom_m(U) = ((shom_m(U), 0), (0, shom_{m,*}^{-1}(U))).
In CoarseGraining's naming the finite-volume annealed blocks of bfAhom_m(U) = E[bfA_m(U)] are Ch04.annealedB (upper left bhom_m(U)),
Ch04.annealedSigmaStarInv (lower right shom_{m,*}^{-1}(U)) and
Ch04.annealedSigma (shom_m(U)), with the two mixed blocks -(khom_m^t shom_{m,*}^{-1})(U) and -(shom_{m,*}^{-1} khom_m)(U) sitting in upperRight
and lowerLeft.
Main results #
ABK26, bhom_m(U) = shom_m(U). The annealed conductivity of the
genuine cutoff equals its annealed upper-left block.
ABK26, e.homs.defs.U.diag. The annealed doubled block matrix of the
genuine coefficient cutoff is block diagonal on every triadic cube, with
diagonal blocks shom_m(U) and shom_{m,*}^{-1}(U).
Origin-cube form of
coefficientCutoffLaw_annealedBlockMatrix_eq_blockDiag.