Finite #
Ported from scottnarmstrong/Superdiffusion at 7f20476385d4af418f110303085ad0740c9eba46. Module imports, support namespace and local option directives adapted for Lean Pool.
Finite infrared cutoff increments #
This module contains only the finite part of the infrared construction. The
lower-infinite cutoff is not defined here: finiteLowerCutoff m q is the
honest truncation over (m - q, m] and will later be sent to the lower
infinite limit on the full-measure carrier.
The canonical sample carrier for the integer-indexed shell sequence.
Equations
Instances For
The regular coefficient-field realization of one shell coordinate.
Equations
- Algsuperdiff.Section3.Cutoff.shellReg omega n = (omega n).forgetShell
Instances For
One shell coordinate, realized as a regular coefficient field, is measurable on the canonical sequence carrier.
The finite stream increment \mathbf{k}_m-\mathbf{k}_n, namely the
literal sum of shells with indices in (n,m].
Equations
- Algsuperdiff.Section3.Cutoff.finiteShellIncrement omega n m = ∑ k ∈ Finset.Ioc n m, Algsuperdiff.Section3.Cutoff.shellReg omega k
Instances For
Matrix-valued evaluation formula for a finite stream increment.
Entrywise evaluation formula for a finite stream increment.
Finite stream increments are measurable as regular coefficient fields.
Every finite stream increment is antisymmetric.
The finite lower truncation of the manuscript cutoff at scale m: the
sum over (m-q,m]. It is finite data, not a lower-infinite replacement.
Equations
- Algsuperdiff.Section3.Cutoff.finiteLowerCutoff m q omega = Algsuperdiff.Section3.Cutoff.finiteShellIncrement omega (m - ↑q) m
Instances For
Matrix-valued evaluation formula for the finite lower truncation.
Entrywise evaluation formula for the finite lower truncation.
Finite lower truncations are measurable as regular coefficient fields.
The finite lower cutoff is the descending partial sum
\sum_{r < q} \mathbf j_{m-r}.
Entrywise descending-partial-sum formula for the finite lower cutoff.