Paper-facing permutation-sum statements #
This file freezes the statements of Propositions 5.7, 5.9, and 5.10 of Deng--Shen, The four-dimensional Anderson model: a case study for critical SPDEs (arXiv:2607.10105v1). It contains no proof of those estimates.
The left sides use the factorial-ledger normalization paperSum. Thus they
are sums over permutations of distinct copies, although their internal carrier
is the pure word model of PermSum.Words.
Totalization conventions #
- Adjacent positions are represented by
AdjacentIndex m; this type is empty whenm = 0, so no out-of-range successor is ever read. - The subtractions in
(n - |W|)!,(m - 2|W|)!, and(m - s)!are natural subtraction. In every estimate below the stated tree, multiplicity, and skipped-set hypotheses imply that no truncation occurs. Those inequalities are proof obligations, rather than extra assumptions weakening the paper's propositions. - Parent scales are read only on non-root branch nodes. Root scales are read
only under the explicit hypothesis that the root is a branch node. Hence
the junk values of
HeppMarking.Nexpaway fromBranchNodesare never used. - The compound-leaf set is required to be a subset of
Leaves; the junk values ofMultiplicities.maway fromLeavesare never used. - Real powers (
3/4andm/2) use mathlib's totalizedReal.rpow. Their bases are positive on the stated domains.
Common paper data and weights #
The leaf carrier of a Hepp tree.
Equations
- Anderson4D.HeppLeaf t = ↥t.Leaves
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The multiplicity function restricted to its meaningful leaf carrier.
Equations
- Anderson4D.leafMultiplicity mu l = mu.m ↑l
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Total word length m = ∑_l m_l from Definition 5.3.
Equations
- Anderson4D.totalMultiplicity mu = ∑ l : Anderson4D.HeppLeaf t, Anderson4D.leafMultiplicity mu l
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The non-root branch nodes. Every parent-scale ratio in (5.15), (5.33), and (5.39) is indexed by this set.
Equations
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Branch nodes in the subtree rooted at v; this is paper notation
B_v = {u ∈ B : u ≤ v} from Definition 5.3.
Equations
- Anderson4D.branchNodesUnder v = {u ∈ t.BranchNodes | ↑v <+: ↑u}
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The quantity N'_v = ∑_{u ≤ v} γ_u^∞ N_u used in (5.32) and (5.38).
Equations
- Anderson4D.accumulatedScale Nm mu v = ∑ u ∈ Anderson4D.branchNodesUnder v, Anderson4D.gammaInf mu u * Anderson4D.scaleN Nm u
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Definition 5.4(a), without the unrelated boundedness and linking clauses: the leaf embedding is injective and separated at the LCA scale.
Equations
- One or more equations did not get rendered due to their size.
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Condition (5.32): every pair of leaves below a branch node is at distance
at most N'_v.
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- One or more equations did not get rendered due to their size.
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Condition (5.38)(a): N_{v⁺} ≤ 8 N'_v for every non-root branch node.
Equations
- Anderson4D.SatisfiesSingleScaleCondition Nm mu = ∀ v ∈ Anderson4D.nonrootBranches t, Anderson4D.scaleN Nm (Anderson4D.PlaneTree.parentV v) ≤ 8 * Anderson4D.accumulatedScale Nm mu v
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Natural dyadic numbers, used for the scale R in Proposition 5.10.
Equations
- Anderson4D.IsDyadicNat R = ∃ (k : ℕ), R = 2 ^ k
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The position immediately to the right of an adjacency index.
Equations
- Anderson4D.adjacentSucc j = ⟨↑↑j + 1, ⋯⟩
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The exact factor ⟨x-y⟩⁻² = (1 + |x-y|²)⁻¹ in (5.15), (5.33), and
(5.39), using the project's fixed lattice sup norm.
Equations
- Anderson4D.latticeEdgeWeight x y = (1 + Anderson4D.znorm (x - y) ^ 2)⁻¹
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Product of all adjacent edge weights in a word.
Equations
- Anderson4D.heppChainWeight z w = ∏ j : Anderson4D.AdjacentIndex m, Anderson4D.latticeEdgeWeight (z (w ↑j)) (z (w (Anderson4D.adjacentSucc j)))
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Product in (5.39), omitting exactly the adjacency indices in O.
Equations
- Anderson4D.heppChainWeightExcept z O w = ∏ j : Anderson4D.AdjacentIndex m, if j ∈ O then 1 else Anderson4D.latticeEdgeWeight (z (w ↑j)) (z (w (Anderson4D.adjacentSucc j)))
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Proposition 5.10's adjacency condition: equal consecutive leaves are
forbidden outside the skipped set O; no primitivity is imposed.
Equations
- Anderson4D.NoAdjacentOutside O w = ∀ j ∉ O, w ↑j ≠ w (Anderson4D.adjacentSucc j)
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The (5.39) summand: omitted factors at O, the adjacency restriction
outside O, and deliberately no primitivity condition.
Equations
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(k!)^{1/2} in the paper.
Equations
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(k!)^{3/4} in the paper, represented by Real.rpow.
Equations
- Anderson4D.factorialThreeQuarters k = ↑k.factorial ^ (3 / 4)
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The scale ratio N_v / N_{v⁺}, used only for non-root branch nodes.
Equations
- Anderson4D.parentScaleRatio Nm v = ↑(Anderson4D.scaleN Nm v) / ↑(Anderson4D.scaleN Nm (Anderson4D.PlaneTree.parentV v))
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Proposition 5.7, equation (5.15) #
The right-hand side of (5.15), with W ranging over subsets of the
non-root branch nodes.
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- One or more equations did not get rendered due to their size.
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Proposition 5.7 / (5.15), frozen statement.
C is the single absolute constant. The hypotheses spell out the ambient
n ≥ 2 context, a valid nontrivial Hepp tree, even leaf multiplicities of
total 2n, and realization by a fully admissible embedding.
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- One or more equations did not get rendered due to their size.
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Proposition 5.9, equations (5.32)--(5.33) #
The right-hand side of (5.33). compound is exactly the set
L_C; simpleLeaves t compound is L_S.
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- One or more equations did not get rendered due to their size.
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Proposition 5.9 / (5.32)--(5.33), frozen statement.
The named constants remain parameters with the literal hypotheses
C0 > 1000 and D = exp(C0^10). Compound multiplicities need not be even.
The left side retains both primitivity and the no-adjacent-equal restriction.
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- One or more equations did not get rendered due to their size.
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Proposition 5.10, equations (5.38)--(5.39) #
The right-hand side of (5.39). The exponent m/2 on C0 is a real
half-power, not natural-number division.
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- One or more equations did not get rendered due to their size.
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Proposition 5.10 / (5.38)--(5.39), frozen statement.
R is explicitly dyadic and dominates N'_r; O is a set of adjacency
indices with |O| = s. The left side has no primitivity restriction.
Equations
- One or more equations did not get rendered due to their size.