Marked integration and coupling reset
What a marked integral records. Insertions must survive blocking as functions, including when a label occurs more than once. The marker algebra records occurrences separately; only the stated substitutions identify their final readings. This is why the numbered-tree estimates, repeated-occurrence factorials and distinct connected-set expansion all remain in the argument. The primitive integrand is the actual finite integrand with its chart Jacobian, Gaussian density, local interactions, insertion factors and masks. Its normalization is retained before any cluster regrouping.
The readout integrates this record and transports the prescribed insertion. Absolute weighted estimates justify the rearrangements and the passage from finite sums to a countable dictionary. Projection onto the coupling direction is followed by an exact reset identity; the unprojected part remains a residual activity, rather than disappearing. The loan cancellation restores the true kinetic base before the later bounds are used. At a group/logarithm interface, multiplication remains ordered: with exp, the neutral residual is exp
, not the reversed product. Its off-chart value stays in the record. This local correction preserves the supplied primitive integration and all subsequent paid restoration estimates.
13.1 Insertion algebra, restoration and local prices
Fix finite markers and their allowed-mode census. A mode is an allowed subset
. Multiplication joins disjoint subsets and discards products outside the census. Write [
and
for coefficient and monomial; the empty mode is scalar. For positive
Searchable transcription
tw(A) = Y v∈A wv, ∥P∥w = X A tw(A)|[P]A|.
Triangle inequality and) prove subadditivity and submultiplicativity by expanding disjoint coefficient pairs. On the zero-scalar nilpotent ideal, the finite exponential Exp
has norm at most
and obeys exponential addition for commuting arguments. An insertion representation consists of density exponent
, primary functions Φ
, forced profiles
) and corrections
), where
) is support plus flagged inventory. With scalar profile
and configuration flag set
), restoration is exactly
Searchable transcription
X
!
v
e{v}Φv(U) +
X
S
H(S, U)
X(U) = eE(U) Exp
!
×
X
Y
bq(U) +
X
v
e{v}ωv(q, U) + K(q, U)
.
P:Pattern(F(U),P)
q∈PPattern requires pairwise disjoint and inventory union
). All sums are finite at fixed torus and census. Corrections have only modes of size at least two, are measurable, gauge invariant, supported on their regions and scoped to markers pinned there. Exponential corrections vanish off the healthy region and have zero scalar part. Flagged corrections require
and
. Scalar multiplication preserves these permissions.
Correction prices use summable nonnegative envelopes with
and
Searchable transcription
X i:x∈Si aieecB(Si) ≤f, sup x
Searchable transcription
where cB is the minimizing cover number. For e ≥0, if each nonzero term has a marker pin in its sup- port, charge it to all such pins. At least one exists by scope and positive degree, and the exponential weight is at least one. Summing the sitewise bound over pins proves P i ∥Yi(U)∥w ≤|V |f. For the unmarked background profiles the same argument charges to all sites, giving P q ∥bq(U)∥w ≤|Λ|u, where u is their sitewise activity budget. If wv|Φv(U)| ≤x and P q wv|ωv(q, U)| ≤y, the exponen- tial argument costs at most |V |(x+f) and all field factors Tq together cost at most |Λ|u+|V |(y+f). Dropping pattern restrictions gives
Searchable transcription
Y q∈P ∥Tq∥w = Y q (1 + ∥Tq∥w) ≤e P X q ∥Tq∥w. P
Searchable transcription
Consequently
∥X(U)∥w ≤exp{E(U) + |V |(x + y + 2f) + |Λ|u}.The lawful-density estimate supplies the uniform majorant. For a normalized mode integral use , integrate against the probability prior and divide by the positive density integral. Its lower bound and the history treasury give the final bill
Λ
). This separates polynomial algebra from the vacuum density and denominator estimates. The lift retains the mode census, weights, pins, inventories and permission predicates. Coefficientwise readout is
an algebra map on that same census, commuting with finite exponential, pattern restoration and probability integration; the retained positive denominator then gives exactly the same normalized mode bill. Explicitly, for a mode-valued coefficient function define its lift by
Searchable transcription
L P = X A eA([P]A ◦π).
The allowed-mode census is fixed in this definition. Since the coefficient of a product is the same finite sum over disjoint allowed pairs before and after composition, one has
Searchable transcription
L (PQ) = (L P)(L Q), [L P]A = [P]A ◦π, (L P) ◦σ = P.
Searchable transcription
The same finite calculation gives L (Exp P) = Exp(L P) on the zero-scalar ideal and ∥L P(z)∥w = ∥P(π(z))∥w. Record the flag set and all support–inventory barcodes so that the pattern predicate is pulled back along with its coefficient. The restoration sum then is exactly L X, including zero terms excluded by the predicate. Finally, for the realized probability prior νZ with π∗νZ = ν, coefficientwise integration gives Z [L X]A dνZ = Z [X]A dν.
The displayed majorant ensures these integrals exist. Applying this also to the scalar density recovers the positive normalizing denominator, so the normalized mode integral and its stated bill are preserved.
13.2 Singleton restoration and response closure
Searchable transcription
For represented density R, primary function Φ and summable forced family gi, define the singleton density coinR(Φ, g)(U) = R(U)Φ(U) + eER(U) X i nickelR,i(U; g).
The second term is the first activity-gas variation in direction. Absolutely convergent grouping by support-and-inventory barcode preserves that variation. Finite polynomial expansion shows the restored scalar mode is
) and its
coefficient is this coin: only one factor can supply a singleton, all others supply scalars; the exponential has scalar one, and higher corrections supply neither scalar nor singleton. The correction representation must preserve the actual singleton insertions after every step. Conversely suppose the polynomial is
Exp(
) Field(
), with zero scalar part of
original background scalar profiles in and prescribed forced singleton profiles
. We show that if the singleton coefficients of the whole expression are coin
), then the singleton coefficients of
are precisely Φ
. If its singleton densities are coin
), subtraction cancels gas variations and gives
Φ
) = 0. Nonvanishing of
) permits cancellation. Projection onto modes of size at least two splits
into prescribed singleton plus higher exponential correction and each
into background, prescribed forced singleton and higher flagged correction. The original density is preserved pointwise.
Searchable transcription
For a misplaced forced singleton, take attached local responses ψv(S, U) supported on regions
containing pin ov and vanishing when that region is healthy. Put J = P
v,S e{v}ψv(S, U). Closure
joins overlapping background factors and responses into connected components, recording support
and flagged inventory. Component expansion proves exactlySearchable transcription
Field(Closure(K, ψ)) = Field(K) Exp J.
Replace by its closure and
by
to preserve the full polynomial. No-response terms reproduce
; terms with a response have zero scalar part; terms with at least two responses have zero singleton part. A sole response is multiplied by the background attached to its support, giving exactly its hook in the singleton profile. Thus no unspecified singleton change is introduced. The converse then identifies primary functions from known singleton densities. Higher-mode projection yields the two higher correction families, preserves locality and permissions, and decreases weighted prices. For field budget
, response budget
and pin occupancy
, the connected-component estimate bounds the higher closure budget by
Searchable transcription
exp{W + M siteFactor(B)c} −1,provided the support-exponent loss pays (2 siteFactor(
. The forest-price argument below supplies this bound; marker-monomial reweighting transfers both higher families to the requested weights. These are the algebraic and numerical operations used in the one-step retained-insertion estimate. The source lift retains response attachments, barcode grouping and component partitions. Coefficientwise recovery commutes with finite projection and nilpotent exponential; absolute summability permits the same grouping. It therefore recovers both the exact closure identity and the nonvanishing cancellation establishing the prescribed singleton fields.
In the notation of the coefficientwise lift, let discard scalar and singleton modes. Its definition gives
L = L
Preserve each response label and its attachment, even when coefficients coincide. The overlap graph is determined by the recorded supports, so readout and the section recover its vertices, edges, connected partitions and inventory unions. Each component coefficient is a sum of products of these same labelled factors. The algebra-map identity therefore gives