Manuscript IX-E@1 · IX-E.tex · 8f8d5e7f
Landmark IX-E Binary time ordering and causal subtraction on the declared sharp comparison sector
Proves the first-stage commutator identity, corrects double ordering to causal disjointness, and gives an algebraic extension criterion plus a conditional unnormalized subtraction theorem. The release is Unresolved: the restriction of K minus its conjugate needed for the decisive causal test is not supplied, and no sharp time-ordered map is constructed. Not a universal obstruction. No compilation is asserted.
Front matter
abstractAbstractFront matter · lines 81–100
Open as its own pageWe formulate the binary causal-extension problem on a fixed actual tensor domain inherited from IX-Free-2 and prove its algebraic consistency tests, its first-stage commutator identity, its double-ordering obstruction, an algebraic extension criterion, and the conditional unnormalized subtraction theorem. We correct the double-ordering geometry: two support orderings require causal disjointness, not overlapping functional supports. Neither full support of the locked contraction kernel nor injectivity of the first-stage maps determines the commutator.
The release outcome is Unresolved. The supplied information does not specify the restriction of needed to evaluate the decisive causal test, an old time-ordered map on a nonzero comparison subspace, or the sharp distributional extension and continuity data. Consequently this manuscript does not claim a constructed causal product or a universal obstruction. Its proved results identify exactly what a subsequent construction or no-go proof must discharge. Degree-four free descent is not reopened.
- figureThe tensor map is not the whole bridgeFront matter · IX-E@1#fig:scope-IX-E · lines 102–115Declared two-point domain→Actual tensor map→Full support bridgeDefining the map does not finish the bridge.
The tensor map is not the whole bridge. The three boxes name objects this manuscript keeps separate. The dashed box is the stated stop. Not a proof, and not an admission of a quantum coefficient.
- figureThe tensor map is not the whole bridgeFront matter · IX-E@1#fig:split-IX-E · lines 117–128Declared two-point domainFull support bridgeDefining the map does not finish the bridge.
The tensor map is not the whole bridge. The boxes name objects this manuscript keeps separate. The dashed box is the stated stop. Not a proof, and not an admission of a quantum coefficient.
- figureReading downward is not a transferFront matter · IX-E@1#fig:chain-IX-E · lines 130–143Declared two-point domain↓Actual tensor map↓Full support bridgeDefining the map does not finish the bridge.
Reading downward is not a transfer. The boxes name objects this manuscript keeps separate. The dashed box is the stated stop. Not a proof, and not an admission of a quantum coefficient.
- figureDeclared two-point domain is not Full support bridgeFront matter · IX-E@1#fig:pair-IX-E · lines 145–158Declared two-point domainnot the same objectFull support bridgeActual tensor map. Defining the map does not finish the bridge.
Declared two-point domain is not Full support bridge. The boxes name objects this manuscript keeps separate. The dashed box is the stated stop. Not a proof, and not an admission of a quantum coefficient.
- figureThree statuses stay separateFront matter · IX-E@1#fig:gate-IX-E · lines 160–173Named: Declared two-point domain→Used here: Actual tensor map→Not claimed: Full support bridgeDefining the map does not finish the bridge.
Three statuses stay separate. The boxes name objects this manuscript keeps separate. The dashed box is the stated stop. Not a proof, and not an admission of a quantum coefficient.
sectionFront matterFront matter · lines 173–182
Open as its own pageFigure fig:split-IX-E records one view of the same separation. Figure fig:chain-IX-E records one view of the same separation. Figure fig:pair-IX-E records one view of the same separation. Figure fig:gate-IX-E records one view of the same separation. The drawings add no hypothesis.
Figure fig:scope-IX-E records that separation. The drawing adds no hypothesis.
Release contract and corrections
sectionScope and legal outcomesRelease contract and corrections › Scope and legal outcomes · lines 185–229
Open as its own pageThe target is a complex-linear actual tensor map
on one fixed flip-stable comparison domain. An “actual” tensor means an element of the algebraic tensor product of actual functionals, rather than an unquotiented presentation by test functions.
There are three legal outcomes:
Constructed: all coefficients exist and every declared interface clause holds on the fixed domain.
Proved obstructed: a contradiction excludes every map satisfying that interface on the fixed domain.
Unresolved: at least one required consistency, extension, admission, contact, continuity, or overlap obligation remains undischarged.
Failure of one proposed replacement kernel excludes that candidate only. Removing an offending tensor changes the target and does not discharge a claim covering that tensor.
{{0.92} Release box. The domain chosen below contains all of and its conjugates. No offending first-stage pair may subsequently be deleted. The outcome of the supplied-data audit is Unresolved. Free-word coherence does not imply causal factorization. No , , general free-domain enlargement, G2 release, or repair of VII-C is asserted. }
The inherited hard stop is retained: the causal-product release is Unresolved because the time-ordered extension and its remaining causal, admission, and overlap obligations are unfinished, not because the degree-four free word has failed to descend.
sectionCorrections required before the gatesRelease contract and corrections › Corrections required before the gates · lines 230–271
Open as its own page. Injectivity is not an ordering comparison. The inherited equations
and the slab witness imply
They do not imply . For example, two injective linear maps can be the same map. The difference of the two contractions must be computed independently.
. Contacts cannot repair inconsistent prescribed values. If both support orderings hold, symmetry and factorization require the new value to equal both fixed free values. If those values are unequal, no alteration of the new value can satisfy both equations. This argument applies even on the permitted contact set.
. Fixed old coefficients must agree exactly. A contact is normalization freedom only where normalization is unfixed. A contact discrepancy from a supplied, fixed old coefficient remains a failed overlap until it is removed by a permitted normalization preserving all other conditions.
. Double ordering means causal disjointness. The sentence that a two-way pair requires overlapping functional supports is incorrect. With the ordering used here, both orderings exclude every causal relation between the two supports, including coincidence and null relation. Proposition prop:geometry proves the precise statement.
. A time slab proves an ordering, not necessarily its uniqueness. A later slab proves . It does not, by itself, rule out : supports in different time slabs can still be spacelike separated. Uniqueness of the ordering needs an actual causal relation between actual functional supports.
Prerequisites and entering state
sectionInherited objects, rather than reconstructed sourcesPrerequisites and entering state › Inherited objects, rather than reconstructed sources · lines 274–325
Open as its own pageThe following are imported premises. They are not proved anew in IX-E. The actual definitions of the sharp functional carrier, , , the locked kernel , and the old products belong to the prerequisite sources.
The labels C-I1–C-I9 are retained as inherited free-sector hypotheses. Their individual wording was not included in the supplied text; no purported verbatim reconstruction of those clauses is made here. The proofs below state the particular inherited properties they use explicitly.
Object Entering status IX-E use on Constructed in IX-Free-2, relative to its premises Named free product, not time ordering Both associations of Constructed through Free data only Evaluated Degree-four descent remains closed Evaluated Not a causal normalization F9a Fixed-support families only Not F9b or hypocontinuity New Absent Binary construction obligation VII-C under its hypotheses (E1)–(E4) Retained Not repaired by G2 Untouched Not opened by binary time ordering The word “new” distinguishes the absent sharp extension from any old time-ordered product that may separately be supplied.
sectionFree domain and wordPrerequisites and entering state › Free domain and word · IX-E@1#eq:word · lines 326–361
Open as its own pageThe inherited algebraic tensor domains are
The two associations of the inherited word agree with
Equation (eq:word) is free-word coherence. It supplies neither a binary time-ordered extension nor causal factorization.
No closure under intermediate multiplication is imported. In particular, an arbitrary expression
need not belong coefficientwise to the declared free domain.
sectionConjugation conventionsPrerequisites and entering state › Conjugation conventions · IX-E@1#eq:free-star · lines 362–387
Open as its own pageLet be complex-linear flip. Let
be componentwise antilinear conjugation. Then
Conjugation fixes the formal parameter . The inherited reversal property is
The comparison domain is
Thus both free orderings exist on . Flip stability of all of is not assumed.
sectionAdmission and supportPrerequisites and entering state › Admission and support · IX-E@1#eq:admission, IX-E@1#eq:sharp, IX-E@1#eq:support-bounds · lines 388–428
Open as its own pageAdmission includes the IX-A requirement
at every smooth configuration and for every finite list of required directions. The admitted coefficient space is treated as a complex vector space stable under conjugation. Admission of required descendants is part of the coefficient requirement, not an automatic consequence of a pairing existing.
The sharp adjoint identity is
Dropping its second term changes the functional; it is not a presentation rewrite.
Functional support is the closed support of configuration dependence. The imported bounds are
These are upper bounds. Their nonempty intersections do not prove nonempty intersections of the actual functional supports.
E0: a fixed comparison domain
sectionE0: a fixed comparison domainE0: a fixed comparison domain · IX-E@1#eq:fixed-domain, IX-E@1#eq:actual-old · lines 429–455
Open as its own pageNo nonzero old comparison subspace carrying an explicitly supplied old time-ordered map is present in the supplied data. The only old seed space on which a map is determined without additional information is
with its unique zero map. We therefore freeze the minimal full first-stage target
This choice does not claim a nonzero old time-ordered overlap. Any actual old intersection must still be audited:
One must not infer merely from : conjugation saturation needs its own subspace information.
propositionProposition: Domain stabilityE0: a fixed comparison domain · IX-E@1#prop:domain · proof attached · lines 456–485
Open as its own pageUnder (eq:free-star), the domain (eq:fixed-domain) satisfies
It contains every tensor in .
Proof. By definition, . Since , this implies . Also
Because dagger commutes with flip and preserves ,
Consequently preserves . Every generator in (eq:fixed-domain) therefore belongs to . Applying either involution permutes these generators; antilinearity of preserves their complex span.
sectionE0: a fixed comparison domainE0: a fixed comparison domain · lines 485–508
Open as its own pageDomain item Decision First-stage pairs All retained Flips and conjugates All retained Old seed Zero; no nonzero supplied old map Actual old intersection ; not evaluated by the excerpt Intermediate products No closure asserted Second-stage binary pairs Not added unless already in the span The interface is classical multiplication, symmetry, coefficient and descendant admission, actual-presentation independence, exact specified old overlaps, causal factorization, anti-time-ordering involution, and one named fixed-support continuity statement. A nonzero old seed may be added only by a separately declared change of target, accompanied by its actual old map.
E1: ordered-data consistency
definitionDefinitionE1: ordered-data consistency › Correct support geometry · lines 513–521
Open as its own pageFor actual functionals , set
The causal relations include their null boundaries and coincidence.
propositionProposition: Double-ordering geometryE1: ordered-data consistency › Correct support geometry · IX-E@1#prop:geometry · proof attached · lines 523–536
Open as its own pageLet and . Both and hold exactly when no point of is causally related in either direction to a point of . In particular, .
Proof. The first condition excludes pairs with . The second excludes pairs with . These are precisely the two directions of causal relation. If , reflexivity gives both relations, so coincidence is excluded as well.
sectionCorrect support geometryE1: ordered-data consistency › Correct support geometry · lines 536–543
Open as its own pageA null-related pair in the actual supports violates at least one ordering condition. An ordered prescription cannot be extended to such a pair merely by taking a limit. Conversely, sufficiently separated spacelike supports satisfy both orderings and are part of the consistency test, not an unordered exceptional region.
lemmaLemma: A spacelike sharp comparison regionE1: ordered-data consistency › Correct support geometry · IX-E@1#lem:spacelike · proof attached · lines 544–565
Open as its own pageIn the flat half-space , suppose are supported at times in , with spatial supports in balls , , respectively. If
then the upper support sets in (eq:support-bounds) are causally disjoint. Hence both and hold.
Proof. A point of has time in and spatial distance at most from . A point of has spatial distance at most from . Their spatial separation is therefore greater than , whereas their time separation is at most . They are strictly spacelike. The actual functional supports are subsets of these sets.
sectionCorrect support geometryE1: ordered-data consistency › Correct support geometry · lines 565–580
Open as its own pageThus two-way first-stage pairs can be specified without knowing exact functional supports. What remains unknown is the locked kernel difference on their observation supports.
For the inherited slab witness, the bounds
give : no later point can lie in the causal past of an earlier point. They do not alone decide the reverse ordering.
sectionThe complete first-stage commutator calculationE1: ordered-data consistency › The complete first-stage commutator calculation · IX-E@1#eq:locked-q · lines 581–600
Open as its own pageThe locked first-stage coefficients are
The brackets denote the supplied distributional pairing, including its configuration arguments. Classical configuration factors commute; no interchange of singular distributions is being made.
propositionProposition: First-stage commutatorE1: ordered-data consistency › The complete first-stage commutator calculation · IX-E@1#prop:commutator, IX-E@1#eq:commutator · proof attached · lines 601–627
Open as its own pageOn the declared first-stage sector,
Proof. Subtract the two inherited first-stage free products. Their classical terms agree. Reorder only the smooth configuration factors and the scalar test factors in the second expression of (eq:locked-q). Distributional linearity gives (eq:commutator). Finally, .
sectionThe complete first-stage commutator calculationE1: ordered-data consistency › The complete first-stage commutator calculation · lines 627–635
Open as its own pageEquation (eq:commutator) is the calculation determined by the supplied kernel data. A further evaluation requires a formula, conjugation identity, or support theorem for . Full support of says nothing of this kind: a real distribution can have full support while .
lemmaLemma: Compact detectionE1: ordered-data consistency › The complete first-stage commutator calculation · IX-E@1#lem:detection · proof attached · lines 636–670
Open as its own pageLet
be a nonzero compactly supported distribution whose support is contained in the interior of . Suppose the configuration space permits arbitrary smooth scalar and metric configurations. Then as an actual functional.
Proof. There are compactly supported smooth functions with
Indeed, finite sums of tensor-product test functions are dense in the test-function space on a product. This can be seen by a partition of unity into product charts followed by smooth Fourier approximation on compact rectangles. Continuity of a distribution would force it to vanish if it vanished on every such tensor.
Extend smoothly by zero where necessary and choose
Then . Choose the smooth metric configuration with and all other components zero. Equation (eq:commutator) gives a nonzero value. If only real configurations are used, decomposition into real and imaginary parts supplies real detecting the complex distribution.
sectionThe complete first-stage commutator calculationE1: ordered-data consistency › The complete first-stage commutator calculation · lines 670–676
Open as its own pageNo compactness of is required: compactness belongs to the functional kernel, while configurations are smooth. If the configuration space is constrained, the realization assumption in this lemma must instead be proved within that space.
theoremTheorem: Fixed-domain obstructionE1: ordered-data consistency › The complete first-stage commutator calculation · IX-E@1#thm:obstruction · proof attached · lines 677–695
Open as its own pageIf , both support orderings hold, and , no symmetric causally factorizing map exists on .
Proof. Factorization and symmetry would give
This contradicts Proposition prop:commutator. The nonzero coefficient at order remains nonzero in . The argument is independent of every contact choice and every higher coefficient.
sectionThe complete first-stage commutator calculationE1: ordered-data consistency › The complete first-stage commutator calculation · lines 695–701
Open as its own pageTheorem thm:obstruction is conditional, not an evaluated obstruction. Lemma lem:spacelike supplies geometric test regions; the supplied excerpt does not evaluate there.
propositionProposition: Classical multiplication is not a solutionE1: ordered-data consistency › The complete first-stage commutator calculation · proof attached · lines 702–714
Open as its own pageThe symmetric candidate fails factorization on the inherited ordered slab witness.
Proof. On that witness and
The candidate has no such coefficient.
sectionThe complete first-stage commutator calculationE1: ordered-data consistency › The complete first-stage commutator calculation · lines 714–719
Open as its own pageThis proves the copied separation statement: free coherence, including (eq:word), does not itself furnish causal factorization.
Actual tensor relations and an algebraic criterion
sectionActual tensor relations and an algebraic criterionActual tensor relations and an algebraic criterion · IX-E@1#eq:A · lines 720–752
Open as its own pageDouble-ordering tests are necessary but not sufficient. Every actual linear relation among prescribed tensors must also be respected. This obligation is distinct from the already closed degree-four descent.
Write on and define
The inherited classical coefficient of is multiplication. Equation (eq:free-star) implies
Let be the collection of all prescribed values: for every ordered pair, together with for every tensor on a supplied old overlap. The index set need not be finite. Assume these values and their required descendants are admitted, and their classical coefficients equal multiplication. Put
Let
Conjugation induces an antilinear involution on .
theoremTheorem: Algebraic consistency criterionActual tensor relations and an algebraic criterion · IX-E@1#thm:algebraic, IX-E@1#eq:relation-test, IX-E@1#eq:X-involution · proof attached · lines 753–820
Open as its own pageThere exists a complex-linear map satisfying all prescribed values, classical multiplication, symmetry, and the binary involution identities if and only if the following finite-relation condition holds:
for every finite and every complex choice of coefficients.
This is an algebraic theorem. It does not assert fixed-support continuity or identify a distributional time-ordering construction.
Proof. Write . Symmetry is equivalent to , so factors through . The binary involution is equivalent to
For prescribed tensors this requires the assignments
Any linear map must respect their finite relations, proving necessity of (eq:relation-test).
Conversely, that condition defines a complex-linear map on
The space is conjugation-stable, and the assignments give . Set . Then
On the real fixed-point space , the map takes values in the real fixed-point space of .
Choose a real vector-space complement of in , extend by zero there, and complexify. Every has the decomposition
into real fixed-point vectors. The extended therefore remains conjugation-equivariant. Define , pulled back to , and .
The range of lies in , so the classical coefficient is unchanged. The construction gives symmetry, prescribed values, and (eq:X-involution). All outputs are finite linear combinations of admitted coefficient functionals. Linearity of the carrier conditions preserves their required descendants.
sectionActual tensor relations and an algebraic criterionActual tensor relations and an algebraic criterion · lines 820–833
Open as its own pageFor a two-way pair the quotient identifies and , while the forced corrections have opposite signs. Condition (eq:relation-test) therefore requires their common correction to vanish, reproducing Theorem thm:obstruction.
The arbitrary complement in the proof is not a continuity argument. It can produce a discontinuous map even when every prescribed coefficient is admitted. The theorem consequently cannot be used to label the complete IX-E interface Constructed without the remaining analytic proof.
E2–E5: analytical obligations and contacts
sectionE2: replacement contractionsE2–E5: analytical obligations and contacts › E2: replacement contractions · lines 836–879
Open as its own pageOnly after consistency of the forced data is established should an unordered extension be proposed. For every contraction, the construction must specify:
the exact inherited free distribution and slot convention;
the proposed time-ordered distribution;
its differential identity and source-contact normalization;
its restrictions to every ordered region;
the singular set requiring extension;
the residual actual functional after contraction.
The flat contractions mentioned in the prerequisite sheet include and
Their names do not specify a time-ordered replacement. In particular, replacing a differentiated contraction requires deciding whether differentiation is applied to a fundamental solution or whether a distinct differentiated time-ordering convention is used.
The sharp metric slot must be derived from the actual functional derivative through , retaining (eq:sharp). Time ordering by observation times alone is not justified by (eq:support-bounds). Nor may differentiation, sharp Cauchy inversion, or the sharp adjoint be silently commuted with time ordering.
The standard perturbative algebraic framework distinguishes time-ordering on regular functionals from the renormalized extension needed for local functionals FR. Its Feynman-kernel formulas must be used with their distributional hypotheses FR. Those results do not, without a separate verification of hypotheses, construct this nonlocal sharp sector.
A wavefront analysis must determine the actual unresolved set. Observation diagonals, the Cauchy surface, and the reflected branch of are candidates until excluded. The binary target does not require importing the degree-four triangle solely because that triangle exists in the inherited word.
sectionE3: admission and named continuityE2–E5: analytical obligations and contacts › E3: admission and named continuity · lines 880–911
Open as its own pageFor every coefficient, the proof must establish existence of its distributional pairings, compact configuration kernels, the metric derivative condition (eq:admission), all required descendants, and annihilation of actual-presentation kernels.
Existence on a test family does not establish admission. In particular, an expression omitting the boundary contribution in (eq:sharp) cannot be justified by referring to a different presentation of the same functional.
For definiteness, a possible weak fixed-support target is the following. Give the locally convex topology generated by
for all configurations and finite direction lists under consideration. For every named test-function presentation with supports in fixed compact sets, require each to be continuous from the product of the corresponding spaces into this topology.
This is one explicit continuity strength; it is not asserted to follow from the supplied F9a statement. It neither claims normal-topology continuity on the full carrier nor hypocontinuity of multiplication. A different topology may be chosen, but it must be named and proved, rather than inferred from the absence of the joint VII-C assumptions.
sectionE4: contact equations and old overlapE2–E5: analytical obligations and contacts › E4: contact equations and old overlap · lines 912–953
Open as its own pageIf a finite-scaling-degree point-extension theorem applies in dimension , uniqueness holds below degree ; at higher degree the degree-preserving freedom is a finite sum of derivatives of delta of order at most BF. Application to a submanifold requires the corresponding transverse and microlocal hypotheses BF. No such hypotheses or degrees have been evaluated here for the sharp Cauchy or reflected loci.
The parent identity
classifies its triangle finite part. It does not classify binary time-ordered ambiguities.
On every supplied old overlap one must compute
and solve for permitted contacts so that this difference is exactly zero. A smooth nonzero spacelike discrepancy away from the named contact set is not a contact.
All coefficients of , all supplied old free and time-ordered coefficients, and the parent parameter remain fixed. No subtraction inside is authorized.
If source slots are included, differentiating
shows why the simultaneous prescription
cannot retain that fundamental-solution identity when . This excludes that simultaneous prescription; it does not exclude every possible sharp causal extension.
sectionE5: involution is a separate equationE2–E5: analytical obligations and contacts › E5: involution is a separate equation · IX-E@1#eq:antitime, IX-E@1#eq:time-star · lines 954–980
Open as its own pageDefine anti-time-ordering by
The required identity is
Using (eq:A), equations (eq:antitime)– (eq:time-star) are exactly
Symmetry instead requires . The two equations are different.
Contacts must solve the overlap, ordered-restriction, admission, symmetry, and involution equations simultaneously. Averaging a candidate is not proof that its old overlap or causal restrictions survive. The algebraic theorem isolates these constraints, but does not solve the sharp distributional contact problem.
E6: conditional unnormalized subtraction
sectionE6: conditional unnormalized subtractionE6: conditional unnormalized subtraction · lines 981–985
Open as its own pageThe next result audits directly the binary implication quoted from IX-D. It does not presume that its hypotheses have been discharged.
theoremTheorem: Conditional causal subtractionE6: conditional unnormalized subtraction · IX-E@1#thm:subtraction, IX-E@1#eq:Rhat · proof attached · lines 986–1040
Open as its own pageSuppose is constructed on with admitted coefficients and required descendants, classical multiplication, factorization, exact supplied old overlaps, and (eq:antitime)–(eq:time-star). Suppose the inherited free map has the corresponding admission and old-overlap properties. Define
Then:
, including required descendants;
its classical coefficient vanishes;
its supplied old unnormalized retarded overlaps agree exactly;
for , it vanishes if
.
If both input maps satisfy the same named fixed-support continuity statement into a locally convex coefficient space, their difference satisfies that statement.
Proof. Admission and descendant admission follow from linearity of the admitted carrier. The classical coefficients of the two maps are both multiplication, so they cancel. Exact old overlap follows by subtracting the two exact old values.
The stated support condition is equivalent to
Thus , and factorization makes the two terms in (eq:Rhat) equal.
For conjugation, use (eq:free-star) and (eq:time-star):
Finally, addition and scalar multiplication are continuous in a locally convex vector space. No multiplication-continuity upgrade is used.
sectionE6: conditional unnormalized subtractionE6: conditional unnormalized subtraction · lines 1040–1045
Open as its own pageThe support assertion concerns the stated functional-support ordering of a pair. It is not a distributional support theorem for independently unsmeared argument slots.
propositionProposition: Order loss under coefficient shiftingE6: conditional unnormalized subtraction › Normalization audit · proof attached · lines 1048–1070
Open as its own pageThe linear coefficient-shift map
is well defined. Order-three numerator data do not determine an order-three normalized coefficient in .
Proof. The coefficient expansion in is unique, so is well defined. Within , multiplication by annihilates every . Hence, for every ,
The coefficient is undetermined. Equivalently, has no inverse in .
sectionNormalization auditE6: conditional unnormalized subtraction › Normalization audit · lines 1070–1086
Open as its own pageIf the conditional construction is completed, the clean normalized output is the coefficient shift
with any phase convention stated explicitly. A zero choice for an additional coefficient is a truncation convention, not a coefficient derived from order-three numerator data. No normalized product is released here because has not been constructed.
Higher retarded identities require higher time ordering and the relevant intermediate products. Consequently neither nor is defined.
E7: decision, missing data, and exclusions
sectionEvaluated statusE7: decision, missing data, and exclusions › Evaluated status · lines 1089–1129
Open as its own pageGate Status on the fixed target E0 Domain containment and flip, conjugation, and reversal stability are proved. The old seed is explicitly zero. The actual old intersection and any required nonzero old map are not supplied. E1a The exact commutator identity is proved. Its kernel restriction on two-way sharp pairs is not evaluated. E1b A necessary and algebraically sufficient finite-relation criterion is proved. It is not evaluated for the complete forced data. E1c The corrected support geometry, later-slab implication, and a spacelike sufficient condition are proved. E2 No locked sharp time-ordered replacement distribution or extension is supplied. Construction remains unfinished. E3 No candidate coefficient family exists to which the admission and fixed-support continuity proofs can be applied. E4 Binary contact freedom and exact nonzero old-overlap equations are unevaluated. E5 The involution constraint is proved algebraically. It is not discharged for an analytic candidate. E6 The conditional subtraction and normalization audit are proved. Their construction hypotheses remain undischarged. theoremTheorem: Release decisionE7: decision, missing data, and exclusions › Evaluated status · proof attached · lines 1130–1149
Open as its own pageRelative to the supplied prerequisite information, the IX-E release outcome on (eq:fixed-domain) is Unresolved. No Constructed or Proved obstructed outcome is established.
Proof. A Constructed outcome requires a map satisfying every declared clause. No sharp replacement distribution, admitted coefficient construction, complete old-overlap solution, or continuity proof has been supplied.
A Proved obstructed outcome requires an evaluated incompatibility. Theorem thm:obstruction supplies such a criterion, but its nonzero kernel premise has not been established on a two-way pair. Likewise, no violation of (eq:relation-test) has been evaluated. The ordered slab excludes classical multiplication only. Therefore the remaining obligations have precisely the third legal status.
sectionEvaluated statusE7: decision, missing data, and exclusions › Evaluated status · lines 1149–1160
Open as its own pageThe earliest unevaluated causal calculation is the restriction of
to admitted pairs for which the support geometry supplies both orderings, followed by the full actual-relation test. The exact locked kernel formula or an appropriate conjugation-support theorem is needed to finish it. Independently, a nonzero old-overlap claim requires the actual old map, not merely its name.
sectionRetained non-identificationsE7: decision, missing data, and exclusions › Retained non-identifications · lines 1161–1175
Open as its own pageThe inherited product is not and is not . The triangle scalar is not a causal subtraction. V's , the oscillator coefficient, and the Newton–wave cubic remain different objects. VI's relational coefficient and VII-A's plateau intertwiner are not the map sought here. VII-E/F and VIII certificates have no supplied map into .
A cutoff or numerical modification of supplies none of the missing order- and order- binary coefficients. The parent finite-part conversion also supplies no binary overlap classification.
sectionG2 and VII-C remain closedE7: decision, missing data, and exclusions › G2 and VII-C remain closed · lines 1176–1195
Open as its own pageThe compact-switch witness copied from IX-A and IX-D is
with nonzero dressing variation under its stated hypotheses. In the coupling expansion its nonzero order- coefficient cannot be canceled by a correction beginning at order : coefficient extraction at order annihilates every such correction. Binary time ordering therefore does not open G2.
VII-C remains in force under its original joint hypotheses (E1)–(E4), which are distinct from the gate labels of this paper. Subtracting a scalar finite part does not prove normal-topology admission continuity. F9a and separate pointwise continuity are not promoted to F9b or hypocontinuity.
Conclusion
sectionConclusionConclusion · lines 1196–1218
Open as its own pageThe first-stage commutator is controlled by the imaginary part of the locked kernel, not by full support or injectivity. Double ordering means causal disjointness of functional supports. A nonzero commutator on any retained two-way pair is a universal obstruction on the fixed domain, and no contact can remove that contradiction without changing prescribed free data.
If the prescribed values instead satisfy all actual relations, Theorem thm:algebraic supplies an algebraic extension criterion. Its arbitrary linear extension is not a substitute for a sharp distributional construction or continuity proof. Admission, contacts, old overlap, and continuity must still be established at the declared analytical strength.
Once those obligations are discharged, Theorem thm:subtraction supplies the unnormalized binary retarded difference through . Normalization shifts the determined order to . With the information presently supplied, the honest release remains Unresolved; the free-sector descent and every stated external boundary remain unchanged.
bibliographyReferencesConclusion · lines 1219–1248
Open as its own pageFR
K. Fredenhagen and K. Rejzner, Perturbative algebraic quantum field theory, arXiv:1208.1428 [math-ph], 2012. Used for the distinction between regular time-ordering formulas and renormalized extensions; not invoked as an existence theorem for the sharp sector.
BF
R. Brunetti and K. Fredenhagen, Microlocal analysis and interacting quantum field theories: Renormalization on physical backgrounds, Communications in Mathematical Physics 208 (2000), 623–661; arXiv:math-ph/9903028. Used only for extension principles under their stated scaling-degree and microlocal hypotheses.
Internal
Internal prerequisite statements: IX-A, IX-Free-2, and IX-D, as quoted in the supplied IX-E specification. The full source manuscripts, the individual wording of C-I1–C-I9, the locked formula for , and a nonzero old time-ordered comparison map were not supplied. Statements imported from these prerequisites are identified as premises rather than reconstructed proofs.