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Manuscript IX-Free-2@1 · IX-Free-2.tex · abb2397a

Landmark IX-Free-2 Degree-four descent and overlap agreement for one sharp ordered word

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Relative to its stated inherited premises, constructs degree-four descent and simultaneous overlap agreement, and one truncated partial product on the named domain D_decl. Both associations of the selected word agree through order hbar^3, and C_desc and C_glue are all of R. Actual-stage continuity, associativity for unspecified triples, a causal lift, and G2 are not asserted. No compilation is asserted.

Front matter

  • abstractAbstractFront matter · lines 132–161
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    We complete the algebraic descent and overlap tests left open in IX-Free for the ordered word . The previously constructed graph outputs are used as inherited values.

    A compact spatial-diagonal metric direction, obtained by applying the wave operator to a test tensor, proves sharp-generator separation even when the -metric component is constrained to vanish. Slot isolation then proves injectivity of both degree-four presentation maps. Consequently all four prescribed degree-four coefficients descend to actual functionals.

    An explicit advanced-trace witness proves that every nonzero sharp generator has nonzero intrinsic metric-derivative charge at some smooth configuration. The partial contractions have zero charge. The old microcausal algebra also has zero charge: a nonzero boundary coefficient would produce a timelike conormal singularity. These facts eliminate the live new-domain intersection and separate the sharp space from the old algebra. An algebraic anchored-domain lemma eliminates the old overlap of the entire new-domain sum, including possible multi-domain relations.

    For every real common parent parameter, the prescriptions therefore glue to one truncated partial product preserving the locked first stages and the old product. The two associations of the selected word agree through order . Reversal, presentation independence, and fixed-support test-family continuity hold. Actual-stage continuity, associativity on unspecified triples, and the IX-D and G2 constructions are not asserted.

  • figureOne partial product stays relativeFront matter · IX-Free-2@1#fig:scope-IX-Free-2 · lines 163–176
    Named tensor domain
    →
    Truncated partial product
    →
    Absolute time-ordered product
    The product is relative to the inherited premises.

    One partial product stays relative. 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.

  • figureOne partial product stays relativeFront matter · IX-Free-2@1#fig:split-IX-Free-2 · lines 178–189
    Named tensor domain
    Absolute time-ordered product
    The product is relative to the inherited premises.

    One partial product stays relative. 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-Free-2@1#fig:chain-IX-Free-2 · lines 191–204
    Named tensor domain
    ↓
    Truncated partial product
    ↓
    Absolute time-ordered product
    The product is relative to the inherited premises.

    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.

  • figureNamed tensor domain is not Absolute time-ordered productFront matter · IX-Free-2@1#fig:pair-IX-Free-2 · lines 206–219
    Named tensor domain
    not the same object
    Absolute time-ordered product
    Truncated partial product. The product is relative to the inherited premises.

    Named tensor domain is not Absolute time-ordered product. 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-Free-2@1#fig:gate-IX-Free-2 · lines 221–234
    Named: Named tensor domain
    →
    Used here: Truncated partial product
    →
    Not claimed: Absolute time-ordered product
    The product is relative to the inherited premises.

    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 234–243
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    Figure fig:split-IX-Free-2 records one view of the same separation. Figure fig:chain-IX-Free-2 records one view of the same separation. Figure fig:pair-IX-Free-2 records one view of the same separation. Figure fig:gate-IX-Free-2 records one view of the same separation. The drawings add no hypothesis.

    Figure fig:scope-IX-Free-2 records that separation. The drawing adds no hypothesis.

  • scopeRelease and scopeFront matter · lines 244–254
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    and scope{ Release: Constructed, relative to the inherited premises stated below. The result is one truncated partial product on an explicitly named tensor domain, together with coherence for the single ordered word .

    No graph-existence or triangle-calibration proof is reconstructed. No Einstein equation, time-ordered product, retarded product, global quantum algebra, causal-support lift, IX-D construction, or G2 opening is included.}

Release alternatives and inherited contract

  • sectionRelease alternatives and inherited contractRelease alternatives and inherited contract · lines 260–281
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    The release alternatives are kept distinct:

    1. Constructed: the prescribed coefficients descend and glue with all declared existing coefficients, satisfying the copied interfaces on the named sector.

    2. Canonical prescription obstructed: an explicit actual-presentation relation or overlap discrepancy contradicts the prescribed coefficients.

    3. Contract proved obstructed: a contradiction excludes every coefficient system satisfying the copied interfaces.

    4. Unresolved: a required proof remains unfinished.

    A missing proof is not an obstruction. Failure of one prescription is not a universal contract obstruction.

    Fix one real parent parameter at the outset. It is not changed by association, presentation, or observation descendant. The results below hold for every such fixed .

  • sectionGeometry and smooth operatorsRelease alternatives and inherited contract › Geometry and smooth operators · IX-Free-2@1#eq:C, IX-Free-2@1#eq:generators · lines 282–329
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    Let

    with metric

    Metric configurations are smooth symmetric covariant tensors. Set

    The operator is the inverse of with zero Cauchy value and zero first time derivative at . The operator is the componentwise advanced inverse of the same massless wave operator.

    All configurations and directions are smooth and off shell. Compact directions supported in are allowed. We use the usual smooth mapping properties, Cauchy uniqueness, and finite propagation of these fixed linear operators.

    With

    the generators are

    Complex tests define complex-valued functionals on real smooth configurations. Complexified directions can equivalently be used by multilinearity.

  • sectionExplicit inherited premisesRelease alternatives and inherited contract › Explicit inherited premises · lines 330–335
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    The supplied IX-Free source is used through the following ledger. Statements reported there from companion manuscripts remain inherited premises, not independently certified companion proofs.

  • assumptionAssumption: Carrier, charge, and classical operationsRelease alternatives and inherited contract › Explicit inherited premises · IX-Free-2@1#ass:carrier, IX-Free-2@1#eq:admission, IX-Free-2@1#eq:charge, IX-Free-2@1#eq:boundary · lines 336–379
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    The carrier consists of actual finite polynomial functionals with compact symmetric distributional kernels, subject to

    for every smooth configuration and every finite list of smooth configuration directions .

    The linear sharp kernels and intrinsic charge are

    The charge is well defined on actual linear kernels and vanishes on . Every element of has no nonzero nonspacelike wavefront covector; compact smooth metric kernels belong to .

    The sharp adjoint retains its surface term:

    Classical multiplication, smooth directional differentiation, and conjugation preserve . Classical multiplication is separately continuous in the locally convex topology , which records strong compact-distribution coefficients and all intrinsic trace coordinates.

    The generating test maps are injective and have fixed-support test-family continuity. The inherited nonconvergence in for nonzero real is retained, but is not used as a charge witness.

  • assumptionAssumption: Old microcausal productRelease alternatives and inherited contract › Explicit inherited premises · IX-Free-2@1#ass:old · lines 381–403
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    The full old compact polynomial microcausal algebra is included in . Its functional derivatives satisfy the standard microcausal wavefront condition: no nonzero joint covector is entirely future causal or entirely past causal, where zero individual covectors are allowed in those closed causal cones.

    The inherited old product is defined on , has classical order zero, and has its unchanged coefficients

    For the reversal statement we use the inherited Hermitian old convention

    No new continuity property of is introduced.

  • sectionExplicit inherited premisesRelease alternatives and inherited contract › Explicit inherited premises · lines 403–409
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    The microcausal condition just specified is the usual functional-derivative condition; see FR. We will prove the zero-charge consequence needed here, rather than infer it from the informal word “bulk.”

  • assumptionAssumption: Locked stages and inherited graph outputsRelease alternatives and inherited contract › Explicit inherited premises · IX-Free-2@1#ass:graphs, IX-Free-2@1#eq:firstL, IX-Free-2@1#eq:firstR, IX-Free-2@1#eq:oneedges, IX-Free-2@1#eq:G1223, IX-Free-2@1#eq:G1213, IX-Free-2@1#eq:G1323, IX-Free-2@1#eq:degree2L, IX-Free-2@1#eq:degree2R · lines 410–490
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    The fixed mixed kernel has . The first stages are the actual maps

    Their metric derivatives are compact smooth kernels, also after the required directional insertions.

    Write

    for the fixed scalar contraction kernel, and

    The three one-edge outputs

    exist and belong to .

    For , the three two-edge values are the already defined and admitted functionals

    Their defining wavefront products, compact coefficient kernels, admission decompositions, and all required descendants have already been established in IX-Free. Their fixed-support test-family continuity is inherited.

    The maps defined below are injective. The inherited degree-two second-stage maps are

    They are maps on actual arguments, with inherited reversal and presentation independence.

  • assumptionAssumption: One calibrated parentRelease alternatives and inherited contract › Explicit inherited premises · IX-Free-2@1#ass:parent, IX-Free-2@1#eq:parent · lines 492–513
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    Fix the inherited regulator and scale. The calibrated distributions exist under the analytical premise explicitly reported in IX-Free. For the one fixed real parameter , set

    The parent has dagger symmetry under conjugation and exchange of , and its declared numerical observation operations use this same parameter. Algebraic scalar descent has already been evaluated:

    The scalar family has inherited fixed-support continuity. No claim about arbitrary nonconstant contact terms follows from this scalar calibration.

  • sectionExplicit inherited premisesRelease alternatives and inherited contract › Explicit inherited premises · lines 513–519
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    The sign ledger is unchanged: each first-stage partial has factor ; the complete word has two sharp insertion signs, whose product is ; the middle-slot assignment factor is , not .

  • requirementRequirement: C-I1–C-I9Release alternatives and inherited contract › Copied interfaces · IX-Free-2@1#req:interfaces · lines 522–540
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    The construction must satisfy:

    1. Every output is admitted, including the required metric derivatives and directional descendants.

    2. Order zero is classical multiplication.

    3. Every specified old-product overlap agrees with .

    4. The first stages are locked to (eq:firstL)–(eq:firstR).

    5. The constant kernel is , using one real common parent parameter and its declared observation compatibility.

    6. No subtraction changes a fixed old product.

    7. Unchanged approximants need not converge sharply in .

    8. All finite relations between actual presentations are respected.

    9. Every continuity claim has a named domain and proof; test-family continuity is not actual-stage hypocontinuity.

  • sectionCopied interfacesRelease alternatives and inherited contract › Copied interfaces · lines 540–583
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    {}1.12

    ObjectEntering statusPresent obligation
    First stages and one-edge outputsConstructed, inheritedRetain their values
    Two-edge outputs and admissionConstructed in IX-FreeUse, do not reconstruct
    , degree-two mapsConstructed in IX-FreeOverlap agreement
    Evaluated as Do not reopen
    Concrete, unevaluatedEvaluate the kernels
    Degree-four coefficientsValues admitted; descent openActual-functional descent
    Live degree-two intersectionUnevaluatedSeparate its factors
    Old and sum-domain overlapsUnevaluatedSimultaneous gluing
    F9aConstructed for inherited familiesExtend to degree-four families
    F9bUnclaimedNo assertion here

Actual spaces, declared domain, and coefficient assignment

  • sectionActual spaces, declared domain, and coefficient assignmentActual spaces, declared domain, and coefficient assignment · IX-Free-2@1#eq:Dfirst, IX-Free-2@1#eq:Dsecond, IX-Free-2@1#eq:Dnewold, IX-Free-2@1#eq:Ddecl · lines 585–693
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    All spans and tensor products in this paper are algebraic over . Define

    and

    These last sums are direct by total field degree. The actual spaces coincide, but their ordered roles remain distinct.

    Let

    with ordered presentation maps

    Inside , the declared domains are

    Thus the full inherited old domain is used, not a smaller regular subdomain.

    We will define coefficient maps

    Their prescribed restrictions are displayed below. On the degree-four rows, initially denote the labelled prescriptions; their actual descent is proved in Section sec:descent.

    {}1.2

    Domain

    On every row,

    The explicit zero entries are part of the selected contraction prescription. They are not a classification excluding every alternative contact term.

The concrete degree-four relation kernel

  • sectionThe concrete degree-four relation kernelThe concrete degree-four relation kernel · IX-Free-2@1#eq:P, IX-Free-2@1#eq:Prelation, IX-Free-2@1#eq:lambdaL, IX-Free-2@1#eq:lambdaR, IX-Free-2@1#eq:annihilation · lines 695–771
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    For

    use the inherited injective realization of this algebraic tensor product as smooth compact joint functions.

    Let be the distribution kernel of , and let . The relation kernel is copied unchanged:

    The symmetrization is the average over the three metric slots. IX-Free establishes

    For , set . The right relation is

    Full coefficient recovery uses one scalar derivative and three metric derivatives. The metric polarization factor is . Two metric derivatives do not recover this coefficient.

    The prescribed values whose descent remains to be proved are

    They descend precisely when

    We now evaluate the kernels. No inference from injectivity of will be used.

Gate K: restricted sharp separation and kernel evaluation

  • sectionGate K: restricted sharp separation and kernel evaluationGate K: restricted sharp separation and kernel evaluation · lines 773–778
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    The restricted separation lemma can be proved without a general range theorem for .

  • lemmaLemma: Restricted sharp-generator separationGate K: restricted sharp separation and kernel evaluation · IX-Free-2@1#lem:restricted, IX-Free-2@1#eq:compactinverse · proof attached · lines 779–827
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    Let . Suppose

    for every smooth symmetric metric direction with and every smooth scalar . Then . It is enough to use compact metric directions supported in .

    Proof. For , let have its only nonzero component

    Then . Because has constant coefficients,

    The vector is compactly supported away from , so has zero Cauchy data there. Cauchy uniqueness gives

    Directly from (eq:C),

    Choose . This is an allowed smooth configuration. Alternatively, use a compact smooth scalar agreeing with near . The hypothesis becomes

    for every . Hence . A smooth function independent of on and compactly supported there must vanish. Thus .

    Real already suffice for complex , by applying the distributional identity to its real and imaginary parts.

  • sectionGate K: restricted sharp separation and kernel evaluationGate K: restricted sharp separation and kernel evaluation · lines 827–833
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    The test direction is off shell. Equation (eq:compactinverse) is an identity for the fixed Cauchy inverse on compact zero-data tests, not an equation-of-motion restriction on configurations.

  • theoremTheorem: Injectivity of the degree-four presentationsGate K: restricted sharp separation and kernel evaluation · IX-Free-2@1#thm:pinjective, IX-Free-2@1#eq:isolation · proof attached · lines 834–895
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    The maps

    are linear isomorphisms onto their actual-functional images. In particular,

    Proof. Suppose . Choose metric directions with

    where ; the other components of may be zero. Differentiate once in a scalar direction and three times in these metric directions at the zero configuration.

    Using the unsymmetrized functional expression,

    the only surviving terms place in the -slot. Consequently the derivative is exactly

    The factor is the surviving permutation count after ; it is consistent with the recovery of the fully symmetric coefficient.

    Define

    It is a smooth compact test. Since (eq:isolation) vanishes for all , Lemma lem:restricted gives for every .

    For any , take and choose equal to one near . Then

    for every . Thus every -test contraction of vanishes, so as a joint smooth function and hence as an algebraic tensor.

    The right map is the same classical product after . Therefore its kernel is also zero. Surjectivity onto the named images is their definition.

  • corollaryCorollary: Evaluation of the copied relation equationGate K: restricted sharp separation and kernel evaluation · IX-Free-2@1#cor:Pevaluated · proof attached · lines 897–909
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    For the algebraic presentation tensors of this paper,

    The exchanged right equation has the same conclusion.

    Proof. Combine (eq:Prelation) with Theorem thm:pinjective.

  • sectionGate K: restricted sharp separation and kernel evaluationGate K: restricted sharp separation and kernel evaluation · lines 909–915
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    The conclusion concerns this particular polynomial product. It is not the false general principle that products of injective linear generating maps are automatically tensor-injective.

Gate A: degree-four descent

  • theoremTheorem: Descended degree-four coefficient mapsGate A: degree-four descent · IX-Free-2@1#thm:degree4 · proof attached · lines 920–947
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    The four prescriptions (eq:lambdaL)–(eq:lambdaR) define unique algebraic bilinear maps

    with the prescribed values.

    Proof. Theorem thm:pinjective makes both relation kernels zero. Thus all four annihilation tests (eq:annihilation) hold.

    More explicitly, an element of has a unique presentation tensor in , and an element of has a unique sharp test. The graph prescriptions are linear in that tensor and in the additional test. They therefore define unique bilinear maps on the actual images. The same argument applies on the right.

    Their values are finite sums of inherited admitted graphs, so belong to , including the required admission descendants. Classical multiplication defines .

  • sectionGate A: degree-four descentGate A: degree-four descent · lines 947–953
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    No operation on an unproved “zero graph factor” is used. Linearity becomes sufficient only after the relevant actual presentation kernel has been evaluated as zero.

Gate S: boundary-charge separation

  • sectionGate S: boundary-charge separationGate S: boundary-charge separation · lines 955–961
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    We first justify the zero-charge property of the old algebra using only its microcausal definition and the copied sharp boundary identity.

  • sectionNonzero charge forces a timelike boundary singularityGate S: boundary-charge separation › Nonzero charge forces a timelike boundary singularity · IX-Free-2@1#eq:Bsurface · lines 962–980
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    For the component convention in (eq:C), integration by parts gives

    Its surface coefficient in (eq:boundary) is

    In particular, is injective on the boundary covector .

  • lemmaLemma: A nonzero surface coefficient is not microcausalGate S: boundary-charge separation › Nonzero charge forces a timelike boundary singularity · IX-Free-2@1#lem:surfaceWF · proof attached · lines 981–1011
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    Let be smooth near . If , then has a nonzero timelike wavefront covector.

    Proof. By (eq:Bsurface), some component of is nonzero on a boundary patch. That component has local form

    with smooth.

    Choose compact localizers , with , so that . The Fourier transform of the localized delta term at is this nonzero constant. The transform of the localized Heaviside term is , by one-sided integration by parts. Thus the localized distribution is not rapidly decreasing along the normal rays as .

    If the distribution had no timelike wavefront covectors on that compact patch, the local wavefront estimates, after a finite partition of unity, would give rapid decay in a cone around those normal rays. This contradicts the preceding asymptotic. Hence a timelike covector occurs.

  • lemmaLemma: Microcausal admitted linear kernels have zero chargeGate S: boundary-charge separation › Nonzero charge forces a timelike boundary singularity · IX-Free-2@1#lem:MCcharge · proof attached · lines 1013–1030
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    If has no nonzero nonspacelike wavefront covector, then .

    Proof. Write . The kernel has only spacelike wavefront covectors by Assumption ass:carrier. Therefore

    also has no nonspacelike covector. The source is compact smooth, so is smooth. Lemma lem:surfaceWF forces . Equation (eq:charge) now gives the conclusion.

  • sectionNonzero charge forces a timelike boundary singularityGate S: boundary-charge separation › Nonzero charge forces a timelike boundary singularity · lines 1030–1036
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    This argument does not reverse the stated inclusion for : it does not assume that every spacelike linear kernel has already been identified with an element of .

  • propositionProposition: Zero-charge comparison classesGate S: boundary-charge separation › Nonzero charge forces a timelike boundary singularity · IX-Free-2@1#prop:zerocharge · proof attached · lines 1037–1073
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    At every smooth configuration and after every finite smooth directional insertion,

    for

    Proof. For the partial contractions, the inherited metric derivative is compact smooth. Inserting a scalar direction replaces the smooth scalar configuration by that direction. Inserting a metric direction removes the only metric slot, so subsequent metric differentiation is zero. Higher derivatives vanish by polynomial degree. All nonzero metric kernels in this calculation are therefore compact smooth elements of , with zero charge.

    For , contraction of its higher functional derivatives against smooth directions is a proper pushforward after inserting compact cutoffs equal to one on the coefficient supports. A wavefront covector of the remaining one-slot kernel can arise only from a joint covector with all integrated covectors zero.

    A nonzero causal covector in the remaining slot, together with those zeros, would belong entirely to one of the excluded closed causal cones. Thus the remaining metric kernel has only spacelike wavefront covectors. It belongs to by carrier admission, and Lemma lem:MCcharge proves its charge is zero.

  • sectionAn explicit sharp trace witnessGate S: boundary-charge separation › An explicit sharp trace witness · IX-Free-2@1#eq:advancedtrace · lines 1075–1101
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    The following trace formula fixes the sign for :

    It is the advanced Kirchhoff formula; compare Ivrii. To see the normalization, the spatial Fourier transform of , for , is . The zero-future-data solution of

    at is

    Inverting the spatial transform gives (eq:advancedtrace).

  • lemmaLemma: Sharp charge separation for every nonzero testGate S: boundary-charge separation › An explicit sharp trace witness · IX-Free-2@1#lem:sharpcharge, IX-Free-2@1#eq:Bderivative, IX-Free-2@1#eq:positivewitness · proof attached · lines 1102–1165
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    For every nonzero , there is a real smooth scalar configuration , which can be chosen compactly supported in , such that

    No directional descendant is needed.

    Proof. The metric derivative is

    Choose with . Select with

    Since , a neighborhood of can be chosen away from the spatial point . Let

    on that neighborhood. Choose , nonnegative and positive at , and form the complex scalar

    Extended by zero outside , it is compact smooth.

    On the cone ,

    Using (eq:advancedtrace) and (eq:Bderivative),

    The denominator is bounded away from zero on the relevant support. Positivity holds on an open spatial patch near .

    Write with real compact smooth . The trace is complex linear in the scalar configuration. Since (eq:positivewitness) is nonzero, at least one of the traces for is nonzero. Choose that real configuration. The metric configuration may be zero, since (eq:Bderivative) is independent of .

  • sectionAn explicit sharp trace witnessGate S: boundary-charge separation › An explicit sharp trace witness · lines 1165–1169
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    This witness is independent of the inherited nonconvergence of regularized sharp generators.

  • theoremTheorem: The required actual-space separationsGate S: boundary-charge separation › An explicit sharp trace witness · IX-Free-2@1#thm:separation · proof attached · lines 1170–1203
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    The intersections are

    Consequently,

    Proof. Every element of is for one test , because the generating map is linear. A nonzero such element has . Lemma lem:sharpcharge gives a configuration at which its metric derivative has nonzero charge.

    Every element of either partial-contraction space or the old algebra has zero charge at that configuration by Proposition prop:zerocharge. Equality of actual functionals would imply equality of their actual metric derivatives and intrinsic charges, a contradiction.

    For algebraic tensor products,

    Apply this identity to the displayed degree-two domains.

Gate G: simultaneous new-domain and old-domain gluing

  • sectionCompatibility of all new domainsGate G: simultaneous new-domain and old-domain gluing › Compatibility of all new domains · lines 1210–1234
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    Metric–scalar homogeneity separates the locked first stages from the second stages. The species degrees are

    Here the entries count metric and scalar slots.

    The six new domains therefore have argument species degrees

  • propositionProposition: Direct decomposition of the new domainGate G: simultaneous new-domain and old-domain gluing › Compatibility of all new domains · IX-Free-2@1#prop:newdirect, IX-Free-2@1#eq:newdirect · proof attached · lines 1235–1272
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    The new domain is the algebraic direct sum

    The prescribed coefficient maps therefore glue uniquely on .

    Proof. The zero intersections involving the degree-four blocks are the inherited field-degree results of IX-Free. The locked first-stage domains have species degrees distinct from all second-stage domains and from each other.

    All relations can be projected onto the distinct homogeneous argument-species components. The only component containing two listed domains is . Its two domains have zero intersection by Theorem thm:separation. Thus that sum is direct as well.

    This proves a direct decomposition of the entire sum, not merely pairwise agreement. Each coefficient restriction is an actual linear map by the inherited first stages, inherited degree-two descent, and Theorem thm:degree4. Their sum is consequently a unique linear map on .

  • lemmaLemma: Vanishing of the old overlap of an anchored sumGate G: simultaneous new-domain and old-domain gluing › An anchored-domain lemma · IX-Free-2@1#lem:anchored · proof attached · lines 1276–1296
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    Let be a complex vector space and let satisfy . Then

    Proof. On , define . Extend this linear map algebraically to , using a vector-space complement, with values in . Then

    The map is the identity on and vanishes on . An element in their intersection must therefore be both unchanged and annihilated by this map, hence zero.

  • sectionAn anchored-domain lemmaGate G: simultaneous new-domain and old-domain gluing › An anchored-domain lemma · lines 1296–1299
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    No continuity of is asserted or needed.

  • theoremTheorem: Whole-sum old-product compatibilityGate G: simultaneous new-domain and old-domain gluing › An anchored-domain lemma · IX-Free-2@1#thm:oldgluing · proof attached · lines 1300–1330
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    The full new-domain sum has zero old overlap:

    Thus

    For each fixed real , all prescribed coefficients glue uniquely with the unchanged old coefficients on .

    Proof. Every new domain has a factor in in at least one argument. Hence

    Theorem thm:separation gives . Apply Lemma lem:anchored with , , and . This proves vanishing of the old overlap of the entire new sum, including any potential sum-domain relation.

    Proposition prop:newdirect already constructs each coefficient on . Combining it with on the disjoint old domain gives a unique map on .

  • sectionAn anchored-domain lemmaGate G: simultaneous new-domain and old-domain gluing › An anchored-domain lemma · lines 1330–1334
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    This proof does not subtract a regular coefficient, alter a fixed old product, or make a convergence assertion.

  • sectionEvaluation of the gluing parameter setGate G: simultaneous new-domain and old-domain gluing › Evaluation of the gluing parameter set · lines 1335–1342
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    Define

  • corollaryCorollary: All real common parents pass gluingGate G: simultaneous new-domain and old-domain gluing › Evaluation of the gluing parameter set · IX-Free-2@1#cor:cglue · proof attached · lines 1343–1360
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    For this declared sector,

    Proof. The first equality is inherited. Every degree-four prescription descends independently of . The degree-two scalar maps descend for every real .

    Proposition prop:newdirect and Theorem thm:oldgluing show that the complete declared domain has no overlap imposing an additional scalar equation. Thus gluing holds for every real .

  • sectionEvaluation of the gluing parameter setGate G: simultaneous new-domain and old-domain gluing › Evaluation of the gluing parameter set · lines 1360–1366
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    The parameter is free only within the inherited parent family. No conclusion is drawn about other normalizations or larger domains.

The constructed truncated partial product

  • definitionDefinition: Truncated partial productThe constructed truncated partial product · IX-Free-2@1#def:product · lines 1371–1384
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    For , set

    Extend this map -linearly to

    A pair of formal functionals is admissible when its formal tensor lies in . On such a pair, the partial product is obtained by this linearized map.

  • sectionThe constructed truncated partial productThe constructed truncated partial product · lines 1384–1389
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    This formulation does not assert that every pair of elements of is admissible, or that the declared domain is closed under every intermediate multiplication.

  • propositionProposition: Interface auditThe constructed truncated partial product · IX-Free-2@1#prop:interfaces · proof attached · lines 1390–1423
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    The product of Definition def:product satisfies C-I1–C-I9 on its declared sector, with the continuity assertions proved in Section sec:continuity.

    Proof. For C-I1, every new positive coefficient is a finite sum of inherited admitted graphs or an admitted constant. Classical closure handles ; old coefficients are inherited. All required admission descendants are included in those statements.

    C-I2 is the definition of . C-I3 follows from the unchanged restriction

    the simultaneous-gluing proof shows this restriction is well defined. C-I4 is the first-stage coefficient assignment.

    For C-I5, the only new scalar coefficients are the inherited maps with kernel , using the one parameter fixed at the start. Their observation compatibility is recorded below. No new parent is selected during descent or gluing.

    C-I6 holds because no old coefficient is changed. C-I7 is respected because no convergence of unchanged sharp approximants is invoked. C-I8 follows from descent to actual spaces and unique gluing on the full declared domain. C-I9 is satisfied by the precisely delimited fixed-support continuity theorem; no actual-stage continuity is asserted.

Gate C: coherence for the selected word

  • sectionGate C: coherence for the selected wordGate C: coherence for the selected word · lines 1427–1444
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    Write

    Both formal intermediate tensors

    belong to . Thus both associations now exist.

  • theoremTheorem: Wordwise coherence through order threeGate C: coherence for the selected word · IX-Free-2@1#thm:coherence · proof attached · lines 1445–1500
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    For every fixed real common parent ,

    Their common coefficients are

    Proof. The left association is

    and the right association is

    There is no contribution on these new blocks by the selected coefficient assignment.

    Classical associativity gives equality at order zero. The descended degree-four prescriptions and inherited degree-two maps give

    These are now equalities of coefficients of existing actual partial products. Equality of all four coefficients is equality in .

  • sectionGate C: coherence for the selected wordGate C: coherence for the selected word · lines 1500–1510
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    The residual total field degrees are . This theorem is coherence for the selected word, not associativity for every triple whose individual factors happen to lie in .

    A discrepancy in a nonconstant coefficient could not be moved into , since the scalar and nonconstant orders are distinct.

Reversal, presentation independence, and observations

  • sectionReversal, presentation independence, and observationsReversal, presentation independence, and observations · lines 1512–1523
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    For an actual functional, denotes complex conjugation on real configurations. On the tensor domain define

    This reversal-conjugation, rather than componentwise conjugation alone, is the appropriate domain operation for a partial-product involution.

  • theoremTheorem: Partial-product reversalReversal, presentation independence, and observations · IX-Free-2@1#thm:reversal · proof attached · lines 1524–1572
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    The declared domain is dagger stable and, for ,

    Consequently every admissible pair has an admissible reversed conjugate pair and

    The formula extends coefficientwise to formal admissible pairs, with .

    Proof. Reality of the smooth operators gives

    The inherited first-stage exchange gives

    Thus dagger exchanges the two first-stage domains and the corresponding left and right second-stage domains. The old domain is dagger stable by its inherited convention.

    On the descended degree-four blocks, the inherited graph exchanges give

    For example, exchanges with , and exchanges with . The inherited degree-two reversal gives the same identity on those blocks. The scalar exchange uses real and the parent dagger symmetry. Classical multiplication and the zero coefficients obey the identity as well.

    It holds on the old domain by Assumption ass:old. Unique gluing on extends these component identities to every declared tensor.

  • sectionReversal, presentation independence, and observationsReversal, presentation independence, and observations · lines 1572–1577
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    Componentwise conjugation of an ordered left block need not remain a left block. No stronger componentwise domain-stability assertion is needed.

  • propositionProposition: Actual-functional presentation independenceReversal, presentation independence, and observations · IX-Free-2@1#prop:presentation · proof attached · lines 1578–1596
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    The constructed coefficient maps preserve every rewriting that leaves the declared tensor of actual off-shell functionals unchanged. This includes finite presentation relations, polarization, kernel permutations, tensor symmetries, and integration by parts with all boundary terms retained.

    Proof. The coefficient maps are linear maps on a subspace of the actual tensor product . Within the presentation blocks, actual equality is respected by the inherited degree-two descent and Theorem thm:degree4. Across blocks it is respected by simultaneous gluing. Hence equal actual tensors have equal coefficients.

  • sectionReversal, presentation independence, and observationsReversal, presentation independence, and observations · lines 1596–1601
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    The surface term in (eq:boundary) remains part of the actual kernel. Omitting it changes the argument; it is not a presentation rewrite. No equation-of-motion quotient is introduced.

  • propositionProposition: One-parent numerical observation compatibilityReversal, presentation independence, and observations · IX-Free-2@1#prop:observations · proof attached · lines 1602–1624
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    For every declared smooth multiplier and smooth-coefficient differential operator on ,

    In particular,

    The parameter in these identities is the same used in the partial product.

    Proof. These are distributional differentiation and multiplication identities for the fixed parent (eq:parent). The inherited numerical calibration supplies the declared analytical compatibility. No descent or gluing step changes the parent.

  • sectionReversal, presentation independence, and observationsReversal, presentation independence, and observations · lines 1624–1631
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    A general joint observation multiplier supplies a numerical operation. It does not, without a separate factorization, enlarge the actual partial-product domain or open new configuration slots.

Gate T: fixed-support continuity and its boundary

  • sectionGate T: fixed-support continuity and its boundaryGate T: fixed-support continuity and its boundary · lines 1633–1647
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    Fix compact sets

    These are Fréchet spaces with their usual smooth seminorms.

    We first record the continuity argument needed for classical products of inherited families.

  • lemmaLemma: Fréchet multilinear continuityGate T: fixed-support continuity and its boundary · IX-Free-2@1#lem:Frechet · proof attached · lines 1648–1671
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    A separately continuous finite multilinear map from a finite product of Fréchet spaces to a locally convex space is jointly continuous.

    Proof. It suffices to obtain a local bound for each target seminorm. Induct on the number of arguments. For a fixed first argument, the map of the remaining arguments is jointly continuous by induction.

    Choose countable neighborhood bases in the remaining Fréchet spaces. The sets of first arguments for which the target seminorm is bounded by one on a specified product of those neighborhoods are closed, balanced, and convex. Their countable dilates cover the first space. The Baire theorem therefore makes one such set have interior; its balanced convex structure then gives a neighborhood of zero. This supplies the required bound on a product of neighborhoods. Multilinearity and homogeneity give joint continuity.

  • sectionGate T: fixed-support continuity and its boundaryGate T: fixed-support continuity and its boundary · lines 1671–1677
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    For completeness, the one-edge factor has the fixed-support continuity needed below. This is a mapping estimate for an inherited value, not a new graph construction.

  • lemmaLemma: Continuity of the sharp–sharp one-edge familyGate T: fixed-support continuity and its boundary · IX-Free-2@1#lem:Tcontinuity · proof attached · lines 1678–1726
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    For fixed , the map

    is jointly continuous from to .

    Proof. Its compact coefficient kernels arise from the fixed distribution , multiplication by , and the fixed field-slot transpositions of . The compact-distribution estimates and continuity of these transpositions are the same inherited operations used in IX-Free. They control all strong coefficient seminorms.

    At a fixed smooth metric configuration, its metric derivative is , where

    These are compact smooth sources supported in and , respectively. The fixed difference-variable distribution , convolved against a compact smooth test times the fixed smooth field , gives a smooth function continuously in that test. On compact sets this follows directly from finite-order distribution estimates after differentiating the smooth test.

    Multiplication by or is continuous in the fixed smooth topologies. Thus both sources depend jointly continuously on , and the trace

    does so as well by the smooth Green-operator mapping property. After one metric direction, replace by . Later metric derivative traces vanish by quadratic degree. Scalar directions have no effect.

    These are all coefficient and trace coordinates required by , proving the assertion.

  • theoremTheorem: F9a for the completed new familiesGate T: fixed-support continuity and its boundary · IX-Free-2@1#thm:F9a · proof attached · lines 1728–1771
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    On

    the descended degree-four coefficient families

    are jointly continuous into . The corresponding degree-two families and scalar family retain their inherited F9a continuity. The zero new -families are continuous.

    Proof. For degree-four , the assertions are exactly the inherited two-edge test-family continuity.

    At degree-four , the terms

    are separately continuous trilinear maps of the fixed-support tests. This follows from inherited test-family continuity, Lemma lem:Tcontinuity, and separately continuous classical multiplication on the carrier. Lemma lem:Frechet makes each trilinear family jointly continuous. Their prescribed sums are therefore continuous.

    For , the family is separately continuous in the three tests by repeated classical multiplication. The same Fréchet multilinear argument gives joint continuity.

    The degree-two positive coefficients and the scalar family are inherited from IX-Free. Their order-zero families also follow from the same classical-product argument. Explicit zero coefficients require no estimate.

  • sectionGate T: fixed-support continuity and its boundaryGate T: fixed-support continuity and its boundary · lines 1771–1789
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    9b remains unclaimed. The theorem concerns compositions with named test presentations. It does not assert continuity of

    in actual-stage subspace topologies, nor corresponding actual-stage continuity on the degree-two blocks.

    Algebraic injectivity of does not give continuous inverse presentation maps. The algebraic projection in Lemma lem:anchored carries no topology claim. No quantum hypocontinuity on , or on all of , has been proved.

Final release and retained boundaries

  • theoremTheorem: IX-Free-2 releaseFinal release and retained boundaries · IX-Free-2@1#thm:release · proof attached · lines 1794–1835
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    Relative to Assumptions ass:carrier–ass:parent, the prescribed degree-four coefficients descend to actual functionals. All declared new coefficients glue with the locked first stages and the unchanged full old product on the named domain .

    For every fixed real common parent , the resulting truncated partial product satisfies C-I1–C-I9. Its two associations of agree through order , and it has partial-product reversal and actual-functional presentation independence. Moreover,

    Fixed-support test-family continuity holds on the named domains. Actual-stage continuity is not asserted.

    The release outcome is Constructed.

    Proof. Theorem thm:pinjective evaluates both degree-four relation kernels. Theorem thm:degree4 proves descent.

    Lemma lem:sharpcharge supplies the explicit sharp charge witness, while Proposition prop:zerocharge establishes the comparison zero-charge classes. Theorem thm:separation proves all required separations. Proposition prop:newdirect handles the entire new domain, including the locked first stages. Theorem thm:oldgluing handles its whole-sum old overlap. Corollary cor:cglue evaluates the gluing parameter set.

    Definition def:product gives one partial product, and Proposition prop:interfaces audits the copied contract. Theorem thm:coherence, Theorem thm:reversal, Proposition prop:presentation, and Theorem thm:F9a prove the remaining assertions.

  • sectionFinal release and retained boundariesFinal release and retained boundaries · lines 1835–1930
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    {}1.12

    Release alternativeOutcomeExact scope
    ConstructedAchievedPrescribed truncated product on , relative to the stated inherited premises
    Canonical prescription obstructedNot the outcomeThe prescribed candidate is constructed; no violating relation is exhibited
    Contract proved obstructedNot the outcomeNo universal no-go theorem is claimed
    Unresolved required gateNone in this releaseF9b and larger-domain constructions are outside the claim, not silently completed

    {}1.12

    ObjectFinal statusProof or boundary
    First stages and one-edge outputsConstructed, inheritedValues unchanged
    Three two-edge outputsConstructed, inheritedExistence and admission not reconstructed
    Constructed, inherited
    EvaluatedBoth zero
    Four degree-four coefficient mapsConstructedActual-functional descent
    Sharp charge witnessConstructedExplicit cone-local scalar test
    Live degree-two overlapEvaluatedZero
    Whole new-domain decompositionConstructedDirect sum, including first stages
    Whole-sum old overlapEvaluatedZero by the anchored-domain lemma
    Evaluated
    One declared partial productConstructed, modulo
    Both sharp associationsConstructedSelected word through
    Partial-product involutionConstructedDagger-stable declared domain
    Presentation independenceConstructedActual off-shell arguments; boundary terms retained
    F9a, new test familiesConstructedNamed fixed-support Fréchet domains
    F9bUnclaimedNo inverse topology estimates
    Associativity for unspecified triplesUnclaimedNo domain-closure theorem
    VII-C under (E1)–(E4)Retained boundaryNot reopened or repaired
    IX-D and G2ClosedNot begun
  • sectionRetained obstruction and enlargement boundariesFinal release and retained boundaries › Retained obstruction and enlargement boundaries · lines 1931–1950
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    The inherited VII-C obstruction under its original (E1)–(E4) hypotheses is retained. In particular, this paper does not establish normal-topology sequential admission continuity, unchanged sharp-approximant convergence, or hypocontinuous quantum multiplication with continuous coefficient extraction on a larger carrier.

    No old coefficient is repaired by subtracting . The calibrated family is not identified with a contact term. Admission of a generator does not admit an unspecified quadratic correction. No logarithm is removed by an observation-diagonal replacement.

    The constructed domain is not advertised as the complete free-product domain required by an unspecified IX-D construction. No causal-support theorem or G2 compatibility is obtained.

  • scopeWhat was actually missingFinal release and retained boundaries › Retained obstruction and enlargement boundaries · lines 1951–1961
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    was actually missing{ IX-Free had already supplied the two-edge outputs and their admission. The missing algebraic steps were actual-functional descent and simultaneous overlap agreement.

    Here the degree-four relation equation has only the zero presentation tensor. The live new-domain overlap vanishes by an explicit boundary-charge separation, and the entire new sum has zero old overlap. These facts, rather than another graph sum or another singular-product construction, release the selected word.}

Proof and verification audit

  • sectionPolarization and operator auditProof and verification audit › Polarization and operator audit · lines 1968–1988
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    The degree-four polynomial has one scalar slot and three metric slots. Full coefficient recovery therefore uses one scalar derivative and three metric derivatives, with the symmetric metric factor .

    In the slot-isolation calculation, setting leaves two surviving middle-slot permutations. This gives the exact factor in (eq:isolation); it does not change the inherited two-edge assignment factor.

    The identity

    uses compact support away from the initial surface and uniqueness of the zero-data Cauchy problem. It neither assumes that and are independent fields nor imposes an equation of motion on the configuration.

  • sectionCharge auditProof and verification audit › Charge audit · lines 1989–2004
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    The advanced-trace sign is determined by . With the source , this sign produces the positive integral in (eq:positivewitness).

    The complex witness is reduced to real smooth configurations by linear decomposition, not by an assumption that nonconvergence itself supplies a charge coordinate.

    For the old algebra, zero charge follows from its microcausal wavefront condition, admission, the injective boundary tensor , and the noncancellation of a delta coefficient by a lower-order Heaviside coefficient.

  • sectionAlgebraic and topological auditProof and verification audit › Algebraic and topological audit · lines 2005–2036
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    The new-domain proof is a direct-sum proof. The old-overlap proof applies to the entire new sum. Thus no untested intersection with an already glued sum remains.

    All tensor products and separating projections used in these arguments are algebraic. None identifies a presentation map with a quotient map or a topological isomorphism.

    The following implications are not asserted:

  • sectionVerification disclosureProof and verification audit › Verification disclosure · lines 2037–2054
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    The new proof calculations are the compact spatial-diagonal test for restricted sharp separation, degree-four slot isolation, the explicit advanced-trace witness, the microcausal zero-charge argument, and simultaneous algebraic gluing.

    Graph construction, graph admission, the degree-two presentation theorem, and the analytical triangle calibration are inherited as explicitly stated. The complete companion manuscripts are not independently reverified here.

    This source is intended for two-pass pdfLaTeX compilation. No successful compilation, page count, proof-assistant verification, or independent review is claimed.

Declarations

  • sectionDeclarationsDeclarations · lines 2055–2076
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    of the result. A relative construction of one explicitly declared truncated partial product and coherence for one ordered word.

    boundary. IX-Free is the supplied reference. Its reports of IX-A, IX-C, IX-B, and VII-D are used only through the explicit inherited premises in this manuscript.

    boundary. Fixed-support test-family continuity is proved. Actual-stage continuity and quantum hypocontinuity are unclaimed.

    and causal boundary. No global algebra, unrestricted associativity, causal realization, interacting construction, retarded or time-ordered map, IX-D construction, or G2 opening is asserted.

  • bibliographyReferencesDeclarations · lines 2077–2137
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    IXFree

    Landmark IX-Free: Actual-functional binary factorization of one sharp ordered word. Supplied source, IX-Free.tex. Used for the explicitly stated relation kernels, degree-two presentation injectivity, scalar descent, graph existence and admission, degree-two maps, reversal, and fixed-support continuity.

    IXC

    Landmark IX-C: Actual-functional factorization and coefficientwise coherence for one sharp ordered word. Companion reported in the supplied IX-Free source. Used through the copied first stages, one-edge values, interfaces, and preservation boundaries.

    IXA

    Landmark IX-A: An off-shell admission domain and boundary-sensitive topology for sharp Cauchy relational insertions. Companion reported in IX-Free. Used through the stated carrier, intrinsic charge, sharp adjoint, and classical closure premises.

    Calibration

    Landmark IX-B: Derivative-stable triangle calibration and counterterm constraints for sharp Cauchy insertions; and Finite part of the regulated Cauchy-reflection triangle. Companions reported in IX-Free. Used only through the inherited numerical parent-calibration premise, not independently reverified.

    VIIC

    Landmark VII-C: A mixed-Wick obstruction to a normal-topology boundary extension for sharp Cauchy harmonic insertions. Companion reported in IX-Free. Its original conditional obstruction boundary is retained.

    FR

    K. Fredenhagen and K. Rejzner. Perturbative algebraic quantum field theory. Lecture notes, arXiv:1208.1428v2, 2013. Section 4, especially the microcausal functional-derivative condition, and Appendix A on wavefront sets. https://arxiv.org/abs/1208.1428

    Ivrii

    V. Ivrii. Partial Differential Equations. Online textbook, Section 9.1: Wave equation in dimensions three and two. Kirchhoff and Duhamel formulas. https://www.math.toronto.edu/ivrii/PDE-textbook/Chapter9/S9.1.html