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Assumptions, dependency chain and source–readout contracts

Shadow Theory and the Wilson Yang–Mills Construction: A Source–Readout Reconstruction

Assumptions, dependency chain and source–readout contracts

Three registers collect what the reconstruction must preserve and how the conclusion depends on it. Table 3 lists the assumptions and scope controls of the supplied construction, with the lines of the supplied text at which each is stated; rows A19–A27 are those of the constructions of Sections 9, 14 and 16 and of the rotation and trace arguments. Table 4 is the chain of stages through which the public conclusion of Section 4 is reached, each with its input contract, the operations that are lifted, and the recovered output. Table 5 lists the source–readout contracts of the general transport statements, with what each readout fails to invert and what is therefore retained. Together with Table 2 they are the summary form of the hypotheses under which every recovery statement of this paper holds; none of them adds a hypothesis to the supplied construction.

Table 3: Assumptions and scope controls of the supplied construction, as preserved in this paper.

Assumption
Input lines
Preserved condition
Scope control
A01
Group and
representation
9
Closed faithful matrix subgroup
of U(m); specified exponential
real Lie algebra is nonabelian
simple.
No connectedness hypothesis
is added.
A02
Finite prior and
Wilson order
11–26
Independent normalized Haar
link prior and literal ordered
Wilson plaquette; insertion
support offsets depend only on
token.
Gauge invariance/continuity
and uniform-period slope
refer to one family.
A03
Volume and
mesh quantifiers
26–28
Every increasing period
sequence admits common
refinement; suitable fixed
periods have full inner mesh
limit before outer period limit.
Auxiliary compact selections
do not weaken full inner
limit.
A04
Field domain
and spectrum
30
Common dense invariant cyclic
word domain, Schwartz
continuity, adjoints/locality,
proper orthochronous
covariance and forward-cone
PVM.
Unique invariant vacuum is
not a positive-gap claim.
A05
OPE parameters
32–45
Fixed finite words/degrees,
M≥0, η>0, ε>0; separated
cluster and spectators; same
phase/truncation-independent
channels.
Radius threshold may
depend on fixed words/
parameters; uniformity is in
phases and stated
configurations.
A06
Public
comparison class
47–60
Centered degree-four trace and
finite complex combinations/
products of stated fixed
mass-shell integrals.
Does not enlarge exclusion
to every generalized-free
comparison; penalty is one.
A07
Analytic
conventions
64–108
Four dimensions; physical
metric/chord/color factors; odd
block ratios ≥3;
connected-union cover; absolute
weighted bounds.
Rate-zero is subpower, not
boundedness; thresholds
independent of period.
A08
Contact
continuation
12526–
12543
Tested rate inequality on every
allowed logarithmic path;
palette continuity and
constancy in assigned normals;
common detector collar.
Remaining branch retains
support t≤s, full finite
remainder; projected gain is
actual degree.
A09
Weak-sequence
Gaussian
comparison
12755–
12767
Same weak scaling sequence/
frames and compact distinct
configurations with each fixed
derivative order.
No interpolation to every
positive real scale; Ward
sign remains fixed.
A10
Private Gaussian
marks
12945–
12973
Finite regulated potential law,
positive semidefinite
infinite-lattice subtraction
matrix; independent private
marks by insertion.
Covariance is bilinear;
same-slot value need not
vanish at finite regulator; no
subtraction inverse required.
Source page 516.
Accessible table transcription
Table transcription, source page 516
AssumptionInput linesPreserved conditionScope control
A01Group and9Closed faithful matrix subgroupNo connectedness hypothesis
representationof U(m); specified exponentialis added.
real Lie algebra is nonabelian
simple.
A02Finite prior and11–26Independent normalized HaarGauge invariance/continuity
Wilson orderlink prior and literal orderedand uniform-period slope
Wilson plaquette; insertionrefer to one family.
support offsets depend only on
token.
A03Volume and26–28Every increasing periodAuxiliary compact selections
mesh quantifierssequence admits commondo not weaken full inner
refinement; suitable fixedlimit.
periods have full inner mesh
limit before outer period limit.
A04Field domain30Common dense invariant cyclicUnique invariant vacuum is
and spectrumword domain, Schwartznot a positive-gap claim.
continuity, adjoints/locality,
proper orthochronous
covariance and forward-cone
PVM.
A05OPE parameters32–45Fixed finite words/degrees,Radius threshold may
M≥0, η>0, ε>0; separateddepend on fixed words/
cluster and spectators; sameparameters; uniformity is in
phase/truncation-independentphases and stated
channels.configurations.
A06Public47–60Centered degree-four trace andDoes not enlarge exclusion
comparison classfinite complex combinations/to every generalized-free
products of stated fixedcomparison; penalty is one.
mass-shell integrals.
A07Analytic64–108Four dimensions; physicalRate-zero is subpower, not
conventionsmetric/chord/color factors; oddboundedness; thresholds
block ratios ≥3;independent of period.
connected-union cover; absolute
weighted bounds.
A08Contact12526–Tested rate inequality on everyRemaining branch retains
continuation12543allowed logarithmic path;support t≤s, full finite
palette continuity andremainder; projected gain is
constancy in assigned normals;actual degree.
common detector collar.
A09Weak-sequence12755–Same weak scaling sequence/No interpolation to every
Gaussian12767frames and compact distinctpositive real scale; Ward
comparisonconfigurations with each fixedsign remains fixed.
derivative order.
A10Private Gaussian12945–Finite regulated potential law,Covariance is bilinear;
marks12973positive semidefinitesame-slot value need not
infinite-lattice subtractionvanish at finite regulator; no
matrix; independent privatesubtraction inverse required.
marks by insertion.
Assumption
Input lines
Preserved condition
Scope control
A11
Laplace
continuity
14113–
14136
Positive future-cone measures
with finite transforms on full
open dual cone; common
polynomial budget for Schwartz
passage.
No arbitrary signed-measure
convergence assertion.
A12
Maxwell
isometry
countertest
14220–
14252
Complex-linear isometry with
physical image, vacuum/
translation intertwining, and
precise local coherent matrix
identity.
Neither surjectivity nor
identification of every field
required; fixed-ball variant
retained.
A13
Projected and
averaged
variants
14326–
14329
Bounded self-adjoint
fixed-image map for projected
variant; physical inner-product
preserving pointwise
fixed-image maps for
probability average.
Individual averaged maps
need no extra linearity,
boundedness or projection
property.
A14
Near-kernel
repair
14648–
14674
Finite real onto map with
nonzero one-dimensional kernel,
exact convergent right inverses
and both weighted near-kernel
errors.
No prior uniform
convergence on near-kernel
direction assumed; precision
paid before correction.
A15
Mass and
volume order
14890–
14982
Strictly positive mass through
volume estimates; moving
masses confined to a fixed
positive interval after tolerance
choice.
Separate eventual endpoint
estimates suffice; no uniform
mass convergence is inserted.
A16
Position
normalization
branch
Real fourth-order remainder
belongs to normalized frame;
weaker positive-ray norm
alignment transfers leading
coefficient only.
A17
Marker and
threshold order
15556–
15647
Finite surgery order fixed
before eventual thresholds;
common windows, two marker
slots and positive weights, exact
common Wilson partition.
15317–
15408
Complementary scalar/stress/
unit projections and positive
adjustment factors; independent
Wilson calibration of measured
charge.
Uniformity in finer cutoff/
volume follows retained
threshold order; no
chamber-count tarifffactor.
A18
Local lens
admissibility
15686–
15766
Fixed read support, measurable
equivariant displacement,
health threshold θ/4, chord D
with 8D≤θ, finite stocks and
nonwrapping.
Flag equality is branchwise
exact; absent insertion
requires no exponent
estimate or hard-mask
differentiation.
A19
Activity domains
and budgets
110–226
Threshold 0 < θ ≤1 with
equality healthy; ordered left
derivatives on healthy domains
only; budgets at a fixed finite
torus; early reserve s + 3.
Masks are never
differentiated; no
volume-independent bound
on the total scalar action is
asserted.
A20
Stationary
corridor
5515–5709
Fixed derivative order n ≥2;
counting gap and exponential
weights; contraction on
∥x∥< RX, ∥v∥≤RV .
Uniqueness of the stationary
point only inside the
corridor; off-shell values and
the residual are retained.
Source page 517.
Accessible table transcription
Table transcription, source page 517
AssumptionInput linesPreserved conditionScope control
A11Laplace14113–Positive future-cone measuresNo arbitrary signed-measure
continuity14136with finite transforms on fullconvergence assertion.
open dual cone; common
polynomial budget for Schwartz
passage.
A12Maxwell14220–Complex-linear isometry withNeither surjectivity nor
isometry14252physical image, vacuum/identification of every field
countertesttranslation intertwining, andrequired; fixed-ball variant
precise local coherent matrixretained.
identity.
A13Projected and14326–Bounded self-adjointIndividual averaged maps
averaged14329fixed-image map for projectedneed no extra linearity,
variantsvariant; physical inner-productboundedness or projection
preserving pointwiseproperty.
fixed-image maps for
probability average.
A14Near-kernel14648–Finite real onto map withNo prior uniform
repair14674nonzero one-dimensional kernel,convergence on near-kernel
exact convergent right inversesdirection assumed; precision
and both weighted near-kernelpaid before correction.
errors.
A15Mass and14890–Strictly positive mass throughSeparate eventual endpoint
volume order14982volume estimates; movingestimates suffice; no uniform
masses confined to a fixedmass convergence is inserted.
positive interval after tolerance
choice.
A16Position15317–Complementary scalar/stress/Real fourth-order remainder
normalization15408unit projections and positivebelongs to normalized frame;
branchadjustment factors; independentweaker positive-ray norm
Wilson calibration of measuredalignment transfers leading
charge.coefficient only.
A17Marker and15556–Finite surgery order fixedUniformity in finer cutoff/
threshold order15647before eventual thresholds;volume follows retained
common windows, two markerthreshold order; no
slots and positive weights, exactchamber-count tarifffactor.
common Wilson partition.
A18Local lens15686–Fixed read support, measurableFlag equality is branchwise
admissibility15766equivariant displacement,exact; absent insertion
health threshold θ/4, chord Drequires no exponent
with 8D≤θ, finite stocks andestimate or hard-mask
nonwrapping.differentiation.
A19Activity domains110–226Threshold 0 < θ ≤1 withMasks are never
and budgetsequality healthy; ordered leftdifferentiated; no
derivatives on healthy domainsvolume-independent bound
only; budgets at a fixed finiteon the total scalar action is
torus; early reserve s + 3.asserted.
A20Stationary5515–5709Fixed derivative order n ≥2;Uniqueness of the stationary
corridorcounting gap and exponentialpoint only inside the
weights; contraction oncorridor; off-shell values and
∥x∥< RX, ∥v∥≤RV .the residual are retained.
Assumption
Input lines
Preserved condition
Scope control
A21
Calendar and
order of choices
6226–6430
Stage data and length floors,
then lengths, then entry delays;
one calendar chosen before
every history, cutoff, period and
observable.
Later enlargements are
monotone and preserve
earlier payments; estimates
on different calendars are
not combined.
A22
Calibration of
finite histories
6617–6819,
7504–7575
Bare parameter in a closed
interval; bottom coupling  ̄β at
level zero; deterministic forward
recipe with continuous
admissible levels.
Existence by the
intermediate value theorem
only; uniqueness within the
retained recipe; no inverse
shooting map is assumed.
A23
Reference tori
and beacons
6843–7259
Read radius r with 2r ≤w; five
folded reference views; compact
coupling band; orders and stage
parameters, then block length,
then delay.
Constants are tied to fixed
reference tori and are not
uniform in the physical
period.
A24
Labels and
calibrated
readers
8399–8753
Simple color Lie algebra, with
no connectedness of the group;
finite slot family; degree and
level fixed before the eventual
threshold.
The label reader is inverted
at each fixed level; its
inverse bound is not uniform
in the level.
A25
Free comparison
hierarchy
8754–9247
Explicit Gaussian kernel on the
fixed real symbol space; one
exterior degree bound for all
weights in detection.
Statements are exact in the
free comparison theory; they
pass to the interacting
hierarchy only by rank
transfer along convergent
readings.
A26
Euclidean
rotations
10373–
10674
Bands, window and tolerance
fixed before the limit removing
the outer flux; three response
signs f ≥0, g ≤0, h ≥0;
contact subtraction.
No positivity is claimed for
the six individual band
readings; the unsubtracted
stress pair is not asserted
conserved at coincident
points.
A27
Scaling
comparison and
trace limit
13237–
13994
Selected radii rk ↓0 and scaling
maps; for every sequence sn ↓0
a subsequence with a scaling
family on the same table and
phase; monotonicity from the
positive-time spectral measure.
No uniformity in the degree
and no bound on the scaling
maps or their inverses; the
interacting theory is not
asserted to be free.
Source page 518.
Accessible table transcription
Table transcription, source page 518
AssumptionInput linesPreserved conditionScope control
A21Calendar and6226–6430Stage data and length floors,Later enlargements are
order of choicesthen lengths, then entry delays;monotone and preserve
one calendar chosen beforeearlier payments; estimates
every history, cutoff, period andon different calendars are
observable.not combined.
A22Calibration of6617–6819,Bare parameter in a closedExistence by the
finite histories7504–7575interval; bottom coupling ̄β atintermediate value theorem
level zero; deterministic forwardonly; uniqueness within the
recipe with continuousretained recipe; no inverse
admissible levels.shooting map is assumed.
A23Reference tori6843–7259Read radius r with 2r ≤w; fiveConstants are tied to fixed
and beaconsfolded reference views; compactreference tori and are not
coupling band; orders and stageuniform in the physical
parameters, then block length,period.
then delay.
A24Labels and8399–8753Simple color Lie algebra, withThe label reader is inverted
calibratedno connectedness of the group;at each fixed level; its
readersfinite slot family; degree andinverse bound is not uniform
level fixed before the eventualin the level.
threshold.
A25Free comparison8754–9247Explicit Gaussian kernel on theStatements are exact in the
hierarchyfixed real symbol space; onefree comparison theory; they
exterior degree bound for allpass to the interacting
weights in detection.hierarchy only by rank
transfer along convergent
readings.
A26Euclidean10373–Bands, window and toleranceNo positivity is claimed for
rotations10674fixed before the limit removingthe six individual band
the outer flux; three responsereadings; the unsubtracted
signs f ≥0, g ≤0, h ≥0;stress pair is not asserted
contact subtraction.conserved at coincident
points.
A27Scaling13237–Selected radii r0 and scalingNo uniformity in the degree
k ↓
comparison and13994maps; for every sequence s0and no bound on the scaling
n ↓
trace limita subsequence with a scalingmaps or their inverses; the
family on the same table andinteracting theory is not
phase; monotonicity from theasserted to be free.
positive-time spectral measure.

Table 4: Dependency chain of the supplied conclusion: each stage with its input contract, the operations lifted, and its recovered output.

Stage (parents)
Input contract
Operation
Recovered output
D01
Finite Wilson
realization
fixed group/
representation, finite
lattice, normalized Haar
frame realization and
section; Wilson density
pushforward
physical
finite-lattice law
D02
Multiscale
calibrated family
(D01)
positive widths,
prescribed stage ordering,
banked histories
exact one-step identities
and common
insertion-token transport
one Wilson family
before volume
subsequence
Source page 518.
Accessible table transcription
Table transcription, source page 518
Stage (parents)Input contractOperationRecovered output
D01Finite Wilsonfixed group/frame realization andphysical
realizationrepresentation, finitesection; Wilson densityfinite-lattice law
lattice, normalized Haarpushforward
D02Multiscalepositive widths,exact one-step identitiesone Wilson family
calibrated familyprescribed stage ordering,and commonbefore volume
(D01)banked historiesinsertion-token transportsubsequence
Stage (parents)
Input contract
Operation
Recovered output
D03
Common
continuum table
(D02)
requested increasing
period sequence;
fixed-period Cauchy
bounds
full mesh limit then outer
refined-period limit
common hierarchy,
coefficients and
finite field filtration
D04
Phases and
Hilbert
reconstruction
(D03)
common-domain
fields, cone
momentum measure
and unique vacuum
D05
Fixed OPE and
contact extension
(D03, D04)
compression algebra,
character hierarchy,
positive Gram/heat data
phase readout and same
heat/tube/boundary
construction
same finite homogeneous
reader, basis and
projections
nested replacement,
tested integration and
combined contact
resolution
same public
channels across
finite truncations/
collisions
D06
Gaussian
comparison (D03)
same weak sequence, free
frames and moving
covariance limits
private marks, corrected
covariance, Wick
recursion and profile
sums
mean Gaussian
comparison with
mixed stress jets
D07
Local equation
sensor (D02, D03)
same served coefficient
difference, chart/coupling
and retained scale
finite marker estimates
and weighted degree-four
spectator detection
both paid
near-kernel leaks
D08
Physical stress
amplitude (D06,
D07)
Ward-normalized
stress and scalar
coefficient −b0/2
D09
Selected trace
ultraviolet
measure (D04,
D08)
exact divergence detector;
same nonzero Ward shell
test
finite correction inverse
and near-kernel
functional repair
selected stress, exact unit
centering, positive
spectral measure
all-distance sandwich;
dilation/Laplace/
Schwartz recovery
trace amplitude and
normalized cone
measure
D10
Specified finite
polynomial
exclusion (D09)
finite mass-shell tracks
with fixed finite data
damped radial expansions
and product-test recovery
source-specified
comparison
exclusion
D11
Specified Maxwell
countertests
(D09)
physical-image
translation isometry and
precise local coherent
identity
common amplitudes;
local dilation polynomial;
finite sector growth
source-specified
Maxwell/projected/
averaged exclusions
D12
Normalized
position
diagnostic (D08,
D09)
positive frame branch;
separated Ward columns
measured
Wilson-calibrated charge
and exact rational
residual
normalized-frame
real fourth-order
remainder; weaker
leading transfer
Source page 519.
Accessible table transcription
Table transcription, source page 519
Stage (parents)Input contractOperationRecovered output
D03Commonrequested increasingfull mesh limit then outercommon hierarchy,
continuum tableperiod sequence;refined-period limitcoefficients and
(D02)fixed-period Cauchyfinite field filtration
bounds
D04Phases andcompression algebra,phase readout and samecommon-domain
Hilbertcharacter hierarchy,heat/tube/boundaryfields, cone
reconstructionpositive Gram/heat dataconstructionmomentum measure
(D03)and unique vacuum
D05Fixed OPE andsame finite homogeneousnested replacement,same public
contact extensionreader, basis andtested integration andchannels across
(D03, D04)projectionscombined contactfinite truncations/
resolutioncollisions
D06Gaussiansame weak sequence, freeprivate marks, correctedmean Gaussian
comparison (D03)frames and movingcovariance, Wickcomparison with
covariance limitsrecursion and profilemixed stress jets
sums
D07Local equationsame served coefficientfinite marker estimatesboth paid
sensor (D02, D03)difference, chart/couplingand weighted degree-fournear-kernel leaks
and retained scalespectator detection
D08Physical stressexact divergence detector;finite correction inverseWard-normalized
amplitude (D06,same nonzero Ward shelland near-kernelstress and scalar
D07)testfunctional repaircoefficient −b/2
0
D09Selected traceselected stress, exact unitall-distance sandwich;trace amplitude and
ultravioletcentering, positivedilation/Laplace/normalized cone
measure (D04,spectral measureSchwartz recoverymeasure
D08)
D10Specified finitefinite mass-shell tracksdamped radial expansionssource-specified
polynomialwith fixed finite dataand product-test recoverycomparison
exclusion (D09)exclusion
D11Specified Maxwellphysical-imagecommon amplitudes;source-specified
counterteststranslation isometry andlocal dilation polynomial;Maxwell/projected/
(D09)precise local coherentfinite sector growthaveraged exclusions
identity
D12Normalizedpositive frame branch;measurednormalized-frame
positionseparated Ward columnsWilson-calibrated chargereal fourth-order
diagnostic (D08,and exact rationalremainder; weaker
D09)residualleading transfer

Table 5: Source–readout contracts of the general transport statements.

Contract
Readout
Non-invertibility and
retained data
Where
M01
Native admission
and literal
preparation
The realized branch supplies
physical configuration/history
readouts only after group,
lattice, law and analytic data
are specified.
Does not recover or
classify all possible native
antecedents; admission
does not select Wilson law
or identify abstract
vertices with physical
sites.
Prop. 6.1
Source page 519.
Accessible table transcription
Table transcription, source page 519
ContractReadoutNon-invertibility andWhere
retained data
M01Native admissionThe realized branch suppliesDoes not recover orProp. 6.1
and literalphysical configuration/historyclassify all possible native
preparationreadouts only after group,antecedents; admission
lattice, law and analytic datadoes not select Wilson law
are specified.or identify abstract
vertices with physical
sites.
Contract
Readout
Non-invertibility and
retained data
Where
M02
Finite frame fibre
and section
π(r, A)e = r−1
x Aery; reverse
links are inverses.
Readout forgets frame
representatives; it does not
quotient physical gauge
equivalence. Physical
gauge acts by r 7→rg−1, A
fixed.
Thm. 7.1
M03
Paths and physical
gauge action
Interior frames cancel; open
paths transform at endpoints
and loop traces read
unchanged.
A trace alone discards
conjugacy and other
matrix information; full
link history remains
retained.
§7
M04
Normalized Wilson
measure and
insertions
π∗eμ = μW ; insertion F reads
F ◦π.
No unnormalized gauge
volume; normalization and
integrability remain part
of the contract.
Thm. 7.2
M05
Tangent operators
and quadratic forms
p2TZ = Tp1 and TZj1 = j2T;
compositions insert piji = I.
Vertical frame directions
remain null. Operator
transport differs from
adjoint form pullback. No
ambient vertical coercivity
follows.
Thm. A.1
M06
Actual nonlinear
predictors and
horizontal
derivatives
Coarse π(s, B) = P(π(r, A));
differentiated frame terms
cancel in the coarse readout.
Multivalued branches
remain tagged relations;
no invented selection or
bound on arbitrary
unbounded frame rates.
§A
M07
Tested limits and
quantitative
estimates
Exact scalar identity IZ
λ = Iλ
at every tag.
No exchange of limits,
stronger test class,
derivative of hard masks,
new compactness or
mixing of unrelated
partition functions.
Thm. B.1
M08
Operations,
relations and
residual histories
πσ = id at every composable
intermediate stage.
No discard of branch tags
or auxiliary histories
merely because functions
coincide.
§B
M09
Reflection quotient,
fields and spectrum
Unitary U : [v] 7→[pv] between
completed reflection spaces.
Null histories are
quotiented; an unbounded
field is not promoted to a
bounded whole-space
operator. Rank-one
vacuum is not a positive
spectral gap.
Thm. C.1
M10
Compression
algebra and phase
measure
Whole-word character
evaluation; ρZ = h∗ρ.
Factors cannot be read
separately without a
proved product identity.
Almost-everywhere
statements require the
original continuity/
full-support upgrade.
Thm. D.1
Source page 520.
Accessible table transcription
Table transcription, source page 520
ContractReadoutNon-invertibility andWhere
retained data
−1
M02Finite frame fibreπ(r, A)e = rx Aery; reverseReadout forgets frameThm. 7.1
and sectionlinks are inverses.representatives; it does not
quotient physical gauge
equivalence. Physical
−1
gauge acts by r 7→rg, A
fixed.
M03Paths and physicalInterior frames cancel; openA trace alone discards§7
gauge actionpaths transform at endpointsconjugacy and other
and loop traces readmatrix information; full
unchanged.link history remains
retained.
M04Normalized Wilsonπeμ = μNo unnormalized gaugeThm. 7.2
∗W ; insertion F reads
measure andF ◦π.volume; normalization and
insertionsintegrability remain part
of the contract.
M05Tangent operatorspT Tp Tj jT;Vertical frame directionsThm. A.1
2Z =1 andZ1 =2
and quadratic formscompositions insert pj I.remain null. Operator
ii =
transport differs from
adjoint form pullback. No
ambient vertical coercivity
follows.
M06Actual nonlinearCoarse π(s, B) = P(π(r, A));Multivalued branches§A
predictors anddifferentiated frame termsremain tagged relations;
horizontalcancel in the coarse readout.no invented selection or
derivativesbound on arbitrary
unbounded frame rates.
Z
M07Tested limits andExact scalar identity I= INo exchange of limits,Thm. B.1
λ λ
quantitativeat every tag.stronger test class,
estimatesderivative of hard masks,
new compactness or
mixing of unrelated
partition functions.
M08Operations,πσ = id at every composableNo discard of branch tags§B
relations andintermediate stage.or auxiliary histories
residual historiesmerely because functions
coincide.
M09Reflection quotient,Unitary U : [v] 7→[pv] betweenNull histories areThm. C.1
fields and spectrumcompleted reflection spaces.quotiented; an unbounded
field is not promoted to a
bounded whole-space
operator. Rank-one
vacuum is not a positive
spectral gap.
M10CompressionWhole-word characterFactors cannot be readThm. D.1
algebra and phaseevaluation; ρZ = h∗ρ.separately without a
measureproved product identity.
Almost-everywhere
statements require the
original continuity/
full-support upgrade.
Contract
Readout
Non-invertibility and
retained data
Where
M11
Fixed OPE reader
and retained
remainder
Applying q recovers the same
channel reader and finite
projections.
Projection Πm is not
inverted; discarded tails
are retained as residuals.
Label inverse is not an
inverse on unreduced
histories.
Prop. E.1
M12
Contact extensions
with subtraction
data
TZ(g) = T(Lg) on the stated
combined integrability domain.
Punctured restriction loses
diagonal-supported
contact information;
separately nonsummable
pieces are not assigned
integrals.
§E
M13
Gaussian means,
covariances and
residuals
Normalized Gaussian integrals
and μ −v = E∗v −P ∗(Av + b),
E = AP −I, A = A∗.
Replacing μ by −Cb loses
the specified mean identity.
No probability covariance
is assigned to
nonsymmetric P.
§F
M14
Ordered inverse,
determinant and
quiet-coordinate
data
C−1 −A = P
k≥1(−S)kA on
the original norm-convergence
domain.
Terminal A cannot be
removed/commuted;
determinant diagnostic
alone is not full log
determinant. Orthogonal
norm invariance does not
preserve coordinate boxes.
§F
Source page 521.
Accessible table transcription
Table transcription, source page 521
ContractReadoutNon-invertibility andWhere
retained data
M11Fixed OPE readerApplying q recovers the sameProjection Πm is notProp. E.1
and retainedchannel reader and finiteinverted; discarded tails
remainderprojections.are retained as residuals.
Label inverse is not an
inverse on unreduced
histories.
M12Contact extensionsT(g) = T(Lg) on the statedPunctured restriction loses§E
Z
with subtractioncombined integrability domain.diagonal-supported
datacontact information;
separately nonsummable
pieces are not assigned
integrals.
M13Gaussian means,Normalized Gaussian integralsReplacing μ by −Cb loses§F
∗∗
covariances andand μ −v = Ev −P (Av + b),the specified mean identity.
∗
residualsE = AP −I, A = A.No probability covariance
is assigned to
nonsymmetric P.
P
−1 k
M14Ordered inverse,C−A = (−S)A onTerminal A cannot be§F
k≥1
determinant andthe original norm-convergenceremoved/commuted;
quiet-coordinatedomain.determinant diagnostic
dataalone is not full log
determinant. Orthogonal
norm invariance does not
preserve coordinate boxes.

Source: Shadow Theory and the Wilson Yang–Mills Construction: A Source–Readout Reconstruction. Both papers belong to one Zenodo record. No external funding.