TFPT scientific source excerpt Original repository path: experiments/theory-contracts/elliptic-moebius-source-bridge-20261026/MARKED-Q-DIVISOR-CENTRAL-TWIST.txt Original file SHA-256: da1f75831a46a0c0662f931486b77e6e2085126df452b009d1a90351d413d904 Inclusive original lines: 181-340 Line numbers below refer to the original source. This bounded excerpt is source evidence; it is not a new proof/checker run. Conversation metadata and personal execution details are omitted where indicated. 000181 | Norm_Dq(P)=mathcal P_delta_q, 000182 | delta_q=D_q-3q_0=q_1-q_2 not_equal 0 in Jac(C)[2]. (14) 000183 | 000184 | The original c moves this nonzero vector through the three nonzero elements 000185 | of V_q. Thus the q_0-normalized one-copy line is not c invariant. This is 000186 | an obstruction to that point normalization, not an intrinsic obstruction to 000187 | the source family: using q_0 as the Poincare rigidification was an additional 000188 | choice, even though q_0 itself was already source marked. 000189 | 000190 | The source has already selected a reference of the correct type, namely the 000191 | degree-one spin line S_0. From (3) and S_0^2=K_C, 000192 | 000193 | O_C(D_q)=S_0 tensor K_C=S_0^3. (15) 000194 | 000195 | Let 000196 | 000197 | mathcal R=
000198 |
000199 | be the Deligne pairing over A, and define the spin-normalized Poincare family
000200 |
000201 | P_spin=P tensor pr_A^*(mathcal R^(-1)). (16)
000202 |
000203 | This tensor factor comes from the base, so P_spin represents the same family
000204 | of degree-zero line bundles on C. Since deg(S_0)=1, bilinearity first gives
000205 |
000206 | tensor mathcal R^(-1)=O_A.
000207 |
000208 | Norm functoriality and bilinearity of the Deligne pairing then give a
000209 | canonical cancellation:
000210 |
000211 | Norm_Dq(P_spin)
000212 | = tensor mathcal R^(-3)
000213 | = tensor ^(-3)
000214 | =O_A. (17)
000215 |
000216 | Consequently the evaluation norm of
000217 |
000218 | E_spin=S_0 tensor P_spin
000219 |
000220 | is the constant equivariant line
000221 |
000222 | mathcal N_q(E_spin)=N_q(S_0) tensor O_A. (18)
000223 |
000224 | The same statement holds for D_p because O(D_p)=O(D_q)=S_0^3. Thus the
000225 | q and p blocks remain a full-family s-exchanged pair with the conjugate
000226 | central characters computed in section 3.
000227 |
000228 | This normalization does not change the ordinary theta determinant. A line
000229 | pulled back from A enters determinant of cohomology with exponent
000230 | chi(S_0 tensor L)=0, so the factor mathcal R^(-1) has weight zero there.
000231 | It changes the length-three evaluation norm with exponent three, exactly as
000232 | needed in (17).
000233 |
000234 | The construction is c and Q covariant because S_0 and D_q were already
000235 | selected invariant objects, and the S_0-normalized universal family is unique
000236 | up to its fixed rigidification. The remaining scalar ambiguity in a lift of
000237 | S_0 does not reintroduce a phase: scaling the second entry of the Deligne
000238 | pairing acts with exponent deg(P_spin|C)=0. Therefore (17) is independent of
000239 | that scalar and obeys the same cocycles as the selected source lifts.
000240 |
000241 | The direct one-copy family correction is hence genuinely
000242 |
000243 | O(2 Theta) tensor N_q(S_0)^(-1), (19)
000244 |
000245 | with no moving Pic^0 factor. It retains the four-dimensional theta space,
000246 | the original c action, and the central relations (2). No new point or flat
000247 | character has been selected; the normalization uses the unique
000248 | c-invariant source spin line S_0.
000249 |
000250 | One distinction remains. If one first imposes vanishing at D_q via (5) and
000251 | then forms the usual two-theta line, the evaluation factor is squared:
000252 |
000253 | (D tensor mathcal N_q(E_spin)^(-1))^(-2)
000254 | =D^(-2) tensor N_q(S_0)^2. (20)
000255 |
000256 | Its beta phase is (-i)^2=-1, not +i. Thus determinant exactness alone does
000257 | not select the one-copy insertion (19). The remaining physical question is
000258 | precise: does the original puncture, boundary, sewing or conformal-block
000259 | construction attach one inverse copy of the marked evaluation norm directly
000260 | to the O(2 Theta) module? The geometry supplies that line canonically, but
000261 | the inspected source has not yet supplied this insertion rule.
000262 |
000263 |
000264 | 5. SOURCE AUDIT AND EXACT REMAINING GAP
000265 |
000266 | The September synthesis already contains every geometric input used above:
000267 |
000268 | * its section 004, lines 276--312, gives C, Q, c, s and the marked q and p
000269 | triples;
000270 | * lines 314--326 warn that the six-point transport is not yet a field
000271 | intertwiner;
000272 | * lines 378--379 require the original test-function space and
000273 | Riemann--Hilbert kernel for an actual quantization statement.
000274 |
000275 | Its following section 005, lines 1--13, gives the different determinant
000276 |
000277 | det Psi(z)=1-z^4
000278 |
000279 | and its primitive winding, while explicitly leaving the contour and boundary
000280 | operator map open. That Fuchs fundamental-matrix determinant is not the
000281 | finite evaluation determinant (4), so it does not already insert N_q^(-1)
000282 | into the source state space.
000283 |
000284 | The targeted Atlas source v519 carries exact CAR reflection and spin phases,
000285 | but on a different freely chosen sixteen-Majorana Fock object. It supplies
000286 | no functor from (C,S_0,D_q) to (1) and cannot be reused as that missing map.
000287 | The inspected Atlas anchors are paper-source:c3a096bf0487b5234a147dce for
000288 | the September determinant/winding passage, and v519 sources
000289 | source:588e55951801405a5c25 and source:bd323276b179791d1d6c for the separate
000290 | CAR object.
000291 | No explicit q-divisor determinant twist was found in the bounded original
000292 | source search. This is a statement about the inspected source family, not
000293 | an assertion that every archived paper has been exhausted.
000294 |
000295 | The sharp result is therefore:
000296 |
000297 | * MATHEMATICALLY PROVED: N_q(S_0)^(-1) is a canonical line constructed from
000298 | existing marked source data and restores exactly the +i central
000299 | character without changing c;
000300 | * MATHEMATICALLY PROVED: its s partner has the conjugate -i character;
000301 | * MATHEMATICALLY PROVED: q_0 normalization creates the moving flat class
000302 | delta_q=q_1-q_2, while the source-selected S_0 normalization cancels it
000303 | canonically and leaves the ordinary theta determinant unchanged;
000304 | * CANDIDATE BRIDGE: the actual field/theta construction uses the one-copy
000305 | line (19), rather than the different boundary-first-then-square operation
000306 | (20);
000307 | * STILL OPEN: the original Calderon, Riemann--Hilbert, sewing or conformal-
000308 | block construction selects this boundary factor and identifies the
000309 | resulting four-dimensional linear module with the native one.
000310 |
000311 |
000312 | MATHEMATICAL REFERENCES
000313 |
000314 | * The Stacks Project, Tag 0FJ9, determinant of finite locally free modules:
000315 | https://stacks.math.columbia.edu/tag/0FJ9
000316 |
000317 | * The Stacks Project, Tag 0FJW, determinant functor for perfect complexes
000318 | and exact/pullback functoriality:
000319 | https://stacks.math.columbia.edu/tag/0FJW
000320 |
000321 | * The Stacks Project, Tag 0BD2, canonical norm for a finite locally free
000322 | morphism and base-change compatibility:
000323 | https://stacks.math.columbia.edu/tag/0BD2
000324 |
000325 | * Pierre Deligne, Le determinant de la cohomologie, Contemporary
000326 | Mathematics 67 (1987), 93--177, for determinant and Deligne-pairing
000327 | functoriality:
000328 | https://publications.ias.edu/book/export/html/404
000329 |
000330 |
000331 | LOCAL SOURCE ANCHORS
000332 |
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