File size: 46,854 Bytes
db6c8f1 | 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60 61 62 63 64 65 66 67 68 69 70 71 72 73 74 75 76 77 78 79 80 81 82 83 84 85 86 87 88 89 90 91 92 93 94 95 96 97 98 99 100 101 102 103 104 105 106 107 108 109 110 111 112 113 114 115 116 117 118 119 120 121 122 123 124 125 126 127 128 129 130 131 132 133 134 135 136 137 138 139 140 141 142 143 144 145 146 147 148 149 150 151 152 153 154 155 156 157 158 159 160 161 162 163 164 165 166 167 168 169 170 171 172 173 174 175 176 177 178 179 180 181 182 183 184 185 186 187 188 189 190 191 192 193 194 195 196 197 198 199 200 201 202 203 204 205 206 207 208 209 210 211 212 213 214 215 216 217 218 219 220 221 222 223 224 225 226 227 228 229 230 231 232 233 234 235 236 237 238 239 240 241 242 243 244 245 246 247 248 249 250 251 252 253 254 255 256 257 258 259 260 261 262 263 264 265 266 267 268 269 270 271 272 273 274 275 276 277 278 279 280 281 282 283 284 285 286 287 288 289 290 291 292 293 294 295 296 297 298 299 300 301 302 303 304 305 306 307 308 309 310 311 312 313 314 315 316 317 318 319 320 321 322 323 324 325 326 327 328 329 330 331 332 333 334 335 336 337 338 339 340 341 342 343 344 345 346 347 348 349 350 351 352 353 354 355 356 357 358 359 360 361 362 363 364 365 366 367 368 369 370 371 372 373 374 375 376 377 378 379 380 381 382 383 384 385 386 387 388 389 390 391 392 393 394 395 396 397 398 399 400 401 402 403 404 405 406 407 408 409 410 411 412 413 414 415 416 417 418 419 420 421 422 423 424 425 426 427 428 429 430 431 432 433 434 435 436 437 438 439 440 441 442 443 444 445 446 447 448 449 450 451 452 453 454 455 456 457 458 459 460 461 462 463 464 465 466 467 468 469 470 471 472 473 474 475 476 477 478 479 480 481 482 483 484 485 486 487 488 489 490 491 492 493 494 495 496 497 498 499 500 501 502 503 504 505 506 507 508 509 510 511 512 513 514 515 516 517 518 519 520 521 522 523 524 525 526 527 528 529 530 531 532 533 534 535 536 537 538 539 540 541 542 543 544 545 546 547 548 549 550 551 552 553 554 555 556 557 558 559 560 561 562 563 564 565 566 567 568 569 570 571 572 573 574 575 576 577 578 579 580 581 582 583 584 585 586 587 588 589 590 591 592 593 594 595 596 597 598 599 600 601 602 603 604 605 606 607 608 609 610 611 612 613 614 615 616 617 618 619 620 621 622 623 624 625 626 627 628 629 630 631 632 633 634 635 636 637 638 639 640 641 642 643 644 645 646 647 648 649 650 651 652 653 654 655 656 657 658 659 660 661 662 663 664 665 666 667 668 669 670 671 672 673 674 675 676 677 678 679 680 681 682 683 684 685 686 687 688 689 690 691 692 693 694 695 696 697 698 699 700 701 702 703 704 705 706 707 708 709 710 711 712 713 714 715 716 717 718 719 720 721 722 723 724 725 726 727 728 729 730 731 732 733 734 735 736 737 738 739 740 741 742 | {
"count": 49,
"results": [
{
"arxiv_ids": [
"2404.02146"
],
"claim": "The proposed super-Poynting criterion vanishes exactly when the Cotton-York and stress tensors commute; the commutator norm is a Cotton-eigenvalue-gap-weighted sum of stress-frame misalignments.",
"classification": "criterion theorem and spectral identity",
"discovery": "Spectral no-radiation criterion",
"exact_check_count": 11,
"index": 1,
"kernel": "run_sabrina_ads_radiation_spectral_commutator",
"scientific_payload_sha256": "241d637afce046d817e7a3107063956a87e7581ccc4ccb9230959c16a846ff1d",
"source_classification": "complete",
"summary": "The proposed super-Poynting criterion vanishes exactly when the Cotton-York and stress tensors commute; the commutator norm is a Cotton-eigenvalue-gap-weighted sum of stress-frame misalignments.",
"title": "Radiation in Holography"
},
{
"arxiv_ids": [
"2411.10527"
],
"claim": "The nonempty scattering region is exactly pi/2 <= mu <= arccos(-1/3) with tau_*(mu) <= tau <= pi-mu, including the collapsed endpoint and linear and quadratic onset laws.",
"classification": "exact feasibility-domain theorem",
"discovery": "Exact two-interval scattering domain",
"exact_check_count": 18,
"index": 2,
"kernel": "run_sabrina_ads_two_interval_scattering_feasibility",
"scientific_payload_sha256": "da08f86ea668e62889d14682aff488ad090f0b3c49d6ffc823e456f799cd580b",
"source_classification": "complete",
"summary": "The nonempty scattering region is exactly pi/2 <= mu <= arccos(-1/3) with tau_*(mu) <= tau <= pi-mu, including the collapsed endpoint and linear and quadratic onset laws.",
"title": "Cryptographic tests of the python's lunch conjecture"
},
{
"arxiv_ids": [
"1502.07644"
],
"claim": "For every d=2m+2 with integer m>=2, every m-dependent factor cancels between the soft charge, Green function, and hard action, leaving the same normalized Ward identity.",
"classification": "all-dimension theorem extension",
"discovery": "All-even-dimensional Ward normalization",
"exact_check_count": 11,
"index": 3,
"kernel": "run_sabrina_all_even_d_ward_normalization",
"scientific_payload_sha256": "36d368057821e69206d459c5b4f34e81d6d3b1df977de35db7a7bd523f3b529e",
"source_classification": "all_even_d_soft_hard_ward_normalization_exact_and_m_independent",
"summary": "For every d=2m+2 with integer m>=2, every m-dependent factor cancels between the soft charge, Green function, and hard action, leaving the same normalized Ward identity.",
"title": "Higher-Dimensional Supertranslations and Weinberg's Soft Graviton Theorem"
},
{
"arxiv_ids": [
"2211.14287",
"2307.16801",
"2607.28718"
],
"claim": "For every integer m>=3, the minimal inverse-total-Z depth is exactly d_min(m)=m-3; distribution order r has exact total-Z multiplicity r+2 through r=m-1, and all orders r>=m vanish.",
"classification": "all-m theorem from finite ladder to exact closure",
"discovery": "All-m transverse-nonlocality saturation theorem",
"exact_check_count": 12,
"index": 4,
"kernel": "run_sabrina_all_m_transverse_nonlocality_chain",
"scientific_payload_sha256": "6600de93b5e0dbb7dc6744cfc31499e4d84760267f62e18bc2a1c9a0e8470db5",
"source_classification": "all_m_transverse_nonlocality_depth_saturation_and_distribution_order_multiplicity_exact",
"summary": "For every integer m>=3, the minimal inverse-total-Z depth is exactly d_min(m)=m-3; distribution order r has exact total-Z multiplicity r+2 through r=m-1, and all orders r>=m vanish.",
"title": "All M Transverse Nonlocality Chain"
},
{
"arxiv_ids": [
"2212.00962"
],
"claim": "The symmetric and antisymmetric celestial prefactors alternate zeros and finite values at positive integers, while complementary simple poles and zeros occur at nonpositive integers, with exact residues at Delta=0 and 1.",
"classification": "analytic zero-and-pole classification",
"discovery": "Ambidextrous prefactor singularity lattice",
"exact_check_count": 11,
"index": 5,
"kernel": "run_sabrina_ambidextrous_integer_prefactor_lattice",
"scientific_payload_sha256": "77e01bb41ab0dd463176786be21185590dc2a06da27f2585d546e2a379c2ff4f",
"source_classification": "complete",
"summary": "The symmetric and antisymmetric celestial prefactors alternate zeros and finite values at positive integers, while complementary simple poles and zeros occur at nonpositive integers, with exact residues at Delta=0 and 1.",
"title": "Celestial amplitudes in an ambidextrous basis"
},
{
"arxiv_ids": [
"2410.20296"
],
"claim": "Changing the infrared scale shifts the correlator only by -(log lambda)/(4 pi) times the angular contact delta; separated-point correlators and logarithmic-time derivatives are invariant.",
"classification": "exact contact-term theorem",
"discovery": "Boundary soft-scale cocycle",
"exact_check_count": 12,
"index": 6,
"kernel": "run_sabrina_boundary_soft_scale_cocycle",
"scientific_payload_sha256": "a335d252d7be59f9c40e7abc990331da16b0b54eda70f70d4fa5172d95b2e084",
"source_classification": "complete",
"summary": "Changing the infrared scale shifts the correlator only by -(log lambda)/(4 pi) times the angular contact delta; separated-point correlators and logarithmic-time derivatives are invariant.",
"title": "A Comment on Boundary Correlators: Soft Omissions and the Massless S-Matrix"
},
{
"arxiv_ids": [
"2501.00462"
],
"claim": "The transform of u^m partial_u^r Phi is fixed at every order by Gamma(nu)/Gamma(nu-m), and the induced raising and lowering operations obey the Weyl relation [D,U]=1.",
"classification": "all-orders representation theorem",
"discovery": "All-orders Carrollian-Mellin intertwiner",
"exact_check_count": 10,
"index": 7,
"kernel": "run_sabrina_carrollian_celestial_weyl_intertwiner",
"scientific_payload_sha256": "d0b52d420b0b0aae1fb470163344d5fb5916c44ba5527310e10482165c6132cd",
"source_classification": "complete",
"summary": "The transform of u^m partial_u^r Phi is fixed at every order by Gamma(nu)/Gamma(nu-m), and the induced raising and lowering operations obey the Weyl relation [D,U]=1.",
"title": "Multiparticle States for the Flat Hologram"
},
{
"arxiv_ids": [
"2501.00462"
],
"claim": "The published coefficient vector is unique only when both chiral weight pairs are nonzero; the kernel jumps to dimension two or four on the corresponding boundary loci.",
"classification": "hypothesis correction and boundary theorem",
"discovery": "Conglomerate-kernel rank stratification",
"exact_check_count": 12,
"index": 8,
"kernel": "run_sabrina_carrollian_conglomerate_kernel_stratification",
"scientific_payload_sha256": "3bd160a7dfa798b30b4390d34d11f59d48bd1398ec53c50dcc434e3fe64a4737",
"source_classification": "complete",
"summary": "The published coefficient vector is unique only when both chiral weight pairs are nonzero; the kernel jumps to dimension two or four on the corresponding boundary loci.",
"title": "Multiparticle States for the Flat Hologram"
},
{
"arxiv_ids": [
"2509.26264"
],
"claim": "If A lies in the manifold interior of B, then J+(A) lies in I+(B) and J-(A) lies in I-(B), with the closed-set boundary corollary stated explicitly.",
"classification": "exact causal lemma",
"discovery": "Causal interior-inclusion lemma",
"exact_check_count": 10,
"index": 9,
"kernel": "run_sabrina_causal_interior_inclusion_lemma",
"scientific_payload_sha256": "d99b817c432380bbff4836ba0a169029b609c9519bb2ee813a581878f4ac7531",
"source_classification": "complete",
"summary": "If A lies in the manifold interior of B, then J+(A) lies in I+(B) and J-(A) lies in I-(B), with the closed-set boundary corollary stated explicitly.",
"title": "On sufficient conditions for holographic scattering"
},
{
"arxiv_ids": [
"2404.14491"
],
"claim": "The cited alpha=0.495 code cannot correct arbitrary t-qubit errors, and after enforcing alpha<=1/4 the stated i.i.d. exponent is positive at base error 0.09; the package isolates repair classes without claiming the amplification theorem false.",
"classification": "proof-parameter obstruction",
"discovery": "CDQS amplification parameter obstruction",
"exact_check_count": 15,
"index": 10,
"kernel": "run_sabrina_cdqs_amplification_singleton_obstruction",
"scientific_payload_sha256": "030824c1879fcf5639d3fb849067dcd70eb43ab728bad7d3961c5fe44ac5f1b5",
"source_classification": "complete",
"summary": "The cited alpha=0.495 code cannot correct arbitrary t-qubit errors, and after enforcing alpha<=1/4 the stated i.i.d. exponent is positive at base error 0.09; the package isolates repair classes without claiming the amplification theorem false.",
"title": "Conditional disclosure of secrets with quantum resources"
},
{
"arxiv_ids": [
"2411.10527"
],
"claim": "Combining F<=min(1,2a) with I>=-2 log F yields I>=max(0,-2 log(2a)), strictly strengthening the displayed -log(a)-1 bound for every a>0.",
"classification": "strict bound strengthening",
"discovery": "Strengthened CDQS fidelity envelope",
"exact_check_count": 11,
"index": 11,
"kernel": "run_sabrina_cdqs_fidelity_envelope_strengthening",
"scientific_payload_sha256": "a74b4d88eeb5eac12a40fce9ce013f2e18f9e4a748ea1a973380efcbeadd519b",
"source_classification": "complete",
"summary": "Combining F<=min(1,2a) with I>=-2 log F yields I>=max(0,-2 log(2a)), strictly strengthening the displayed -log(a)-1 bound for every a>0.",
"title": "Cryptographic tests of the python's lunch conjecture"
},
{
"arxiv_ids": [
"2204.02505"
],
"claim": "A strict celestial circle separates finite incoming and outgoing point sets exactly when their embedded convex hulls are disjoint; either a separating plane or a finite Caratheodory obstruction certifies the answer.",
"classification": "geometric equivalence and certificates",
"discovery": "Celestial-circle convex-hull certificate",
"exact_check_count": 11,
"index": 12,
"kernel": "run_sabrina_celestial_circle_convex_hull_certificate",
"scientific_payload_sha256": "e838335f66a4c68f81f7e6f5678fe10cea02f297400cd6d76dda8ab4d73e73eb",
"source_classification": "complete",
"summary": "A strict celestial circle separates finite incoming and outgoing point sets exactly when their embedded convex hulls are disjoint; either a separating plane or a finite Caratheodory obstruction certifies the answer.",
"title": "Celestial Geometry"
},
{
"arxiv_ids": [
"2205.10901"
],
"claim": "Signed momentum conservation removes every leg-separable logarithm shift, and under the spanning hypothesis cancellation for all independent shifts conversely forces each participating p_i dot P to vanish.",
"classification": "exact invariance criterion and converse",
"discovery": "Eikonal logarithm gauge criterion",
"exact_check_count": 11,
"index": 13,
"kernel": "run_sabrina_celestial_eikonal_logarithm_gauge",
"scientific_payload_sha256": "496aa27aa4e52fa3a6f9da412561aaa652cf21690744c98593d94d0ffbe1e6f8",
"source_classification": "complete",
"summary": "Signed momentum conservation removes every leg-separable logarithm shift, and under the spanning hypothesis cancellation for all independent shifts conversely forces each participating p_i dot P to vanish.",
"title": "A Comment on Loop Corrections to the Celestial Stress Tensor"
},
{
"arxiv_ids": [
"2309.16602"
],
"claim": "Opposite Euclidean winding gives monodromy exp(2 pi i(alpha-beta)); paired factors are single-valued exactly for integer alpha-beta, while a one-variable complexified continuation remains obstructed generically.",
"classification": "monodromy theorem and boundary",
"discovery": "Euclidean monodromy cancellation",
"exact_check_count": 11,
"index": 14,
"kernel": "run_sabrina_celestial_euclidean_monodromy_cancellation",
"scientific_payload_sha256": "a1a2263b72c97030c657dcafd5ebb59be09b6c15290e6578fd342c0c83eba049",
"source_classification": "complete",
"summary": "Opposite Euclidean winding gives monodromy exp(2 pi i(alpha-beta)); paired factors are single-valued exactly for integer alpha-beta, while a one-variable complexified continuation remains obstructed generically.",
"title": "Multicollinear Singularities in Celestial CFT"
},
{
"arxiv_ids": [
"2012.15694"
],
"claim": "Repeated momentum insertions generate the exact rising-factorial ratio (Delta)_r/Delta^r, including its recurrence, zeros at negative integers, and pole of order r-1 at Delta=0.",
"classification": "all-orders operator identity",
"discovery": "All-order celestial momentum prefactor",
"exact_check_count": 11,
"index": 15,
"kernel": "run_sabrina_celestial_momentum_rising_factorial",
"scientific_payload_sha256": "643a45bec4e1890d5a2fb13854b61ccd5e0eccb5cce7a7a293ce045edef79e9c",
"source_classification": "complete",
"summary": "Repeated momentum insertions generate the exact rising-factorial ratio (Delta)_r/Delta^r, including its recurrence, zeros at negative integers, and pole of order r-1 at Delta=0.",
"title": "Shifting Spin on the Celestial Sphere"
},
{
"arxiv_ids": [
"2208.11635"
],
"claim": "The complete symmetric polynomial recursion resums to 1/((1-ax)(1-bx)) and exponentiates the amplitude PDE into an exact two-factor rational translation law.",
"classification": "generating-function resummation",
"discovery": "Closed celestial-recursion generating function",
"exact_check_count": 12,
"index": 16,
"kernel": "run_sabrina_celestial_recursion_pde_generating_function",
"scientific_payload_sha256": "94cf744ae42b66c5db61c4d853a7867562d928a7eb80e7cc3297657eb8fcf1cd",
"source_classification": "complete",
"summary": "The complete symmetric polynomial recursion resums to 1/((1-ax)(1-bx)) and exponentiates the amplitude PDE into an exact two-factor rational translation law.",
"title": "Celestial Recursion"
},
{
"arxiv_ids": [
"2606.13889"
],
"claim": "All geometric and gravitational scales cancel from C_flat/C_throat=[32+(7-p)^2]/[16(9-p)]; p=3 uniquely gives the maximal one-half reduction.",
"classification": "exact universal ratio",
"discovery": "Universal Coulomb-branch complexity ratio",
"exact_check_count": 15,
"index": 17,
"kernel": "run_sabrina_coulomb_branch_complexity_ratio",
"scientific_payload_sha256": "0a48392a955f724766d46453ed8d209ae2f1cfca84d21c71d0807b479504eb06",
"source_classification": "complete",
"summary": "All geometric and gravitational scales cancel from C_flat/C_throat=[32+(7-p)^2]/[16(9-p)]; p=3 uniquely gives the maximal one-half reduction.",
"title": "Flat Space Entanglement: A Coulomb Branch Perspective"
},
{
"arxiv_ids": [
"2307.16801"
],
"claim": "A prior Ouroboros correction was a false positive caused by reading source-local falling-factorial notation as a rising Pochhammer symbol; the source identity is exact under its stated convention, and the earlier claim is superseded.",
"classification": "self-correction and source confirmation",
"discovery": "Self-corrected detector sum identity",
"exact_check_count": 15,
"index": 18,
"kernel": "run_sabrina_detector_sum_identity_correction",
"scientific_payload_sha256": "a1b7a157ca0f6b33a4e558a471219f1c3b5c077bbca275918db542a467ec6aad",
"source_classification": "v1_false_positive_superseded_source_local_falling_factorial_identity_exact",
"summary": "A prior Ouroboros correction was a false positive caused by reading source-local falling-factorial notation as a rising Pochhammer symbol; the source identity is exact under its stated convention, and the earlier claim is superseded.",
"title": "Detector Operators for Celestial Symmetries"
},
{
"arxiv_ids": [
"1505.00716"
],
"claim": "For a fixed memory impulse M delivered over duration T, the driving fluence obeys Phi>=M^2/T, with equality for a constant ramp and an exact signal-to-noise relation for the detector.",
"classification": "sharp tradeoff bound",
"discovery": "Memory-detector fluence tradeoff",
"exact_check_count": 21,
"index": 19,
"kernel": "run_sabrina_electromagnetic_memory_detector_tradeoff",
"scientific_payload_sha256": "015631d9110b4b95c4a08337ca93d0143257d133d51159fe68736db9947d926e",
"source_classification": "complete",
"summary": "For a fixed memory impulse M delivered over duration T, the driving fluence obeys Phi>=M^2/T, with equality for a constant ramp and an exact signal-to-noise relation for the detector.",
"title": "Asymptotic Symmetries and Electromagnetic Memory"
},
{
"arxiv_ids": [
"2604.22612"
],
"claim": "The gap S_gen(s_ent)-I(V1;V2) is exactly the sum of four nonnegative geometric slacks divided by 4G_N, so saturation occurs if and only if all four source inequalities saturate.",
"classification": "exact slack decomposition",
"discovery": "Entanglement-scattering upper slack identity",
"exact_check_count": 11,
"index": 20,
"kernel": "run_sabrina_entanglement_scattering_slack_identity",
"scientific_payload_sha256": "65ed4ac892b7bc06c0e00a75b8253eceebe84a4342dbbdfc165c226b7a62fdf3",
"source_classification": "complete",
"summary": "The gap S_gen(s_ent)-I(V1;V2) is exactly the sum of four nonnegative geometric slacks divided by 4G_N, so saturation occurs if and only if all four source inequalities saturate.",
"title": "Generalized Entanglement Wedges and the Connected Wedge Theorem"
},
{
"arxiv_ids": [
"2604.22612"
],
"claim": "The finite-scale endpoint map is an eight-dimensional bijection with determinant -ell^-4, but its strict flat limit has rank four and loses exactly the four endpoint-time directions.",
"classification": "rank-drop theorem with exact kernel",
"discovery": "Flat boundary-corner rank drop",
"exact_check_count": 13,
"index": 21,
"kernel": "run_sabrina_flat_boundary_corner_rank_drop",
"scientific_payload_sha256": "0853ed3bb32e027bf8d6f6b380fcb29ace7776981e3c033036dac278b99443a6",
"source_classification": "complete",
"summary": "The finite-scale endpoint map is an eight-dimensional bijection with determinant -ell^-4, but its strict flat limit has rank four and loses exactly the four endpoint-time directions.",
"title": "Generalized Entanglement Wedges and the Connected Wedge Theorem"
},
{
"arxiv_ids": [
"2310.02186"
],
"claim": "The displayed extrapolate-dictionary equivalence is exact: the apparently missing factor is supplied by the positive rescaling t=(2u)^-1 together with the regulator rename, with no branch or normalization error.",
"classification": "source-equivalence proof",
"discovery": "Inverted Mellin normalization equivalence",
"exact_check_count": 14,
"index": 22,
"kernel": "run_sabrina_inverted_mellin_equivalence",
"scientific_payload_sha256": "8238ba9f3410ddad34f4ba9d8b58fed3f8b73f2da4ac14bd651fe311098aed7e",
"source_classification": "source_equation_consistent_normalization_rescaling_made_explicit",
"summary": "The displayed extrapolate-dictionary equivalence is exact: the apparently missing factor is supplied by the positive rescaling t=(2u)^-1 together with the regulator rename, with no branch or normalization error.",
"title": "Equating Extrapolate Dictionaries for Massless Scattering"
},
{
"arxiv_ids": [
"1905.10052"
],
"claim": "A permutation-invariant three-cut residual vanishes for every affine late-time signal and factorizes into a Vandermonde product times the quadratic curvature coefficient for the first nonlinear correction.",
"classification": "exact null test and curvature extractor",
"discovery": "Three-cut late-time null test",
"exact_check_count": 12,
"index": 23,
"kernel": "run_sabrina_late_time_three_cut_null_test",
"scientific_payload_sha256": "fc350a6e78c22144f885c36d6387db83ad9717444e32af7a851e5a32136bcbe8",
"source_classification": "late_time_three_cut_affine_null_test_and_quadratic_curvature_extraction_exact",
"summary": "A permutation-invariant three-cut residual vanishes for every affine late-time signal and factorizes into a Vandermonde product times the quadratic curvature coefficient for the first nonlinear correction.",
"title": "Implications of Superrotations"
},
{
"arxiv_ids": [
"1905.10052"
],
"claim": "Two cuts reconstruct the four late-time image components exactly, with an explicit origin-shift law and the additional condition required for origin-independent cross-order matching.",
"classification": "exact reconstruction theorem",
"discovery": "Two-cut late-time image reconstruction",
"exact_check_count": 16,
"index": 24,
"kernel": "run_sabrina_late_time_two_cut_reconstruction",
"scientific_payload_sha256": "db1fd19b1f87b4ae81f8df3e51fb7af41553eddcc0138d1b499afb0ace0a7614",
"source_classification": "late_time_two_cut_image_reconstruction_exact_with_origin_covariance",
"summary": "Two cuts reconstruct the four late-time image components exactly, with an explicit origin-shift law and the additional condition required for origin-independent cross-order matching.",
"title": "Implications of Superrotations"
},
{
"arxiv_ids": [
"2202.11127"
],
"claim": "A nonzero omega^m log^r(omega/mu) term produces a pole of exact order r+1 at Delta=-m with leading coefficient (-1)^r r!; changing scale mixes only lower poles.",
"classification": "pole-order theorem and correction",
"discovery": "Goldilocks logarithmic pole-order correction",
"exact_check_count": 11,
"index": 25,
"kernel": "run_sabrina_logarithmic_mellin_pole_order_correction",
"scientific_payload_sha256": "7e71ad1c811616ad2bae1d0eff9e16fe5a8aca3e975f7016352c215d2a8062a2",
"source_classification": "complete",
"summary": "A nonzero omega^m log^r(omega/mu) term produces a pole of exact order r+1 at Delta=-m with leading coefficient (-1)^r r!; changing scale mixes only lower poles.",
"title": "Goldilocks Modes and the Three Scattering Bases"
},
{
"arxiv_ids": [
"1407.3814"
],
"claim": "The commutator of two Low hard generators has no angular component and closes in the original family only when a specific covariant derivative vanishes; generic monomial modes provide explicit obstructions.",
"classification": "nonclosure theorem",
"discovery": "Low hard-generator nonclosure",
"exact_check_count": 18,
"index": 26,
"kernel": "run_sabrina_low_hard_generator_nonclosure",
"scientific_payload_sha256": "923662d26ef1703e8e9b20da3584065e853328708a7abc6c4e522e16abb2d9b5",
"source_classification": "complete",
"summary": "The commutator of two Low hard generators has no angular component and closes in the original family only when a specific covariant derivative vanishes; generic monomial modes provide explicit obstructions.",
"title": "Low's Subleading Soft Theorem as a Symmetry of QED"
},
{
"arxiv_ids": [],
"claim": "For the ordered complex conformal-scalar witness, the complete finite weight-(2,0) stress-tensor light-ray basis has rank three while the augmented system has rank four; an explicit left-null witness evaluates to 105/16.",
"classification": "basis-exclusion theorem",
"discovery": "Exact finite stress-basis exclusion at m=3",
"exact_check_count": 11,
"index": 27,
"kernel": "run_sabrina_m3_unclassified_module_construction",
"scientific_payload_sha256": "87a52883c1ab297c98ffbc371b709b01fb9e2a6054647a4be0487d54f0768bc7",
"source_classification": "exact_full_stress_basis_exclusion",
"summary": "For the ordered complex conformal-scalar witness, the complete finite weight-(2,0) stress-tensor light-ray basis has rank three while the augmented system has rank four; an explicit left-null witness evaluates to 105/16.",
"title": "M3 Unclassified Module Construction"
},
{
"arxiv_ids": [
"2501.00462"
],
"claim": "Each displayed beta-function pole has twice the printed residue because its pole-bearing Gamma argument has slope -1/2 in Delta; when branches collide, the corrected residues sum exactly to the coalesced tower.",
"classification": "source-equation correction",
"discovery": "Multiparticle beta-residue factor-two correction",
"exact_check_count": 11,
"index": 28,
"kernel": "run_sabrina_multiparticle_beta_residue_factor_two",
"scientific_payload_sha256": "6485daa678a208dfd8860503be6c60a553e2d767188c34ec80b762520c23e455",
"source_classification": "complete",
"summary": "Each displayed beta-function pole has twice the printed residue because its pole-bearing Gamma argument has slope -1/2 in Delta; when branches collide, the corrected residues sum exactly to the coalesced tower.",
"title": "Multiparticle States for the Flat Hologram"
},
{
"arxiv_ids": [
"1701.00049"
],
"claim": "The angular variable pushes forward exactly to a bounded radial interval with dc=(rho^2+2 epsilon)/(2 epsilon rho^2)drho, width and endpoint product 2 epsilon, and median sqrt(2 epsilon).",
"classification": "exact change-of-variables theorem",
"discovery": "Near-extremal radial pushforward",
"exact_check_count": 20,
"index": 29,
"kernel": "run_sabrina_near_extremal_radial_pushforward",
"scientific_payload_sha256": "2e51bc35b918b5683ba9f4c83c8ff6e0488713eb143c0d120e66640262410e4e",
"source_classification": "complete",
"summary": "The angular variable pushes forward exactly to a bounded radial interval with dc=(rho^2+2 epsilon)/(2 epsilon rho^2)drho, width and endpoint product 2 epsilon, and median sqrt(2 epsilon).",
"title": "Flat Space Amplitudes and Conformal Symmetry of the Celestial Sphere"
},
{
"arxiv_ids": [
"2606.13889"
],
"claim": "The p=4 spherical extremal surface admits an explicit matched large-P expansion through the first two nontrivial orders, including the renormalized area -3gR^2P^3/10+81g^2RP/35+O(P^-1).",
"classification": "theorem extension",
"discovery": "Omitted p=4 spherical entanglement extension",
"exact_check_count": 11,
"index": 30,
"kernel": "run_sabrina_p4_spherical_entanglement_expansion",
"scientific_payload_sha256": "15b684b9177c314bc5aeca308c80eae5ad95abfcd73c261eb7e7e51848f6b300",
"source_classification": "complete",
"summary": "The p=4 spherical extremal surface admits an explicit matched large-P expansion through the first two nontrivial orders, including the renormalized area -3gR^2P^3/10+81g^2RP/35+O(P^-1).",
"title": "Flat Space Entanglement: A Coulomb Branch Perspective"
},
{
"arxiv_ids": [
"2606.13889"
],
"claim": "Applying the refined-entropy operator to the p=4 spherical expansion gives g^3/P[45 log(P/R)/16+82933/560000]+O(P^-3), positive in the stated infrared regime and decaying to zero.",
"classification": "theorem extension and asymptotic result",
"discovery": "First nonzero p=4 refined-entropy term",
"exact_check_count": 11,
"index": 31,
"kernel": "run_sabrina_p4_spherical_refined_entropy",
"scientific_payload_sha256": "391c082d381a39de409e09c5d5d1798607ab16101326c4103bafbd5f220a2345",
"source_classification": "complete",
"summary": "Applying the refined-entropy operator to the p=4 spherical expansion gives g^3/P[45 log(P/R)/16+82933/560000]+O(P^-3), positive in the stated infrared regime and decaying to zero.",
"title": "Flat Space Entanglement: A Coulomb Branch Perspective"
},
{
"arxiv_ids": [
"2604.22612"
],
"claim": "The lower gap I(V1;V2)-S_gen(e_max(s_pts'')) is exactly the sum of four nonnegative CWT, ridge, focusing, and maximization slacks, with an if-and-only-if saturation criterion.",
"classification": "exact slack decomposition",
"discovery": "Point-scattering lower slack identity",
"exact_check_count": 14,
"index": 32,
"kernel": "run_sabrina_points_scattering_lower_slack_identity",
"scientific_payload_sha256": "7f9b013510e795182939e14d751abafa52301bf7e7cd140ff4fa5a32a2b8db69",
"source_classification": "complete",
"summary": "The lower gap I(V1;V2)-S_gen(e_max(s_pts'')) is exactly the sum of four nonnegative CWT, ridge, focusing, and maximization slacks, with an if-and-only-if saturation criterion.",
"title": "Generalized Entanglement Wedges and the Connected Wedge Theorem"
},
{
"arxiv_ids": [
"1905.10052"
],
"claim": "The principal-series measure factorizes into explicit positive polynomials for every even and odd integer dimension, obeys a two-dimension recurrence, and has the correct quadratic zero at the origin.",
"classification": "all-dimension factorization theorem",
"discovery": "All-integer-d Plancherel factorization",
"exact_check_count": 14,
"index": 33,
"kernel": "run_sabrina_principal_series_plancherel_factorization",
"scientific_payload_sha256": "4047efe441ad0800b95a0d64b4354de371b4f6fdf6be4f1cbe59763680be8178",
"source_classification": "principal_series_plancherel_measure_all_integer_d_factorization_exact",
"summary": "The principal-series measure factorizes into explicit positive polynomials for every even and odd integer dimension, obeys a two-dimension recurrence, and has the correct quadratic zero at the origin.",
"title": "Implications of Superrotations"
},
{
"arxiv_ids": [
"1706.03917"
],
"claim": "Under canonical massless scaling, stripped-amplitude, Mellin-weight, momentum-delta, and projective-Jacobian degrees cancel exactly for arbitrary spacetime dimension D and particle count n.",
"classification": "all-D, all-n theorem",
"discovery": "All-D, all-n projective Mellin scale cancellation",
"exact_check_count": 12,
"index": 34,
"kernel": "run_sabrina_projective_mellin_scale_theorem",
"scientific_payload_sha256": "bb866693a5cac8a1a30c7d4d3dec8feea3e6911173eca33cae0c27c503449354",
"source_classification": "all_D_all_n_projective_mellin_radial_scale_cancellation_exact_under_canonical_scaling",
"summary": "Under canonical massless scaling, stripped-amplitude, Mellin-weight, momentum-delta, and projective-Jacobian degrees cancel exactly for arbitrary spacetime dimension D and particle count n.",
"title": "Gluon Amplitudes as 2d Conformal Correlators"
},
{
"arxiv_ids": [
"1706.03917"
],
"claim": "For a square localization system, Cramer signed-minor ratios give the unique simplex coordinates; strict positivity characterizes interior support, nonnegativity with a zero characterizes the boundary, and the Jacobian is 1/abs(det M).",
"classification": "support, positivity, and Jacobian theorem",
"discovery": "Projective-simplex signed-minor theorem",
"exact_check_count": 13,
"index": 35,
"kernel": "run_sabrina_projective_simplex_positivity_theorem",
"scientific_payload_sha256": "04b196f77ef38f277dfbb7ebeccf2b1964f90157335f9a1dc268c6654d548af4",
"source_classification": "square_projective_simplex_signed_minor_support_and_jacobian_theorem_exact",
"summary": "For a square localization system, Cramer signed-minor ratios give the unique simplex coordinates; strict positivity characterizes interior support, nonnegativity with a zero characterizes the boundary, and the Jacobian is 1/abs(det M).",
"title": "Gluon Amplitudes as 2d Conformal Correlators"
},
{
"arxiv_ids": [
"1706.03917"
],
"claim": "For a (D+1)-by-n constraint matrix of generic rank min(D+1,n), the theorem gives the exact number of residual external constraints or unfixed simplex moduli and separates unique, boundary, incompatible, and continuous-support regimes.",
"classification": "all-D rank and support theorem",
"discovery": "All-D projective-simplex rank theorem",
"exact_check_count": 18,
"index": 36,
"kernel": "run_sabrina_projective_simplex_rank_theorem",
"scientific_payload_sha256": "a4be65bfe6724693b679405e1985b33302d94ec8113edf75512620fcc58045f7",
"source_classification": "all_D_projective_simplex_localization_rank_theorem_exact_with_support_and_positivity_boundaries",
"summary": "For a (D+1)-by-n constraint matrix of generic rank min(D+1,n), the theorem gives the exact number of residual external constraints or unfixed simplex moduli and separates unique, boundary, incompatible, and continuous-support regimes.",
"title": "Gluon Amplitudes as 2d Conformal Correlators"
},
{
"arxiv_ids": [
"1502.06120"
],
"claim": "The cap response is an explicit quintic with antipodal-complement antisymmetry F(1-x)=-F(x), complete physical zero set {0,1/2,1}, and an exact factorization exposing every sign change.",
"classification": "duality and factorization theorem",
"discovery": "Quadrupole spin-memory cap duality",
"exact_check_count": 16,
"index": 37,
"kernel": "run_sabrina_quadrupole_spin_memory_cap_duality",
"scientific_payload_sha256": "ec237ce1930d800c155dbce44a6eb3a8c2c5c9d65bcf638d05a6583ce813ba9a",
"source_classification": "complete",
"summary": "The cap response is an explicit quintic with antipodal-complement antisymmetry F(1-x)=-F(x), complete physical zero set {0,1/2,1}, and an exact factorization exposing every sign change.",
"title": "New Gravitational Memories"
},
{
"arxiv_ids": [
"1905.09809"
],
"claim": "The published fourth-order radial equation factorizes exactly as [rho^2(D^2-4)+4L]^2, revealing generalized-kernel modes killed by the square but not by the second-order factor.",
"classification": "operator factorization theorem",
"discovery": "Radial Einstein operator is an exact square",
"exact_check_count": 10,
"index": 38,
"kernel": "run_sabrina_radial_einstein_square_factorization",
"scientific_payload_sha256": "7ecf43b482eecb12234e230a243c73209adfdb80078a068221722a2dd1380e56",
"source_classification": "complete",
"summary": "The published fourth-order radial equation factorizes exactly as [rho^2(D^2-4)+4L]^2, revealing generalized-kernel modes killed by the square but not by the second-order factor.",
"title": "Uplifting AdS3/CFT2 to Flat Space Holography"
},
{
"arxiv_ids": [
"2606.13889"
],
"claim": "An exact boundary identity proves the coefficient equality previously supported numerically: C3^(p)=(7-p)/(9-p)[(C1^(p))^2+(C2^(p))^2], with the mechanism traced to alpha^2+beta^2=7-p.",
"classification": "analytic proof of source equality",
"discovery": "Analytic proof of the flat-space RT equality",
"exact_check_count": 14,
"index": 39,
"kernel": "run_sabrina_rt_area_boundary_identity",
"scientific_payload_sha256": "ee27f366b07f19111f42a6487e69e75576daa09711cfb41f9012311047bff850",
"source_classification": "complete",
"summary": "An exact boundary identity proves the coefficient equality previously supported numerically: C3^(p)=(7-p)/(9-p)[(C1^(p))^2+(C2^(p))^2], with the mechanism traced to alpha^2+beta^2=7-p.",
"title": "Flat Space Entanglement: A Coulomb Branch Perspective"
},
{
"arxiv_ids": [
"2512.02825"
],
"claim": "Ward conservation gives an exact subset-sum formula for every connected soft cumulant of order n>=2; deterministic incoming charge drops out, while mixed cumulants are the precise obstruction to a factorized hard-only reduction.",
"classification": "all-orders hierarchy and obstruction",
"discovery": "Full soft-charge cumulant hierarchy",
"exact_check_count": 13,
"index": 40,
"kernel": "run_sabrina_soft_charge_cumulant_hierarchy",
"scientific_payload_sha256": "8ed6c8d8dcc8eabf62402d94d7fdfcc3c000f15edec4ba8c1f437a6040cb2731",
"source_classification": "complete",
"summary": "Ward conservation gives an exact subset-sum formula for every connected soft cumulant of order n>=2; deterministic incoming charge drops out, while mixed cumulants are the precise obstruction to a factorized hard-only reduction.",
"title": "Memory Correlators and Ward Identities in the 'in-in' Formalism"
},
{
"arxiv_ids": [
"2012.03850"
],
"claim": "Fixed total-charge support forces the reduced radiation state to commute with its charge, permits arbitrary degeneracy inside each charge block, and yields the exact entropy decomposition into sector entropy plus within-sector entropy.",
"classification": "reduced-state structure theorem",
"discovery": "Soft-charge reduced-state block theorem",
"exact_check_count": 15,
"index": 41,
"kernel": "run_sabrina_soft_charge_reduced_state_theorem",
"scientific_payload_sha256": "1934ba760699c1f3d024f8428611b3b7b3dde43b9a45a54fd868c65b4cc5a8f6",
"source_classification": "complete",
"summary": "Fixed total-charge support forces the reduced radiation state to commute with its charge, permits arbitrary degeneracy inside each charge block, and yields the exact entropy decomposition into sector entropy plus within-sector entropy.",
"title": "HPS meets AMPS: How Soft Hair Dissolves the Firewall"
},
{
"arxiv_ids": [
"2604.19866"
],
"claim": "Under linear mode action and the derivation rule, multiplying every elementary charge commutator by lambda multiplies the whole dressing commutator by lambda; lambda=2 cannot preserve a nonzero target without compensating repair.",
"classification": "no-go theorem and repair boundary",
"discovery": "Soft-dressing factor-two no-go",
"exact_check_count": 13,
"index": 42,
"kernel": "run_sabrina_soft_dressing_factor_two_no_go",
"scientific_payload_sha256": "694c94424ad44968ecc374bad8ce5fce735e410342d9142b79c566066a0ca029",
"source_classification": "complete",
"summary": "Under linear mode action and the derivation rule, multiplying every elementary charge commutator by lambda multiplies the whole dressing commutator by lambda; lambda=2 cannot preserve a nonzero target without compensating repair.",
"title": "Asymptotic charges as detectors and the memory effect in massive QED and perturbative quantum gravity"
},
{
"arxiv_ids": [
"2105.09792"
],
"claim": "The unqualified all-n identity requires an n! factor: the Mellin residue is g^(n)(0)/n!, so the source formula is exact at n=0,1 and is restored for all n by multiplying the residue side by n! or dividing u^n by n!.",
"classification": "source-equation correction",
"discovery": "Soft-Mellin factorial correction",
"exact_check_count": 12,
"index": 43,
"kernel": "run_sabrina_soft_mellin_residue_identity",
"scientific_payload_sha256": "2bac79f473b925a796d826a6c2d4fdd4003b5c269b8843d9f37dd83ed0e4d58f",
"source_classification": "physical_n0_n1_exact_unqualified_all_n_extension_requires_factorial",
"summary": "The unqualified all-n identity requires an n! factor: the Mellin residue is g^(n)(0)/n!, so the source formula is exact at n=0,1 and is restored for all n by multiplying the residue side by n! or dividing u^n by n!.",
"title": "Revisiting the Conformally Soft Sector with Celestial Diamonds"
},
{
"arxiv_ids": [
"1705.01027"
],
"claim": "The formal Delta=1 shadow field strength carries an unavoidable factor d-2 and has an explicit nonzero component for d!=2; only d=2 is self-shadow and pure gauge in the tested sense.",
"classification": "dimension-specific obstruction theorem",
"discovery": "Spin-1 shadow gauge obstruction",
"exact_check_count": 19,
"index": 44,
"kernel": "run_sabrina_spin1_shadow_gauge_obstruction",
"scientific_payload_sha256": "147d7f9336fd649e66d2d1995c6287514571d2ae8c83f798615712be5580eda5",
"source_classification": "complete",
"summary": "The formal Delta=1 shadow field strength carries an unavoidable factor d-2 and has an explicit nonzero component for d!=2; only d=2 is self-shadow and pure gauge in the tested sense.",
"title": "A Conformal Basis for Flat Space Amplitudes"
},
{
"arxiv_ids": [
"1406.3312"
],
"claim": "Pure-gauge variation of the subleading soft factor vanishes for every reference pair exactly when the summed angular-momentum defect Delta J is zero; basis polarizations recover every defect component.",
"classification": "if-and-only-if gauge theorem",
"discovery": "Subleading-soft gauge-defect theorem",
"exact_check_count": 12,
"index": 45,
"kernel": "run_sabrina_subleading_soft_gauge_defect_theorem",
"scientific_payload_sha256": "f7f1619f5cf9b96d1c0093c8a1f8c0aff35360814eeaa17ab81bc686a50a3b61",
"source_classification": "complete",
"summary": "Pure-gauge variation of the subleading soft factor vanishes for every reference pair exactly when the summed angular-momentum defect Delta J is zero; basis polarizations recover every defect component.",
"title": "Semiclassical Virasoro Symmetry of the Quantum Gravity S-Matrix"
},
{
"arxiv_ids": [
"2108.11422"
],
"claim": "All routes to a fixed fermionic mode span a rank-one commutator image and obey an exact pairwise syzygy, with a classified exceptional route whenever m=2t/3 is integral.",
"classification": "infinite algebraic identity family",
"discovery": "Infinite super-BMS commutator syzygy family",
"exact_check_count": 9,
"index": 46,
"kernel": "run_sabrina_super_bms_commutator_syzygy_family",
"scientific_payload_sha256": "0c0559f924de94f512ba19fd2d867bfef93412978ddcb2cfd055a85cdcf94086",
"source_classification": "complete",
"summary": "All routes to a fixed fermionic mode span a rank-one commutator image and obey an exact pairwise syzygy, with a classified exceptional route whenever m=2t/3 is integral.",
"title": "Conformally Soft Fermions"
},
{
"arxiv_ids": [
"2005.08990"
],
"claim": "Under the source's explicit holomorphic restriction, the boundary term cancels both shear terms and the antiholomorphic news term, doubles only the holomorphic news term, and reproduces the exact 1/(16 pi G) charge.",
"classification": "exact source reduction",
"discovery": "Holomorphic superrotation charge cancellation",
"exact_check_count": 12,
"index": 47,
"kernel": "run_sabrina_superrotation_charge_cancellation",
"scientific_payload_sha256": "9081bdaa476d9558567b5363b9a85389cdaf84998fd93684f74822acd8c1ad47",
"source_classification": "source_consistent_holomorphic_superrotation_charge_exactly_reduced",
"summary": "Under the source's explicit holomorphic restriction, the boundary term cancels both shear terms and the antiholomorphic news term, doubles only the holomorphic news term, and reproduces the exact 1/(16 pi G) charge.",
"title": "Asymptotic Symmetries and Celestial CFT"
},
{
"arxiv_ids": [
"2402.18798"
],
"claim": "The OPE ambiguity depends on the normalized kernel only through M[f]=1/4-integral f(t)(t-1/2)^2dt; positivity gives the sharp interval [0,1/4], while normalization alone admits an explicit unbounded signed family.",
"classification": "sharp bound and counterexample family",
"discovery": "Two-particle kernel variance theorem",
"exact_check_count": 14,
"index": 48,
"kernel": "run_sabrina_two_particle_kernel_variance",
"scientific_payload_sha256": "7b1aa48423c6010da14e5d02a47c618b324310dbf80b043db8546fbcc3ee59b6",
"source_classification": "complete",
"summary": "The OPE ambiguity depends on the normalized kernel only through M[f]=1/4-integral f(t)(t-1/2)^2dt; positivity gives the sharp interval [0,1/4], while normalization alone admits an explicit unbounded signed family.",
"title": "Multiparticle Contributions to the Celestial OPE"
},
{
"arxiv_ids": [
"2012.15694"
],
"claim": "Delta maps to 2-Delta as an exact involution exchanging primary and shadow gauge, scalar, and Weyl data while preserving the reduced double-copy quotient and exchanging its Delta=0 and 2 divisors.",
"classification": "involution and equivariance theorem",
"discovery": "Weyl-double-copy shadow involution",
"exact_check_count": 17,
"index": 49,
"kernel": "run_sabrina_weyl_double_copy_shadow_involution",
"scientific_payload_sha256": "f6243bc6dfdd05769cab60b02d4e23c53ef9c0119f2ac7a10d54eda023956fee",
"source_classification": "complete",
"summary": "Delta maps to 2-Delta as an exact involution exchanging primary and shadow gauge, scalar, and Weyl data while preserving the reduced double-copy quotient and exchanging its Delta=0 and 2 divisors.",
"title": "Shifting Spin on the Celestial Sphere"
}
],
"schema": "ouroboros_result_catalog_v1"
}
|