{
 "id": "LIB2-104",
 "entry_version": 7,
 "class": "CLAIM",
 "title": "The bare quartic is not stationary at the registered golden boundary point",
 "statement": "At the registered split-real golden boundary point z0, dI4(z0) ≠ 0, so the bare quartic cannot by itself select that point as a stationary vacuum.",
 "scope": {
  "carrier": "The bare quartic I4 at the registered golden boundary point z0",
  "domain": "Stationarity of the bare quartic only, not the constrained potentials treated elsewhere.",
  "group": null,
  "hypotheses": [
   "Retain the declared split real form.",
   "Appendix Q assigns its statements conditional tier on the κphys candidate mechanism."
  ],
  "physical_target": null,
  "quantifier": "The declared source class only.",
  "real_form": "Declared split real form"
 },
 "source_labels_as_printed": {
  "math_status": "NOT_PRINTED",
  "attachment": "NOT_PRINTED",
  "scorecard_tier_word": null,
  "pdf_page": 277
 },
 "house_tier": null,
 "review_state": "PUBLISHED",
 "scientific_status": "UNDER_REVIEW (house status not yet adjudicated)",
 "evidence_status": [
  {
   "kind": "registry",
   "availability": "shipped"
  }
 ],
 "primary_source": {
  "component": "Appendix Q",
  "section": "§3(i), Bare-quartic gradient",
  "pdf_page": 292,
  "quote": "z0 is not a critical point of the bare quartic. Direct computation gives dI4 (z0 ) ̸= 0,"
 },
 "caution": "Nonstationarity of the bare quartic does not contradict stationarity of a separately constrained or sourced action.",
 "candidate_ids": [
  "C2-042"
 ],
 "basis": {
  "pdf_sha256_prefix": "b64ddcd9e16a6dcd",
  "release": "Rev33.1_S369"
 },
 "relationships": [
  {
   "type": "related_to",
   "target": "LIB2-079"
  }
 ],
 "url": "/library-v2/LIB2-104/",
 "content_sha256": "977583e35e0fda3585fa223ff24315a5992f395b40eec756cdd0d716819ece5b",
 "build_stamp": "BUILD_STAMP S371a · 2026-09-26T22:53Z · master 01d1a5873ede42f5 · cut 9dcc6ce9a8ee3e02"
}