{"as_of":"2026-08-08T20:50:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:6e9afe60f1f453092b6dc24d2be2f87d97640ae742045c860af0cf95461ed449","coverage":[{"denominator":32,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":32,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-02T09:19:10.431987Z","state":"measured"},{"denominator":32,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":32,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-08T06:32:00.761636+00:00","state":"measured"},{"denominator":0,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":0,"source":"paper_references, paper_reference_links","source_observed_at":null,"state":"measured"},{"denominator":1,"lane":"external_citation_measurements","note":"A source-named dated measurement, never combined with another source.","records_observed":0,"source":"cited_works","source_observed_at":null,"state":"measured"}],"external_citation_measurements":[],"inbound":[],"links":{"evidence":"/evidence","html":"/paper/2607.01274/citation-record","integrity":"/paper/2607.01274/integrity","json":"/paper/2607.01274/citation-record.json","paper":"/paper/2607.01274"},"outbound":[{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-02T09:19:05.843701Z","title":"Lorentzian metric signa- ture is (−,+,+,+) and Euclidean metric signature is (+,+,+,+)","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2607.01274","last_updated":"2026-07-27T13:47:41Z","snapshot_observed_at":"2026-08-02T09:19:04.904084Z","submitted_at":"2026-06-30T22:28:24Z","title":"Inflation from Covariant Signature Change: A Geometric Mechanism","version":2},"reference_index":1,"source":"pdf_text","source_observed_at":"2026-08-02T09:19:05.843701Z"},"links":{"citing_paper":"/paper/2607.01274"},"observation_digest":"sha256:ee3d473d319484f66f01da13a5b804d17e37add285c03b93c211167c8ce001bb","observation_id":"21bbad55-ba55-4461-9c48-692860ec4fa1","resolution":{"observed_at":"2026-08-02T09:19:05.843701Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-02T09:19:05.914414Z","title":"degenerate but non–singular","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2607.01274","last_updated":"2026-07-27T13:47:41Z","snapshot_observed_at":"2026-08-02T09:19:04.904084Z","submitted_at":"2026-06-30T22:28:24Z","title":"Inflation from Covariant Signature Change: A Geometric Mechanism","version":2},"reference_index":2,"source":"pdf_text","source_observed_at":"2026-08-02T09:19:05.914414Z"},"links":{"citing_paper":"/paper/2607.01274"},"observation_digest":"sha256:0012f23eb39a48548607df554438d67b5428a72ac8a09b39b83d648f14103d85","observation_id":"a7525d16-eb30-4b5b-84e1-ee17179e4bfd","resolution":{"observed_at":"2026-08-02T09:19:05.914414Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-02T09:19:05.999961Z","title":null,"venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2607.01274","last_updated":"2026-07-27T13:47:41Z","snapshot_observed_at":"2026-08-02T09:19:04.904084Z","submitted_at":"2026-06-30T22:28:24Z","title":"Inflation from Covariant Signature Change: A Geometric Mechanism","version":2},"reference_index":3,"source":"pdf_text","source_observed_at":"2026-08-02T09:19:05.999961Z"},"links":{"citing_paper":"/paper/2607.01274"},"observation_digest":"sha256:39fb3b50a1fdc2a0ababc5dbfeb08c371b6e55ec8a7372c3fa843e4856602163","observation_id":"1628a2f0-d533-4dc2-81f0-31051836142a","resolution":{"observed_at":"2026-08-02T09:19:05.999961Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-02T09:19:06.079424Z","title":null,"venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2607.01274","last_updated":"2026-07-27T13:47:41Z","snapshot_observed_at":"2026-08-02T09:19:04.904084Z","submitted_at":"2026-06-30T22:28:24Z","title":"Inflation from Covariant Signature Change: A Geometric Mechanism","version":2},"reference_index":4,"source":"pdf_text","source_observed_at":"2026-08-02T09:19:06.079424Z"},"links":{"citing_paper":"/paper/2607.01274"},"observation_digest":"sha256:38cc4e5f9ff7c34a42ff9e1a5ff6030e8ce5b20a34b0f4377bb82c5919f956d5","observation_id":"a03a6f88-f2d9-42ee-a0ae-274365467729","resolution":{"observed_at":"2026-08-02T09:19:06.079424Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-02T09:19:06.166489Z","title":"III is πmn = Θ \" 2t(mKn)a∇uua −KK mn − ∇uKmn + hmn 3 ∇uK+K 2 # + ˙Θ 6 (Kh mn −3K mn),(B8) with∇ u ≡u a∇a","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2607.01274","last_updated":"2026-07-27T13:47:41Z","snapshot_observed_at":"2026-08-02T09:19:04.904084Z","submitted_at":"2026-06-30T22:28:24Z","title":"Inflation from Covariant Signature Change: A Geometric Mechanism","version":2},"reference_index":5,"source":"pdf_text","source_observed_at":"2026-08-02T09:19:06.166489Z"},"links":{"citing_paper":"/paper/2607.01274"},"observation_digest":"sha256:a2bcb63ec05c4f450b437cef9ceb7200bc6d979ce9d45d5876fab358c9d183bf","observation_id":"df1a5e81-0a20-41ed-8b6b-eff3fab14447","resolution":{"observed_at":"2026-08-02T09:19:06.166489Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-02T09:19:06.386571Z","title":"III, the effective energy density can be writ- ten as ρ= F 2 ∇mam − (3)R+ Θ∇ uK , F≡ Θ 1 + Θ","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2607.01274","last_updated":"2026-07-27T13:47:41Z","snapshot_observed_at":"2026-08-02T09:19:04.904084Z","submitted_at":"2026-06-30T22:28:24Z","title":"Inflation from Covariant Signature Change: A Geometric Mechanism","version":2},"reference_index":6,"source":"pdf_text","source_observed_at":"2026-08-02T09:19:06.386571Z"},"links":{"citing_paper":"/paper/2607.01274"},"observation_digest":"sha256:fda6f95b1c8498a3c7c90f0d7781f154caee14d556be881bebc7f76fb0a525f0","observation_id":"32cd37c2-f8ac-4605-a1dc-437a2786343c","resolution":{"observed_at":"2026-08-02T09:19:06.386571Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-02T09:19:06.564625Z","title":"Definition and slope","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2607.01274","last_updated":"2026-07-27T13:47:41Z","snapshot_observed_at":"2026-08-02T09:19:04.904084Z","submitted_at":"2026-06-30T22:28:24Z","title":"Inflation from Covariant Signature Change: A Geometric Mechanism","version":2},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-08-02T09:19:06.564625Z"},"links":{"citing_paper":"/paper/2607.01274"},"observation_digest":"sha256:5ba74f8ba6fe203eba499ceb8f347e1f92e0c3942e988c9df6b8ec28817c0312","observation_id":"8faf6350-ba96-4a0e-bc2f-7aff81cd4253","resolution":{"observed_at":"2026-08-02T09:19:06.564625Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-02T09:19:06.707389Z","title":null,"venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2607.01274","last_updated":"2026-07-27T13:47:41Z","snapshot_observed_at":"2026-08-02T09:19:04.904084Z","submitted_at":"2026-06-30T22:28:24Z","title":"Inflation from Covariant Signature Change: A Geometric Mechanism","version":2},"reference_index":8,"source":"pdf_text","source_observed_at":"2026-08-02T09:19:06.707389Z"},"links":{"citing_paper":"/paper/2607.01274"},"observation_digest":"sha256:921d5764d1c9c5c1864169b07c8769d1192be1adb415a51c35cf80939e73ab5e","observation_id":"108fc960-a444-4050-8119-082142f434ec","resolution":{"observed_at":"2026-08-02T09:19:06.707389Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-02T09:19:06.893438Z","title":"Definition and slope","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2607.01274","last_updated":"2026-07-27T13:47:41Z","snapshot_observed_at":"2026-08-02T09:19:04.904084Z","submitted_at":"2026-06-30T22:28:24Z","title":"Inflation from Covariant Signature Change: A Geometric Mechanism","version":2},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-08-02T09:19:06.893438Z"},"links":{"citing_paper":"/paper/2607.01274"},"observation_digest":"sha256:2b5fa33c6d53c99a8e7c486e2d9894cea775e018a40f08e58d9d88674b279bcd","observation_id":"922e640e-b294-4c7d-aeb8-5017dbefebb5","resolution":{"observed_at":"2026-08-02T09:19:06.893438Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-02T09:19:07.052335Z","title":null,"venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2607.01274","last_updated":"2026-07-27T13:47:41Z","snapshot_observed_at":"2026-08-02T09:19:04.904084Z","submitted_at":"2026-06-30T22:28:24Z","title":"Inflation from Covariant Signature Change: A Geometric Mechanism","version":2},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-08-02T09:19:07.052335Z"},"links":{"citing_paper":"/paper/2607.01274"},"observation_digest":"sha256:8f460309912fc5dab62e52a5adb99ea73b1d48267331e6b4b2f9dc6be59a8784","observation_id":"315f9b45-389d-4eac-9993-178dac16d6eb","resolution":{"observed_at":"2026-08-02T09:19:07.052335Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-02T09:19:07.144498Z","title":"(D1) gives Ne = 1 ϵH ln 1 +ϵ H H⋆∆tinf ,∆t inf ≡t end −t ⋆","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2607.01274","last_updated":"2026-07-27T13:47:41Z","snapshot_observed_at":"2026-08-02T09:19:04.904084Z","submitted_at":"2026-06-30T22:28:24Z","title":"Inflation from Covariant Signature Change: A Geometric Mechanism","version":2},"reference_index":11,"source":"pdf_text","source_observed_at":"2026-08-02T09:19:07.144498Z"},"links":{"citing_paper":"/paper/2607.01274"},"observation_digest":"sha256:9c0187332778bb24c0b50e04d2c436f9548b7d370b660de41f2f5cd3844ff2a3","observation_id":"b2ef82fc-bf85-4af6-b6b9-d5bc8cce1c24","resolution":{"observed_at":"2026-08-02T09:19:07.144498Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-02T09:19:07.243032Z","title":"relative corrections∼ϵ eff Ne","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2607.01274","last_updated":"2026-07-27T13:47:41Z","snapshot_observed_at":"2026-08-02T09:19:04.904084Z","submitted_at":"2026-06-30T22:28:24Z","title":"Inflation from Covariant Signature Change: A Geometric Mechanism","version":2},"reference_index":12,"source":"pdf_text","source_observed_at":"2026-08-02T09:19:07.243032Z"},"links":{"citing_paper":"/paper/2607.01274"},"observation_digest":"sha256:963d390c32688bff80cf2032434c55ad31d4c7af97ea28fe6b07476b5ef4c3b7","observation_id":"861304ef-70fd-4a70-a85e-6f126275b0a7","resolution":{"observed_at":"2026-08-02T09:19:07.243032Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-02T09:19:07.376525Z","title":null,"venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2607.01274","last_updated":"2026-07-27T13:47:41Z","snapshot_observed_at":"2026-08-02T09:19:04.904084Z","submitted_at":"2026-06-30T22:28:24Z","title":"Inflation from Covariant Signature Change: A Geometric Mechanism","version":2},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-08-02T09:19:07.376525Z"},"links":{"citing_paper":"/paper/2607.01274"},"observation_digest":"sha256:6e9f8781f2b6581c448aa7c8e5097bafeb2345e7e8d4dda6ae76c5aa56594fc7","observation_id":"34619a78-805f-45f9-947a-b258efac3e02","resolution":{"observed_at":"2026-08-02T09:19:07.376525Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-02T09:19:07.549019Z","title":null,"venue":null,"work_id":null,"year":1983},"citing_paper":{"arxiv_id":"2607.01274","last_updated":"2026-07-27T13:47:41Z","snapshot_observed_at":"2026-08-02T09:19:04.904084Z","submitted_at":"2026-06-30T22:28:24Z","title":"Inflation from Covariant Signature Change: A Geometric Mechanism","version":2},"reference_index":14,"source":"pdf_text","source_observed_at":"2026-08-02T09:19:07.549019Z"},"links":{"citing_paper":"/paper/2607.01274"},"observation_digest":"sha256:34d2dc28dce088121880be5a4552d675a59266cd5b2a1a2090d6c7d782b8248e","observation_id":"1595ac66-70ee-46fa-95fe-df82173f2108","resolution":{"observed_at":"2026-08-02T09:19:07.549019Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-02T09:19:07.725872Z","title":null,"venue":null,"work_id":null,"year":1990},"citing_paper":{"arxiv_id":"2607.01274","last_updated":"2026-07-27T13:47:41Z","snapshot_observed_at":"2026-08-02T09:19:04.904084Z","submitted_at":"2026-06-30T22:28:24Z","title":"Inflation from Covariant Signature Change: A Geometric Mechanism","version":2},"reference_index":15,"source":"pdf_text","source_observed_at":"2026-08-02T09:19:07.725872Z"},"links":{"citing_paper":"/paper/2607.01274"},"observation_digest":"sha256:447a78e391feb2eb928a0681701a4f21e538cbb85ca61d3bfafdfd66c000a5ee","observation_id":"6f6d40c3-9bf0-4608-9685-6cdeba2a55f4","resolution":{"observed_at":"2026-08-02T09:19:07.725872Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1112.1899","last_updated":"2011-12-08T17:56:59Z","snapshot_observed_at":"2026-07-06T02:39:03.428680Z","submitted_at":"2011-12-08T17:56:59Z","title":"Deformed General Relativity and Effective Actions from Loop Quantum Gravity","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1112.1899","snapshot_observed_at":"2026-08-02T09:19:07.912491Z","title":"Bojowald and G","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"2607.01274","last_updated":"2026-07-27T13:47:41Z","snapshot_observed_at":"2026-08-02T09:19:04.904084Z","submitted_at":"2026-06-30T22:28:24Z","title":"Inflation from Covariant Signature Change: A Geometric Mechanism","version":2},"reference_index":16,"source":"pdf_text","source_observed_at":"2026-08-02T09:19:07.912491Z"},"links":{"cited_paper":"/paper/1112.1899","citing_paper":"/paper/2607.01274"},"observation_digest":"sha256:a5168a5a7cc31d32b557252faaceb2bee52fab42ada6a07ee64a8f8a46e341ce","observation_id":"73827696-8fae-443f-9389-30ece86b3624","resolution":{"observed_at":"2026-08-02T09:19:07.912491Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1909.10669","last_updated":"2019-09-24T01:04:40Z","snapshot_observed_at":"2026-07-06T08:24:02.658708Z","submitted_at":"2019-09-24T01:04:40Z","title":"Alternative route towards the change of metric signature","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1909.10669","snapshot_observed_at":"2026-08-02T09:19:08.088455Z","title":"Zhang, Phys","venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2607.01274","last_updated":"2026-07-27T13:47:41Z","snapshot_observed_at":"2026-08-02T09:19:04.904084Z","submitted_at":"2026-06-30T22:28:24Z","title":"Inflation from Covariant Signature Change: A Geometric Mechanism","version":2},"reference_index":17,"source":"pdf_text","source_observed_at":"2026-08-02T09:19:08.088455Z"},"links":{"cited_paper":"/paper/1909.10669","citing_paper":"/paper/2607.01274"},"observation_digest":"sha256:3377fdac57b97af1cc457c41a8463de617ebeff1ba34bcee1f982152533ce1be","observation_id":"c90b4de3-f838-46c3-b6be-409c8e704215","resolution":{"observed_at":"2026-08-02T09:19:08.088455Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"gr-qc/0404018","last_updated":"2004-09-03T23:18:29Z","snapshot_observed_at":"2026-07-07T03:19:04.182335Z","submitted_at":"2004-04-05T13:34:11Z","title":"Background Independent Quantum Gravity: A Status Report","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"gr-qc/0404018","snapshot_observed_at":"2026-08-02T09:19:08.252465Z","title":"Ashtekar and J","venue":null,"work_id":null,"year":2004},"citing_paper":{"arxiv_id":"2607.01274","last_updated":"2026-07-27T13:47:41Z","snapshot_observed_at":"2026-08-02T09:19:04.904084Z","submitted_at":"2026-06-30T22:28:24Z","title":"Inflation from Covariant Signature Change: A Geometric Mechanism","version":2},"reference_index":18,"source":"pdf_text","source_observed_at":"2026-08-02T09:19:08.252465Z"},"links":{"cited_paper":"/paper/gr-qc/0404018","citing_paper":"/paper/2607.01274"},"observation_digest":"sha256:3d01a8a1d26dec9fa5a98ec271d05051dcaa7e49424f2e663ec8de1f0ab78e26","observation_id":"4467937b-93b5-4c5b-a691-72ad63f96039","resolution":{"observed_at":"2026-08-02T09:19:08.252465Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1111.3535","last_updated":"2011-12-15T09:32:39Z","snapshot_observed_at":"2026-08-02T02:05:30.450995Z","submitted_at":"2011-11-15T14:35:03Z","title":"Anomaly-free scalar perturbations with holonomy corrections in loop quantum cosmology","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1111.3535","snapshot_observed_at":"2026-08-02T09:19:08.467159Z","title":"Cailleteau, J","venue":null,"work_id":null,"year":2012},"citing_paper":{"arxiv_id":"2607.01274","last_updated":"2026-07-27T13:47:41Z","snapshot_observed_at":"2026-08-02T09:19:04.904084Z","submitted_at":"2026-06-30T22:28:24Z","title":"Inflation from Covariant Signature Change: A Geometric Mechanism","version":2},"reference_index":19,"source":"pdf_text","source_observed_at":"2026-08-02T09:19:08.467159Z"},"links":{"cited_paper":"/paper/1111.3535","citing_paper":"/paper/2607.01274"},"observation_digest":"sha256:f66e797823b844d8ca1214e9568c4c31e4ab11dabf3e5f3ef7e547d695092175","observation_id":"7c126b5c-0932-40cf-acb9-79d33cd37e7e","resolution":{"observed_at":"2026-08-02T09:19:08.467159Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1702.05572","last_updated":"2017-02-26T01:44:41Z","snapshot_observed_at":"2026-08-06T00:59:02.994502Z","submitted_at":"2017-02-18T05:25:39Z","title":"How to Wick rotate generic curved spacetime","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1702.05572","snapshot_observed_at":"2026-08-02T09:19:08.645927Z","title":"Visser, arXiv:1702.05572 [gr-qc]","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2607.01274","last_updated":"2026-07-27T13:47:41Z","snapshot_observed_at":"2026-08-02T09:19:04.904084Z","submitted_at":"2026-06-30T22:28:24Z","title":"Inflation from Covariant Signature Change: A Geometric Mechanism","version":2},"reference_index":20,"source":"pdf_text","source_observed_at":"2026-08-02T09:19:08.645927Z"},"links":{"cited_paper":"/paper/1702.05572","citing_paper":"/paper/2607.01274"},"observation_digest":"sha256:9ac63136cead790684bb0c83bda806a2e0814a3139bdeb062b9f7b007621ea6e","observation_id":"724c3b70-7381-466f-938d-300d0ca5d4e2","resolution":{"observed_at":"2026-08-02T09:19:08.645927Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1510.07365","last_updated":"2015-10-26T05:28:21Z","snapshot_observed_at":"2026-08-02T13:11:12.987493Z","submitted_at":"2015-10-26T05:28:21Z","title":"Wick Rotation in the Tangent Space","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1510.07365","snapshot_observed_at":"2026-08-02T09:19:08.827809Z","title":"Samuel, Class","venue":null,"work_id":null,"year":2016},"citing_paper":{"arxiv_id":"2607.01274","last_updated":"2026-07-27T13:47:41Z","snapshot_observed_at":"2026-08-02T09:19:04.904084Z","submitted_at":"2026-06-30T22:28:24Z","title":"Inflation from Covariant Signature Change: A Geometric Mechanism","version":2},"reference_index":21,"source":"pdf_text","source_observed_at":"2026-08-02T09:19:08.827809Z"},"links":{"cited_paper":"/paper/1510.07365","citing_paper":"/paper/2607.01274"},"observation_digest":"sha256:5969cd9c0f85e022a36bf391cf2297bd7c83fd48ec5d0f8fd67078acbe31e050","observation_id":"6bb60103-6869-4de2-9dad-8a11f7808919","resolution":{"observed_at":"2026-08-02T09:19:08.827809Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1705.02504","last_updated":"2017-12-19T08:28:22Z","snapshot_observed_at":"2026-07-06T05:41:34.653013Z","submitted_at":"2017-05-06T16:42:33Z","title":"Action and Observer dependence in Euclidean quantum gravity","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1705.02504","snapshot_observed_at":"2026-08-02T09:19:08.971551Z","title":"Kothawala, Class","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2607.01274","last_updated":"2026-07-27T13:47:41Z","snapshot_observed_at":"2026-08-02T09:19:04.904084Z","submitted_at":"2026-06-30T22:28:24Z","title":"Inflation from Covariant Signature Change: A Geometric Mechanism","version":2},"reference_index":22,"source":"pdf_text","source_observed_at":"2026-08-02T09:19:08.971551Z"},"links":{"cited_paper":"/paper/1705.02504","citing_paper":"/paper/2607.01274"},"observation_digest":"sha256:3863d01584bf1c43a23c111ebb64fb3dfedcabb3ffa8b305b4139a110eb150c8","observation_id":"c7d841f8-419e-49b2-ab62-7070cf6fb650","resolution":{"observed_at":"2026-08-02T09:19:08.971551Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1802.07055","last_updated":"2018-06-27T05:31:08Z","snapshot_observed_at":"2026-07-06T06:24:20.288673Z","submitted_at":"2018-02-20T10:52:55Z","title":"Euclidean Action and the Einstein tensor","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1802.07055","snapshot_observed_at":"2026-08-02T09:19:09.084636Z","title":"Kothawala, Phys","venue":null,"work_id":null,"year":2018},"citing_paper":{"arxiv_id":"2607.01274","last_updated":"2026-07-27T13:47:41Z","snapshot_observed_at":"2026-08-02T09:19:04.904084Z","submitted_at":"2026-06-30T22:28:24Z","title":"Inflation from Covariant Signature Change: A Geometric Mechanism","version":2},"reference_index":23,"source":"pdf_text","source_observed_at":"2026-08-02T09:19:09.084636Z"},"links":{"cited_paper":"/paper/1802.07055","citing_paper":"/paper/2607.01274"},"observation_digest":"sha256:911cd457e246f48a0a4c07a34bbd6dee7e7b1f5ce11ed2adaaf0555283ae76b7","observation_id":"4771b55b-45a6-4fb3-bfde-85776a87d39f","resolution":{"observed_at":"2026-08-02T09:19:09.084636Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2010.01822","last_updated":"2021-07-01T17:39:01Z","snapshot_observed_at":"2026-07-06T10:01:26.447380Z","submitted_at":"2020-10-05T07:16:22Z","title":"Geometric aspects of covariant Wick rotation","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2010.01822","snapshot_observed_at":"2026-08-02T09:19:09.191479Z","title":"Singh and D","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2607.01274","last_updated":"2026-07-27T13:47:41Z","snapshot_observed_at":"2026-08-02T09:19:04.904084Z","submitted_at":"2026-06-30T22:28:24Z","title":"Inflation from Covariant Signature Change: A Geometric Mechanism","version":2},"reference_index":24,"source":"pdf_text","source_observed_at":"2026-08-02T09:19:09.191479Z"},"links":{"cited_paper":"/paper/2010.01822","citing_paper":"/paper/2607.01274"},"observation_digest":"sha256:c5781e77905bddf47da18a4092e4c44300e3d9c07b86acb9e78ef856da7b467d","observation_id":"9cddb22f-b76f-422b-80f0-7a5e9589bc97","resolution":{"observed_at":"2026-08-02T09:19:09.191479Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"gr-qc/0012099","last_updated":"2001-04-27T14:06:39Z","snapshot_observed_at":"2026-07-07T03:13:29.390303Z","submitted_at":"2000-12-27T16:01:43Z","title":"Signature Change on the Brane","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"gr-qc/0012099","snapshot_observed_at":"2026-08-02T09:19:09.281363Z","title":null,"venue":null,"work_id":null,"year":2001},"citing_paper":{"arxiv_id":"2607.01274","last_updated":"2026-07-27T13:47:41Z","snapshot_observed_at":"2026-08-02T09:19:04.904084Z","submitted_at":"2026-06-30T22:28:24Z","title":"Inflation from Covariant Signature Change: A Geometric Mechanism","version":2},"reference_index":25,"source":"pdf_text","source_observed_at":"2026-08-02T09:19:09.281363Z"},"links":{"cited_paper":"/paper/gr-qc/0012099","citing_paper":"/paper/2607.01274"},"observation_digest":"sha256:80a5ef5c4729379179a69bc0d0c72fe122afb69336b739a622ce3cd64f3e6d7c","observation_id":"b44a2ba0-0401-48e1-95d3-64d1ce755a9a","resolution":{"observed_at":"2026-08-02T09:19:09.281363Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0705.3380","last_updated":"2007-05-23T13:54:45Z","snapshot_observed_at":"2026-08-04T23:46:40.857223Z","submitted_at":"2007-05-23T13:54:45Z","title":"Lorentzian and signature changing branes","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0705.3380","snapshot_observed_at":"2026-08-02T09:19:09.472014Z","title":null,"venue":null,"work_id":null,"year":2007},"citing_paper":{"arxiv_id":"2607.01274","last_updated":"2026-07-27T13:47:41Z","snapshot_observed_at":"2026-08-02T09:19:04.904084Z","submitted_at":"2026-06-30T22:28:24Z","title":"Inflation from Covariant Signature Change: A Geometric Mechanism","version":2},"reference_index":26,"source":"pdf_text","source_observed_at":"2026-08-02T09:19:09.472014Z"},"links":{"cited_paper":"/paper/0705.3380","citing_paper":"/paper/2607.01274"},"observation_digest":"sha256:90be58a0bbc4ef068c54d964428966c46f4c053a403a74e50eb334f47ce5c9cb","observation_id":"9648dbba-7913-4e03-9b82-f7fbd9ef79c6","resolution":{"observed_at":"2026-08-02T09:19:09.472014Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0710.0820","last_updated":"2007-11-29T16:46:53Z","snapshot_observed_at":"2026-07-06T01:31:35.420762Z","submitted_at":"2007-10-03T15:41:11Z","title":"Is the accelerated expansion evidence of a forthcoming change of signature on the brane?","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0710.0820","snapshot_observed_at":"2026-08-02T09:19:09.648055Z","title":null,"venue":null,"work_id":null,"year":2008},"citing_paper":{"arxiv_id":"2607.01274","last_updated":"2026-07-27T13:47:41Z","snapshot_observed_at":"2026-08-02T09:19:04.904084Z","submitted_at":"2026-06-30T22:28:24Z","title":"Inflation from Covariant Signature Change: A Geometric Mechanism","version":2},"reference_index":27,"source":"pdf_text","source_observed_at":"2026-08-02T09:19:09.648055Z"},"links":{"cited_paper":"/paper/0710.0820","citing_paper":"/paper/2607.01274"},"observation_digest":"sha256:0f2cd54012aaf93d033362dc219ea8d7c174eab961b45798619f227e324cb69d","observation_id":"a8031e6f-2775-4b0c-99f0-051a446fc151","resolution":{"observed_at":"2026-08-02T09:19:09.648055Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0712.1462","last_updated":"2007-12-10T16:31:47Z","snapshot_observed_at":"2026-07-06T01:36:35.133583Z","submitted_at":"2007-12-10T16:31:47Z","title":"Accelerating expansion and change of signature","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0712.1462","snapshot_observed_at":"2026-08-02T09:19:09.828573Z","title":null,"venue":null,"work_id":null,"year":2008},"citing_paper":{"arxiv_id":"2607.01274","last_updated":"2026-07-27T13:47:41Z","snapshot_observed_at":"2026-08-02T09:19:04.904084Z","submitted_at":"2026-06-30T22:28:24Z","title":"Inflation from Covariant Signature Change: A Geometric Mechanism","version":2},"reference_index":28,"source":"pdf_text","source_observed_at":"2026-08-02T09:19:09.828573Z"},"links":{"cited_paper":"/paper/0712.1462","citing_paper":"/paper/2607.01274"},"observation_digest":"sha256:48817f5049f5ae76ef45a25eb63bd003537d9578c7a82920a59471920e173241","observation_id":"7b8e318d-bb7a-416a-a65a-4f746d9e6b07","resolution":{"observed_at":"2026-08-02T09:19:09.828573Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-02T09:19:10.027780Z","title":null,"venue":null,"work_id":null,"year":1992},"citing_paper":{"arxiv_id":"2607.01274","last_updated":"2026-07-27T13:47:41Z","snapshot_observed_at":"2026-08-02T09:19:04.904084Z","submitted_at":"2026-06-30T22:28:24Z","title":"Inflation from Covariant Signature Change: A Geometric Mechanism","version":2},"reference_index":29,"source":"pdf_text","source_observed_at":"2026-08-02T09:19:10.027780Z"},"links":{"citing_paper":"/paper/2607.01274"},"observation_digest":"sha256:ea7ae3e30a683c929de396d3894bdfbf4bab777e930df1edd0af989a53822a44","observation_id":"f09f3df3-349c-4f8f-9d88-9bcd9b2aba40","resolution":{"observed_at":"2026-08-02T09:19:10.027780Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2111.06095","last_updated":"2022-09-12T06:00:59Z","snapshot_observed_at":"2026-08-03T15:14:28.944948Z","submitted_at":"2021-11-11T08:12:25Z","title":"Dynamical signature: complex manifolds, gauge fields and non-flat tangent space","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2111.06095","snapshot_observed_at":"2026-08-02T09:19:10.177889Z","title":"Bondarenko, Universe8, 497 (2022), arXiv:2111.06095 15 [gr-qc]","venue":null,"work_id":null,"year":2022},"citing_paper":{"arxiv_id":"2607.01274","last_updated":"2026-07-27T13:47:41Z","snapshot_observed_at":"2026-08-02T09:19:04.904084Z","submitted_at":"2026-06-30T22:28:24Z","title":"Inflation from Covariant Signature Change: A Geometric Mechanism","version":2},"reference_index":30,"source":"pdf_text","source_observed_at":"2026-08-02T09:19:10.177889Z"},"links":{"cited_paper":"/paper/2111.06095","citing_paper":"/paper/2607.01274"},"observation_digest":"sha256:3b242a610c33f817dbe6d16a4d6a83d94aa929813d714f2cf60b7384b1244a7a","observation_id":"2b7ce0f9-2092-44fb-8d8d-6b228505ef96","resolution":{"observed_at":"2026-08-02T09:19:10.177889Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-02T09:19:10.303167Z","title":"Embacher, Physical Review D51, 6764 (1995)","venue":null,"work_id":null,"year":1995},"citing_paper":{"arxiv_id":"2607.01274","last_updated":"2026-07-27T13:47:41Z","snapshot_observed_at":"2026-08-02T09:19:04.904084Z","submitted_at":"2026-06-30T22:28:24Z","title":"Inflation from Covariant Signature Change: A Geometric Mechanism","version":2},"reference_index":31,"source":"pdf_text","source_observed_at":"2026-08-02T09:19:10.303167Z"},"links":{"citing_paper":"/paper/2607.01274"},"observation_digest":"sha256:82baba3a00b572fc43a5d08b3a5ab843d8beef7f28a77d7ecc82652203c4bec9","observation_id":"a30fd71f-8790-4324-a0d1-d3c0c635c2d6","resolution":{"observed_at":"2026-08-02T09:19:10.303167Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1812.01760","last_updated":"2018-12-05T00:23:59Z","snapshot_observed_at":"2026-07-06T07:19:11.957225Z","submitted_at":"2018-12-05T00:23:59Z","title":"What is the No-Boundary Wave Function of the Universe?","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1812.01760","snapshot_observed_at":"2026-08-02T09:19:10.431987Z","title":null,"venue":null,"work_id":null,"year":2019},"citing_paper":{"arxiv_id":"2607.01274","last_updated":"2026-07-27T13:47:41Z","snapshot_observed_at":"2026-08-02T09:19:04.904084Z","submitted_at":"2026-06-30T22:28:24Z","title":"Inflation from Covariant Signature Change: A Geometric Mechanism","version":2},"reference_index":32,"source":"pdf_text","source_observed_at":"2026-08-02T09:19:10.431987Z"},"links":{"cited_paper":"/paper/1812.01760","citing_paper":"/paper/2607.01274"},"observation_digest":"sha256:94e295f7f7c5abcf39f2d69a30801313a425ce5133a69d28fe84e5dc54c8cef0","observation_id":"33bca9d2-4244-4b69-9242-ce6d40365518","resolution":{"observed_at":"2026-08-02T09:19:10.431987Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"paper":{"arxiv_id":"2607.01274","last_updated":"2026-07-27T13:47:41Z","latest_version":2,"primary_category":"gr-qc","snapshot_observed_at":"2026-08-02T09:19:04.904084Z","submitted_at":"2026-06-30T22:28:24Z","title":"Inflation from Covariant Signature Change: A Geometric Mechanism"},"reference_resolution":{"displayed":32,"state_counts":{"malformed_identifier":0,"metadata_mismatch":0,"parse_uncertain":0,"unresolved":32,"verified_exact":0,"verified_fuzzy":0},"total_outbound_references":32},"refusal":"A citation records a reference. It does not transfer a finding from one paper to another.","schema":"pith.paper-citation-record.v1","standing_sources":[{"observed_at":"2026-08-08T06:32:00.761636+00:00","source":"crossref"},{"observed_at":"2026-08-08T06:31:55.24221+00:00","source":"retraction_watch"}],"thesis":"As of 8 August 2026, this Paper Citation Record lists 32 of 32 outbound references and 0 inbound Pith citation observations for arXiv:2607.01274."}