{"as_of":"2026-08-10T03:18:00Z","caps":{"database_statements":6,"inbound":100,"outbound":100},"context_digest":"sha256:75626c70e3d03a75174d2f5a8a870cd4a0b9d0d844a788c49e18852ae38d72de","coverage":[{"denominator":48,"lane":"reference_resolution","note":"Typed states for the displayed outbound observations.","records_observed":48,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-06T11:19:55.961212Z","state":"measured"},{"denominator":50,"lane":"standing_notices","note":"One-hop event checks from named stored sources.","records_observed":50,"source":"scholarly_work_events, retraction_status_cache","source_observed_at":"2026-08-09T06:31:02.800959+00:00","state":"measured"},{"denominator":2,"lane":"inbound_itemization","note":"Pith citing papers itemized under the disclosed page cap.","records_observed":2,"source":"paper_references, paper_reference_links","source_observed_at":"2026-08-03T08:35:14.903517Z","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":[{"citation":{"cited_paper":{"arxiv_id":"2507.22980","last_updated":"2025-07-30T18:00:01Z","snapshot_observed_at":"2026-08-07T23:42:10.881444Z","submitted_at":"2025-07-30T18:00:01Z","title":"Hidden Sector Custodial Naturalness","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2507.22980","snapshot_observed_at":"2026-08-03T08:35:14.903517Z","title":"de Boer, M","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2601.16731","last_updated":"2026-07-25T14:22:53Z","snapshot_observed_at":"2026-08-08T09:37:48.937203Z","submitted_at":"2026-01-23T13:28:55Z","title":"Fermi scale from quantum gravity scaling solution","version":2},"reference_index":16,"source":"pdf_text","source_observed_at":"2026-08-03T08:35:14.903517Z"},"links":{"cited_paper":"/paper/2507.22980","citing_paper":"/paper/2601.16731"},"observation_digest":"sha256:8c92f5d335a28adeed32918b1379ca8b7d9012e1d46a6a23e5f6900048df6b1b","observation_id":"2a388a91-d935-4b8e-957f-841b6cc3c841","resolution":{"observed_at":"2026-08-03T08:35:14.903517Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2507.22980","last_updated":"2025-07-30T18:00:01Z","snapshot_observed_at":"2026-08-07T23:42:10.881444Z","submitted_at":"2025-07-30T18:00:01Z","title":"Hidden Sector Custodial Naturalness","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2507.22980","snapshot_observed_at":"2026-08-02T23:26:29.022092Z","title":"de Boer, M","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2602.14115","last_updated":"2026-07-07T23:28:15Z","snapshot_observed_at":"2026-08-09T00:32:07.759569Z","submitted_at":"2026-02-15T12:31:44Z","title":"Scale invariant radiative neutrino mass model","version":2},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-08-02T23:26:29.022092Z"},"links":{"cited_paper":"/paper/2507.22980","citing_paper":"/paper/2602.14115"},"observation_digest":"sha256:672676ce0f94374c0fc09f78fef9d2c329eea026e49d977e91eb172088970410","observation_id":"460011ba-e977-42ce-85c6-9646cc615fc5","resolution":{"observed_at":"2026-08-02T23:26:29.022092Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"links":{"evidence":"/evidence","html":"/paper/2507.22980/citation-record","integrity":"/paper/2507.22980/integrity","json":"/paper/2507.22980/citation-record.json","paper":"/paper/2507.22980"},"outbound":[{"citation":{"cited_paper":{"arxiv_id":"2506.05472","last_updated":"2026-05-05T16:05:57Z","snapshot_observed_at":"2026-08-02T05:55:53.417755Z","submitted_at":"2025-06-05T18:00:06Z","title":"The Intrinsic and Extrinsic Hierarchy Problems","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2506.05472","snapshot_observed_at":"2026-08-06T11:19:53.840021Z","title":"The Intrinsic and Extrinsic Hierarchy Problems,","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2507.22980","last_updated":"2025-07-30T18:00:01Z","snapshot_observed_at":"2026-08-07T23:42:10.881444Z","submitted_at":"2025-07-30T18:00:01Z","title":"Hidden Sector Custodial Naturalness","version":1},"reference_index":1,"source":"pdf_text","source_observed_at":"2026-08-06T11:19:53.840021Z"},"links":{"cited_paper":"/paper/2506.05472","citing_paper":"/paper/2507.22980"},"observation_digest":"sha256:de784173877d9af2b51130968c790238c8fc7c84850eead9f3899e5c640b9f05","observation_id":"9f355110-9ea3-4799-a40d-8dda46bde99a","resolution":{"observed_at":"2026-08-06T11:19:53.840021Z","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":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-06T11:19:57.359546Z","title":"On naturalness in the standard model,","venue":null,"work_id":"cd01425e-3eec-451b-aa47-45841d35e484","year":1995},"citing_paper":{"arxiv_id":"2507.22980","last_updated":"2025-07-30T18:00:01Z","snapshot_observed_at":"2026-08-07T23:42:10.881444Z","submitted_at":"2025-07-30T18:00:01Z","title":"Hidden Sector Custodial Naturalness","version":1},"reference_index":2,"source":"pdf_text","source_observed_at":"2026-08-06T11:19:53.846716Z"},"links":{"citing_paper":"/paper/2507.22980"},"observation_digest":"sha256:78d7f78242e0c7da1fedf3fe882b2d0cb112cec83e581f1f4b42c1378e364815","observation_id":"a28eace1-f886-43ae-8202-28ee3a0ea7e9","resolution":{"observed_at":"2026-08-06T11:19:57.364862Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-06T11:19:57.341181Z","title":"Radiative Corrections as the Origin of Spontaneous Symmetry Breaking,","venue":null,"work_id":"306b1e66-99d1-4702-a352-3b1585b4f5e4","year":1973},"citing_paper":{"arxiv_id":"2507.22980","last_updated":"2025-07-30T18:00:01Z","snapshot_observed_at":"2026-08-07T23:42:10.881444Z","submitted_at":"2025-07-30T18:00:01Z","title":"Hidden Sector Custodial Naturalness","version":1},"reference_index":3,"source":"pdf_text","source_observed_at":"2026-08-06T11:19:53.852070Z"},"links":{"citing_paper":"/paper/2507.22980"},"observation_digest":"sha256:db58f06354644be702bef452a4d961301fc6ab80a2eb7cc35b777943d4598095","observation_id":"3bc1589a-c2ac-413c-88d8-7ff95ff4d21e","resolution":{"observed_at":"2026-08-06T11:19:57.346435Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1904.05237","last_updated":"2020-10-05T13:32:05Z","snapshot_observed_at":"2026-08-06T16:00:19.010291Z","submitted_at":"2019-04-10T15:15:14Z","title":"Measurement of $\\mathrm{t\\bar t}$ normalised multi-differential cross sections in pp collisions at $\\sqrt{s} =13$ TeV, and simultaneous determination of the strong coupling strength, top quark pole mass, and parton distribution functions","version":2},"cited_work":{"arxiv_id":"1904.05237","doi":null,"metadata_source":"pith","pith_arxiv_id":"1904.05237","snapshot_observed_at":"2026-08-06T11:19:57.241631Z","title":"Measurement of $\\mathrm{t\\bar t}$ normalised multi-differential cross sections in pp collisions at $\\sqrt{s} =13$ TeV, and simultaneous determination of the strong coupling strength, top quark pole mass, and parton distribution functions","venue":"hep-ex","work_id":"52969350-b7df-44d9-8210-c1f5c9096270","year":2019},"citing_paper":{"arxiv_id":"2507.22980","last_updated":"2025-07-30T18:00:01Z","snapshot_observed_at":"2026-08-07T23:42:10.881444Z","submitted_at":"2025-07-30T18:00:01Z","title":"Hidden Sector Custodial Naturalness","version":1},"reference_index":4,"source":"pdf_text","source_observed_at":"2026-08-06T11:19:53.858860Z"},"links":{"cited_paper":"/paper/1904.05237","citing_paper":"/paper/2507.22980"},"observation_digest":"sha256:54cca4d886dca6a1d42b27174c53f6f91300f4cbe63df998ac77493b390cd6e0","observation_id":"9bfaa05d-ca85-457c-a5ab-4e0e83866362","resolution":{"observed_at":"2026-08-06T11:19:57.247103Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-06T11:19:53.864430Z","title":"Vacuum stability in the Standard Model and beyond,","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2507.22980","last_updated":"2025-07-30T18:00:01Z","snapshot_observed_at":"2026-08-07T23:42:10.881444Z","submitted_at":"2025-07-30T18:00:01Z","title":"Hidden Sector Custodial Naturalness","version":1},"reference_index":5,"source":"pdf_text","source_observed_at":"2026-08-06T11:19:53.864430Z"},"links":{"citing_paper":"/paper/2507.22980"},"observation_digest":"sha256:dc4ae56f5d12271dec300519a0db9159ccd1bb4acb6849ff2b344e6674fdfd0b","observation_id":"59bdb028-75f8-49db-90fa-609852645f3a","resolution":{"observed_at":"2026-08-06T11:19:53.864430Z","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":"2026-08-06T11:19:53.873307Z","title":"The quantum criticality of the Standard Model and the hierarchy problem,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2507.22980","last_updated":"2025-07-30T18:00:01Z","snapshot_observed_at":"2026-08-07T23:42:10.881444Z","submitted_at":"2025-07-30T18:00:01Z","title":"Hidden Sector Custodial Naturalness","version":1},"reference_index":6,"source":"pdf_text","source_observed_at":"2026-08-06T11:19:53.873307Z"},"links":{"citing_paper":"/paper/2507.22980"},"observation_digest":"sha256:3058660efdc8f4c36409d11075e125fc2c187ddad1ad10624a7a048417a62df4","observation_id":"b080fca6-1a62-42b4-b015-580eee299828","resolution":{"observed_at":"2026-08-06T11:19:53.873307Z","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":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-06T11:19:57.324927Z","title":"Mass of the Higgs Boson,","venue":null,"work_id":"2761326d-fad1-4969-9532-6d964d16b059","year":1976},"citing_paper":{"arxiv_id":"2507.22980","last_updated":"2025-07-30T18:00:01Z","snapshot_observed_at":"2026-08-07T23:42:10.881444Z","submitted_at":"2025-07-30T18:00:01Z","title":"Hidden Sector Custodial Naturalness","version":1},"reference_index":7,"source":"pdf_text","source_observed_at":"2026-08-06T11:19:53.888642Z"},"links":{"citing_paper":"/paper/2507.22980"},"observation_digest":"sha256:9ffa147b2141a3f194205d92299fe5161ef52802515b783686bc90f5350e49e0","observation_id":"090a4818-3065-4537-b4ed-d970eb6580a7","resolution":{"observed_at":"2026-08-06T11:19:57.330129Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-06T11:19:57.307572Z","title":"Symmetry Breaking and Scalar Bosons,","venue":null,"work_id":"ebbef0ae-74cf-4148-9200-93c07e77fd22","year":1976},"citing_paper":{"arxiv_id":"2507.22980","last_updated":"2025-07-30T18:00:01Z","snapshot_observed_at":"2026-08-07T23:42:10.881444Z","submitted_at":"2025-07-30T18:00:01Z","title":"Hidden Sector Custodial Naturalness","version":1},"reference_index":8,"source":"pdf_text","source_observed_at":"2026-08-06T11:19:53.899418Z"},"links":{"citing_paper":"/paper/2507.22980"},"observation_digest":"sha256:922c845f12734909cba0f4c224d02be2409776312ad2a73fe8907df40af8283f","observation_id":"8e28162a-3f18-487e-9828-f9a7f8d0e6b0","resolution":{"observed_at":"2026-08-06T11:19:57.313261Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/9604278","last_updated":"1996-04-11T15:14:52Z","snapshot_observed_at":"2026-07-07T04:22:24.348335Z","submitted_at":"1996-04-10T07:33:44Z","title":"The Next-to-Minimal Coleman-Weinberg Model","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/9604278","snapshot_observed_at":"2026-08-06T11:19:53.909536Z","title":"The Next-to-minimal Coleman-Weinberg model,","venue":null,"work_id":null,"year":1996},"citing_paper":{"arxiv_id":"2507.22980","last_updated":"2025-07-30T18:00:01Z","snapshot_observed_at":"2026-08-07T23:42:10.881444Z","submitted_at":"2025-07-30T18:00:01Z","title":"Hidden Sector Custodial Naturalness","version":1},"reference_index":9,"source":"pdf_text","source_observed_at":"2026-08-06T11:19:53.909536Z"},"links":{"cited_paper":"/paper/hep-ph/9604278","citing_paper":"/paper/2507.22980"},"observation_digest":"sha256:3202457efa881d97c3b76c458b347c4a5311a9cc898f075ae23427699e3fca72","observation_id":"527ea633-dddd-408a-ad03-f3fa94eabb4f","resolution":{"observed_at":"2026-08-06T11:19:53.909536Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-th/0612165","last_updated":"2007-03-26T18:33:59Z","snapshot_observed_at":"2026-08-10T01:16:58.704764Z","submitted_at":"2006-12-15T19:34:12Z","title":"Conformal Symmetry and the Standard Model","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-th/0612165","snapshot_observed_at":"2026-08-06T11:19:53.918803Z","title":"Conformal Symmetry and the Standard Model,","venue":null,"work_id":null,"year":2007},"citing_paper":{"arxiv_id":"2507.22980","last_updated":"2025-07-30T18:00:01Z","snapshot_observed_at":"2026-08-07T23:42:10.881444Z","submitted_at":"2025-07-30T18:00:01Z","title":"Hidden Sector Custodial Naturalness","version":1},"reference_index":10,"source":"pdf_text","source_observed_at":"2026-08-06T11:19:53.918803Z"},"links":{"cited_paper":"/paper/hep-th/0612165","citing_paper":"/paper/2507.22980"},"observation_digest":"sha256:7d943802a3dcfbb00dbcd773e14bbe630abebda08b409f21316a211b129b3ddd","observation_id":"a3164928-b9a4-410a-b566-b1301f9678e4","resolution":{"observed_at":"2026-08-06T11:19:53.918803Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0701145","last_updated":"2007-01-18T14:18:24Z","snapshot_observed_at":"2026-07-07T04:13:36.473155Z","submitted_at":"2007-01-18T14:18:24Z","title":"Novel Effects in Electroweak Breaking from a Hidden Sector","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0701145","snapshot_observed_at":"2026-08-06T11:19:53.928506Z","title":"Novel Effects in Electroweak Breaking from a Hidden Sector,","venue":null,"work_id":null,"year":2007},"citing_paper":{"arxiv_id":"2507.22980","last_updated":"2025-07-30T18:00:01Z","snapshot_observed_at":"2026-08-07T23:42:10.881444Z","submitted_at":"2025-07-30T18:00:01Z","title":"Hidden Sector Custodial Naturalness","version":1},"reference_index":11,"source":"pdf_text","source_observed_at":"2026-08-06T11:19:53.928506Z"},"links":{"cited_paper":"/paper/hep-ph/0701145","citing_paper":"/paper/2507.22980"},"observation_digest":"sha256:c9bdb82d0676bd51a97a012eb0f32898e9cccc0a73c48784850632b7da38d763","observation_id":"23fd999f-a6d2-46c7-afc2-f209392534eb","resolution":{"observed_at":"2026-08-06T11:19:53.928506Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"hep-ph/0701254","last_updated":"2007-01-30T19:27:08Z","snapshot_observed_at":"2026-07-07T04:13:41.297122Z","submitted_at":"2007-01-30T19:27:08Z","title":"Shadow Higgs from a scale-invariant hidden $U(1)_s$ model","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"hep-ph/0701254","snapshot_observed_at":"2026-08-06T11:19:53.938278Z","title":"Shadow Higgs from a scale-invariant hidden U(1)(s) model,","venue":null,"work_id":null,"year":2007},"citing_paper":{"arxiv_id":"2507.22980","last_updated":"2025-07-30T18:00:01Z","snapshot_observed_at":"2026-08-07T23:42:10.881444Z","submitted_at":"2025-07-30T18:00:01Z","title":"Hidden Sector Custodial Naturalness","version":1},"reference_index":12,"source":"pdf_text","source_observed_at":"2026-08-06T11:19:53.938278Z"},"links":{"cited_paper":"/paper/hep-ph/0701254","citing_paper":"/paper/2507.22980"},"observation_digest":"sha256:ad1aa834487e3f66552ac79d39d59cead174fdf1ce4bb782ff31921158c6b7a5","observation_id":"d974d973-481d-4a8f-b8f5-2fd8e287d609","resolution":{"observed_at":"2026-08-06T11:19:53.938278Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0704.1165","last_updated":"2007-09-23T02:29:05Z","snapshot_observed_at":"2026-07-06T01:26:00.785058Z","submitted_at":"2007-04-09T23:41:24Z","title":"Electroweak Higgs as a pseudo-Goldstone boson of broken scale invariance","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0704.1165","snapshot_observed_at":"2026-08-06T11:19:53.949128Z","title":"Electroweak Higgs as a pseudo-Goldstone boson of broken scale invariance,","venue":null,"work_id":null,"year":2007},"citing_paper":{"arxiv_id":"2507.22980","last_updated":"2025-07-30T18:00:01Z","snapshot_observed_at":"2026-08-07T23:42:10.881444Z","submitted_at":"2025-07-30T18:00:01Z","title":"Hidden Sector Custodial Naturalness","version":1},"reference_index":13,"source":"pdf_text","source_observed_at":"2026-08-06T11:19:53.949128Z"},"links":{"cited_paper":"/paper/0704.1165","citing_paper":"/paper/2507.22980"},"observation_digest":"sha256:114f128a6ece6bad852da4b8f26b30b82c5b1c461626cc699473b1a9daa5bdd3","observation_id":"e165dfeb-a9de-4261-8bce-37064d8ea9f0","resolution":{"observed_at":"2026-08-06T11:19:53.949128Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0902.4050","last_updated":"2009-04-17T00:48:32Z","snapshot_observed_at":"2026-08-08T04:23:05.391028Z","submitted_at":"2009-02-24T01:45:26Z","title":"Classically Conformal B-L extended Standard Model","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0902.4050","snapshot_observed_at":"2026-08-06T11:19:53.958636Z","title":"Classically conformal B − L extended Standard Model,","venue":null,"work_id":null,"year":2009},"citing_paper":{"arxiv_id":"2507.22980","last_updated":"2025-07-30T18:00:01Z","snapshot_observed_at":"2026-08-07T23:42:10.881444Z","submitted_at":"2025-07-30T18:00:01Z","title":"Hidden Sector Custodial Naturalness","version":1},"reference_index":14,"source":"pdf_text","source_observed_at":"2026-08-06T11:19:53.958636Z"},"links":{"cited_paper":"/paper/0902.4050","citing_paper":"/paper/2507.22980"},"observation_digest":"sha256:7b8f5c12d7155cbbc126667898fc08d40389f8546b318d24bbd8496afced896c","observation_id":"37ea93a8-34c7-410c-aa23-eaf1dd3de21a","resolution":{"observed_at":"2026-08-06T11:19:53.958636Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0911.0710","last_updated":"2010-09-14T12:20:27Z","snapshot_observed_at":"2026-07-06T02:03:37.088756Z","submitted_at":"2009-11-03T23:29:36Z","title":"Radiative Symmetry Breaking of the Minimal Left-Right Symmetric Model","version":2},"cited_work":{"arxiv_id":"0911.0710","doi":null,"metadata_source":"pith","pith_arxiv_id":"0911.0710","snapshot_observed_at":"2026-08-06T11:19:56.963306Z","title":"Radiative Symmetry Breaking of the Minimal Left-Right Symmetric Model","venue":"hep-ph","work_id":"e2529da7-6a0a-4767-a631-e13124e2f9b7","year":2009},"citing_paper":{"arxiv_id":"2507.22980","last_updated":"2025-07-30T18:00:01Z","snapshot_observed_at":"2026-08-07T23:42:10.881444Z","submitted_at":"2025-07-30T18:00:01Z","title":"Hidden Sector Custodial Naturalness","version":1},"reference_index":15,"source":"pdf_text","source_observed_at":"2026-08-06T11:19:53.968108Z"},"links":{"cited_paper":"/paper/0911.0710","citing_paper":"/paper/2507.22980"},"observation_digest":"sha256:7b7b6d4d3d4a2b1d6596cf1c31b1d2031a2d4a60a85efbbda90e3912cbb45771","observation_id":"51225ab2-2ecd-498f-a599-47bbc3cdd769","resolution":{"observed_at":"2026-08-06T11:19:56.968088Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1308.0295","last_updated":"2013-10-01T18:02:27Z","snapshot_observed_at":"2026-07-06T03:19:47.291095Z","submitted_at":"2013-08-01T18:40:30Z","title":"Natural Electroweak Symmetry Breaking from Scale Invariant Higgs Mechanism","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1308.0295","snapshot_observed_at":"2026-08-06T11:19:53.978135Z","title":"Natural Electroweak Symmetry Breaking from Scale Invariant Higgs Mechanism,","venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"2507.22980","last_updated":"2025-07-30T18:00:01Z","snapshot_observed_at":"2026-08-07T23:42:10.881444Z","submitted_at":"2025-07-30T18:00:01Z","title":"Hidden Sector Custodial Naturalness","version":1},"reference_index":16,"source":"pdf_text","source_observed_at":"2026-08-06T11:19:53.978135Z"},"links":{"cited_paper":"/paper/1308.0295","citing_paper":"/paper/2507.22980"},"observation_digest":"sha256:c7c028b6ad3ea2faf22cbe08d762e31b24fbdedfac0f44c77725f6b7ecd7675e","observation_id":"c0dcf20a-52d9-4d5a-bd04-c0032045f5bf","resolution":{"observed_at":"2026-08-06T11:19:53.978135Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1401.4185","last_updated":"2014-01-27T17:50:15Z","snapshot_observed_at":"2026-07-06T03:33:32.934187Z","submitted_at":"2014-01-16T21:35:22Z","title":"Is the Higgs Boson Associated with Coleman-Weinberg Dynamical Symmetry Breaking?","version":2},"cited_work":{"arxiv_id":"1401.4185","doi":null,"metadata_source":"pith","pith_arxiv_id":"1401.4185","snapshot_observed_at":"2026-08-06T11:19:56.922136Z","title":"Is the Higgs Boson Associated with Coleman-Weinberg Dynamical Symmetry Breaking?","venue":"hep-ph","work_id":"4f158c37-5ea5-44f7-847b-dd5402e68ec2","year":2014},"citing_paper":{"arxiv_id":"2507.22980","last_updated":"2025-07-30T18:00:01Z","snapshot_observed_at":"2026-08-07T23:42:10.881444Z","submitted_at":"2025-07-30T18:00:01Z","title":"Hidden Sector Custodial Naturalness","version":1},"reference_index":17,"source":"pdf_text","source_observed_at":"2026-08-06T11:19:53.987032Z"},"links":{"cited_paper":"/paper/1401.4185","citing_paper":"/paper/2507.22980"},"observation_digest":"sha256:24ecd3266f40d1da7175b9cdf04e12ced74323ff5707e3afbdf02358be458644","observation_id":"6f5661aa-8deb-4102-9cc7-93129f76e256","resolution":{"observed_at":"2026-08-06T11:19:56.928060Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1408.3429","last_updated":"2014-08-14T21:02:49Z","snapshot_observed_at":"2026-07-06T03:51:46.310434Z","submitted_at":"2014-08-14T21:02:49Z","title":"Light Dark Matter, Naturalness, and the Radiative Origin of the Electroweak Scale","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1408.3429","snapshot_observed_at":"2026-08-06T11:19:53.998361Z","title":"Light Dark Matter, Naturalness, and the Radiative Origin of the Electroweak Scale,","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2507.22980","last_updated":"2025-07-30T18:00:01Z","snapshot_observed_at":"2026-08-07T23:42:10.881444Z","submitted_at":"2025-07-30T18:00:01Z","title":"Hidden Sector Custodial Naturalness","version":1},"reference_index":18,"source":"pdf_text","source_observed_at":"2026-08-06T11:19:53.998361Z"},"links":{"cited_paper":"/paper/1408.3429","citing_paper":"/paper/2507.22980"},"observation_digest":"sha256:83af06987c56c457f171eb253e1cec0597185e11f75273d1b353eac74ca3ed71","observation_id":"613b717e-f4f0-4644-bc8a-24aa02da967f","resolution":{"observed_at":"2026-08-06T11:19:53.998361Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2407.15920","last_updated":"2025-01-09T13:09:51Z","snapshot_observed_at":"2026-07-06T18:50:17.892140Z","submitted_at":"2024-07-22T18:00:01Z","title":"Electroweak hierarchy from conformal and custodial symmetry","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2407.15920","snapshot_observed_at":"2026-08-06T11:19:54.008463Z","title":"Electroweak hierarchy from conformal and custodial symmetry,","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2507.22980","last_updated":"2025-07-30T18:00:01Z","snapshot_observed_at":"2026-08-07T23:42:10.881444Z","submitted_at":"2025-07-30T18:00:01Z","title":"Hidden Sector Custodial Naturalness","version":1},"reference_index":19,"source":"pdf_text","source_observed_at":"2026-08-06T11:19:54.008463Z"},"links":{"cited_paper":"/paper/2407.15920","citing_paper":"/paper/2507.22980"},"observation_digest":"sha256:16402f213491e254dac44dcde30ce67e08a12a1c0f98e9c2fe3e3e9170de5b0e","observation_id":"4d0145d1-f9fd-4a6f-bda6-35ac1f504c49","resolution":{"observed_at":"2026-08-06T11:19:54.008463Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2502.09699","last_updated":"2025-04-28T09:41:56Z","snapshot_observed_at":"2026-08-09T17:36:02.914809Z","submitted_at":"2025-02-13T19:00:00Z","title":"Custodial Naturalness","version":2},"cited_work":{"arxiv_id":"2502.09699","doi":null,"metadata_source":"pith","pith_arxiv_id":"2502.09699","snapshot_observed_at":"2026-08-06T11:19:56.866266Z","title":"Custodial Naturalness","venue":"hep-ph","work_id":"cfe0a3d8-2d97-40b4-9fbf-b73d2296d945","year":2025},"citing_paper":{"arxiv_id":"2507.22980","last_updated":"2025-07-30T18:00:01Z","snapshot_observed_at":"2026-08-07T23:42:10.881444Z","submitted_at":"2025-07-30T18:00:01Z","title":"Hidden Sector Custodial Naturalness","version":1},"reference_index":20,"source":"pdf_text","source_observed_at":"2026-08-06T11:19:54.021752Z"},"links":{"cited_paper":"/paper/2502.09699","citing_paper":"/paper/2507.22980"},"observation_digest":"sha256:d86224092cd3a0ac20bcf050abea53370e413247782b0d022fcabfed639c92da","observation_id":"61761f64-3c66-4e65-9283-b21fbb3c790b","resolution":{"observed_at":"2026-08-06T11:19:56.871521Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1112.2696","last_updated":"2012-03-05T21:19:59Z","snapshot_observed_at":"2026-07-06T02:39:14.897428Z","submitted_at":"2011-12-12T20:59:46Z","title":"Dark Matter in Classically Scale-Invariant Two Singlets Standard Model","version":2},"cited_work":{"arxiv_id":"1112.2696","doi":null,"metadata_source":"pith","pith_arxiv_id":"1112.2696","snapshot_observed_at":"2026-08-06T11:19:56.844588Z","title":"Dark Matter in Classically Scale-Invariant Two Singlets Standard Model","venue":"hep-ph","work_id":"addba580-5048-4808-a6eb-842aa06911df","year":2011},"citing_paper":{"arxiv_id":"2507.22980","last_updated":"2025-07-30T18:00:01Z","snapshot_observed_at":"2026-08-07T23:42:10.881444Z","submitted_at":"2025-07-30T18:00:01Z","title":"Hidden Sector Custodial Naturalness","version":1},"reference_index":21,"source":"pdf_text","source_observed_at":"2026-08-06T11:19:54.032592Z"},"links":{"cited_paper":"/paper/1112.2696","citing_paper":"/paper/2507.22980"},"observation_digest":"sha256:35a4e6984bb8888cdcb6f449b20a2b85fd499a5249c43da86dc33c66ae61ca53","observation_id":"5bf389d1-635a-4f7d-ae00-795f9c904921","resolution":{"observed_at":"2026-08-06T11:19:56.849456Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2204.01744","last_updated":"2022-04-04T18:00:01Z","snapshot_observed_at":"2026-08-04T04:35:07.729872Z","submitted_at":"2022-04-04T18:00:01Z","title":"Dark Matter-Induced Multi-Phase Dynamical Symmetry Breaking","version":1},"cited_work":{"arxiv_id":"2204.01744","doi":null,"metadata_source":"pith","pith_arxiv_id":"2204.01744","snapshot_observed_at":"2026-08-06T11:19:56.821983Z","title":"Dark Matter-Induced Multi-Phase Dynamical Symmetry Breaking","venue":"hep-ph","work_id":"6b708a30-81a0-407b-805b-57078da507ee","year":2022},"citing_paper":{"arxiv_id":"2507.22980","last_updated":"2025-07-30T18:00:01Z","snapshot_observed_at":"2026-08-07T23:42:10.881444Z","submitted_at":"2025-07-30T18:00:01Z","title":"Hidden Sector Custodial Naturalness","version":1},"reference_index":22,"source":"pdf_text","source_observed_at":"2026-08-06T11:19:54.041613Z"},"links":{"cited_paper":"/paper/2204.01744","citing_paper":"/paper/2507.22980"},"observation_digest":"sha256:271a886b5a41261954db1c0e6f8570de31cc5c20d86f321ceb5629d905016399","observation_id":"322bfeb9-957b-4a81-bf73-e29aa67b6247","resolution":{"observed_at":"2026-08-06T11:19:56.827236Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2102.01084","last_updated":"2021-03-19T13:02:53Z","snapshot_observed_at":"2026-08-03T16:15:16.095844Z","submitted_at":"2021-02-01T19:00:01Z","title":"Light Higgs boson from multi-phase criticality in dynamical symmetry breaking","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2102.01084","snapshot_observed_at":"2026-08-06T11:19:54.052798Z","title":"Light Higgs boson from multi-phase criticality in dynamical symmetry breaking,","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2507.22980","last_updated":"2025-07-30T18:00:01Z","snapshot_observed_at":"2026-08-07T23:42:10.881444Z","submitted_at":"2025-07-30T18:00:01Z","title":"Hidden Sector Custodial Naturalness","version":1},"reference_index":23,"source":"pdf_text","source_observed_at":"2026-08-06T11:19:54.052798Z"},"links":{"cited_paper":"/paper/2102.01084","citing_paper":"/paper/2507.22980"},"observation_digest":"sha256:4fc49a9dd76216db672c71fb750431cbb7f76aeb7340a29092dd834a734c7a94","observation_id":"8f4bfd93-14cb-45da-b392-f232f8262e16","resolution":{"observed_at":"2026-08-06T11:19:54.052798Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2201.00824","last_updated":"2022-01-03T19:00:01Z","snapshot_observed_at":"2026-07-06T12:24:25.416929Z","submitted_at":"2022-01-03T19:00:01Z","title":"Multi-phase critical Higgs boson at colliders","version":1},"cited_work":{"arxiv_id":"2201.00824","doi":null,"metadata_source":"pith","pith_arxiv_id":"2201.00824","snapshot_observed_at":"2026-08-06T11:19:56.782342Z","title":"Multi-phase critical Higgs boson at colliders","venue":"hep-ph","work_id":"e09c05d4-754a-4644-8bbf-9bfe965ea373","year":2022},"citing_paper":{"arxiv_id":"2507.22980","last_updated":"2025-07-30T18:00:01Z","snapshot_observed_at":"2026-08-07T23:42:10.881444Z","submitted_at":"2025-07-30T18:00:01Z","title":"Hidden Sector Custodial Naturalness","version":1},"reference_index":24,"source":"pdf_text","source_observed_at":"2026-08-06T11:19:54.063588Z"},"links":{"cited_paper":"/paper/2201.00824","citing_paper":"/paper/2507.22980"},"observation_digest":"sha256:98e89689eedc5cfcfd389eb2ea5ff45e455e43ccd485e5a18bc82767db645a80","observation_id":"60e867aa-9822-42be-81c0-a1da2404be8a","resolution":{"observed_at":"2026-08-06T11:19:56.786840Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-06T11:19:57.291709Z","title":"Isospin Breaking in Technicolor Models,","venue":null,"work_id":"0c5e2833-c375-4345-880b-b619df693336","year":1980},"citing_paper":{"arxiv_id":"2507.22980","last_updated":"2025-07-30T18:00:01Z","snapshot_observed_at":"2026-08-07T23:42:10.881444Z","submitted_at":"2025-07-30T18:00:01Z","title":"Hidden Sector Custodial Naturalness","version":1},"reference_index":25,"source":"pdf_text","source_observed_at":"2026-08-06T11:19:54.136134Z"},"links":{"citing_paper":"/paper/2507.22980"},"observation_digest":"sha256:660b8944bfb5491116286498977b01528697b701186c54821bf59399f2b1115f","observation_id":"8142a7cb-1081-468d-bd38-53d7113ad7fa","resolution":{"observed_at":"2026-08-06T11:19:57.296237Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1306.4669","last_updated":"2013-06-19T20:39:07Z","snapshot_observed_at":"2026-08-07T15:21:57.641748Z","submitted_at":"2013-06-19T20:39:07Z","title":"Complex Spinors and Unified Theories","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1306.4669","snapshot_observed_at":"2026-08-06T11:19:54.223723Z","title":"µ → eγ at a Rate of One Out of 10 9 Muon Decays?,","venue":null,"work_id":null,"year":1977},"citing_paper":{"arxiv_id":"2507.22980","last_updated":"2025-07-30T18:00:01Z","snapshot_observed_at":"2026-08-07T23:42:10.881444Z","submitted_at":"2025-07-30T18:00:01Z","title":"Hidden Sector Custodial Naturalness","version":1},"reference_index":26,"source":"pdf_text","source_observed_at":"2026-08-06T11:19:54.223723Z"},"links":{"cited_paper":"/paper/1306.4669","citing_paper":"/paper/2507.22980"},"observation_digest":"sha256:9c1d64723106d378c8e406bcad05ee2b7db7808a86f8d2eec87083538d46deab","observation_id":"be706f84-8b60-4512-9284-676d5fa6c0ac","resolution":{"observed_at":"2026-08-06T11:19:54.223723Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2007.12700","last_updated":"2021-01-13T09:43:11Z","snapshot_observed_at":"2026-08-04T20:24:08.648843Z","submitted_at":"2020-07-24T18:00:01Z","title":"PyR@TE 3","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2007.12700","snapshot_observed_at":"2026-08-06T11:19:54.310627Z","title":"PyR@TE 3,","venue":null,"work_id":null,"year":2021},"citing_paper":{"arxiv_id":"2507.22980","last_updated":"2025-07-30T18:00:01Z","snapshot_observed_at":"2026-08-07T23:42:10.881444Z","submitted_at":"2025-07-30T18:00:01Z","title":"Hidden Sector Custodial Naturalness","version":1},"reference_index":27,"source":"pdf_text","source_observed_at":"2026-08-06T11:19:54.310627Z"},"links":{"cited_paper":"/paper/2007.12700","citing_paper":"/paper/2507.22980"},"observation_digest":"sha256:71f7ffd03c0d4c7cf63ceb2511e2d6a8d0b196f56ac60199bf28ffe6b6762dac","observation_id":"b094f624-e041-4d26-ad27-4ce5260b3b27","resolution":{"observed_at":"2026-08-06T11:19:54.310627Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1307.3536","last_updated":"2014-09-22T14:12:25Z","snapshot_observed_at":"2026-08-02T08:26:57.200757Z","submitted_at":"2013-07-12T18:34:05Z","title":"Investigating the near-criticality of the Higgs boson","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1307.3536","snapshot_observed_at":"2026-08-06T11:19:54.402409Z","title":"Investigating the near-criticality of the Higgs boson,","venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"2507.22980","last_updated":"2025-07-30T18:00:01Z","snapshot_observed_at":"2026-08-07T23:42:10.881444Z","submitted_at":"2025-07-30T18:00:01Z","title":"Hidden Sector Custodial Naturalness","version":1},"reference_index":28,"source":"pdf_text","source_observed_at":"2026-08-06T11:19:54.402409Z"},"links":{"cited_paper":"/paper/1307.3536","citing_paper":"/paper/2507.22980"},"observation_digest":"sha256:755413e246a498a9e8f6bcdd85a6063e25f87f1bf7239b51a18831dd4faf3ecc","observation_id":"512d27d0-ad46-4879-8b7b-439392afd0df","resolution":{"observed_at":"2026-08-06T11:19:54.402409Z","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":"raw_reference","pith_arxiv_id":null,"snapshot_observed_at":"2026-08-06T11:19:57.276115Z","title":"Upper Bounds on Supersymmetric Particle Masses,","venue":null,"work_id":"8259c806-a306-468a-85af-5a25a073687a","year":1988},"citing_paper":{"arxiv_id":"2507.22980","last_updated":"2025-07-30T18:00:01Z","snapshot_observed_at":"2026-08-07T23:42:10.881444Z","submitted_at":"2025-07-30T18:00:01Z","title":"Hidden Sector Custodial Naturalness","version":1},"reference_index":29,"source":"pdf_text","source_observed_at":"2026-08-06T11:19:54.474143Z"},"links":{"citing_paper":"/paper/2507.22980"},"observation_digest":"sha256:2db76f85c22f55d1442d70f9ad6a62badabbdea0446fc1b54a3ff18beba12089","observation_id":"641b1b5a-ec67-4bb2-b462-a90f28fa7439","resolution":{"observed_at":"2026-08-06T11:19:57.281114Z","resolver_source":"raw_fallback","status":"verified_fuzzy"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1501.02234","last_updated":"2015-04-17T19:58:28Z","snapshot_observed_at":"2026-07-06T04:05:49.379983Z","submitted_at":"2015-01-09T19:07:45Z","title":"Status of the Higgs Singlet Extension of the Standard Model after LHC Run 1","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1501.02234","snapshot_observed_at":"2026-08-06T11:19:54.579076Z","title":"Status of the Higgs Singlet Extension of the Standard Model after LHC Run 1,","venue":null,"work_id":null,"year":2015},"citing_paper":{"arxiv_id":"2507.22980","last_updated":"2025-07-30T18:00:01Z","snapshot_observed_at":"2026-08-07T23:42:10.881444Z","submitted_at":"2025-07-30T18:00:01Z","title":"Hidden Sector Custodial Naturalness","version":1},"reference_index":30,"source":"pdf_text","source_observed_at":"2026-08-06T11:19:54.579076Z"},"links":{"cited_paper":"/paper/1501.02234","citing_paper":"/paper/2507.22980"},"observation_digest":"sha256:ee47b25886139d4c305a13053b3e3941ee64780dde93a4f516274c2870f10ea8","observation_id":"9a3718db-b729-4fcb-bc01-8bd43de0d283","resolution":{"observed_at":"2026-08-06T11:19:54.579076Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2409.19657","last_updated":"2024-11-18T09:21:01Z","snapshot_observed_at":"2026-07-06T19:24:03.133851Z","submitted_at":"2024-09-29T11:11:01Z","title":"Overview on low mass scalars at $e^+e^-$ facilities -- theory","version":2},"cited_work":{"arxiv_id":"2409.19657","doi":null,"metadata_source":"pith","pith_arxiv_id":"2409.19657","snapshot_observed_at":"2026-08-06T11:19:56.692367Z","title":"Overview on low mass scalars at $e^+e^-$ facilities -- theory","venue":"hep-ph","work_id":"49ee3325-70f4-4ce9-9257-adbb342988d8","year":2024},"citing_paper":{"arxiv_id":"2507.22980","last_updated":"2025-07-30T18:00:01Z","snapshot_observed_at":"2026-08-07T23:42:10.881444Z","submitted_at":"2025-07-30T18:00:01Z","title":"Hidden Sector Custodial Naturalness","version":1},"reference_index":31,"source":"pdf_text","source_observed_at":"2026-08-06T11:19:54.637661Z"},"links":{"cited_paper":"/paper/2409.19657","citing_paper":"/paper/2507.22980"},"observation_digest":"sha256:d55842bc940f77ac24c9e6e02715d44b1752c4f5a5f132951461fbd1e36fe265","observation_id":"2c6d6b0c-4b55-40a6-a622-94a07946e0e0","resolution":{"observed_at":"2026-08-06T11:19:56.697254Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":null,"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":null,"snapshot_observed_at":"2026-08-06T11:19:54.704868Z","title":"Abidi et al","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2507.22980","last_updated":"2025-07-30T18:00:01Z","snapshot_observed_at":"2026-08-07T23:42:10.881444Z","submitted_at":"2025-07-30T18:00:01Z","title":"Hidden Sector Custodial Naturalness","version":1},"reference_index":32,"source":"pdf_text","source_observed_at":"2026-08-06T11:19:54.704868Z"},"links":{"citing_paper":"/paper/2507.22980"},"observation_digest":"sha256:dc7d9fc374f3c008228673c69fd4fbc457b08191f7e482d808c3404eb5e8beb8","observation_id":"091fd781-6cff-471c-ac33-e1ce15156d14","resolution":{"observed_at":"2026-08-06T11:19:54.704868Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"0708.1463","last_updated":"2007-08-10T18:53:16Z","snapshot_observed_at":"2026-07-06T01:29:38.856548Z","submitted_at":"2007-08-10T18:53:16Z","title":"Light scalar at LHC: the Higgs or the dilaton?","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"0708.1463","snapshot_observed_at":"2026-08-06T11:19:54.756643Z","title":"Distinguishing the Higgs boson from the dilaton at the Large Hadron Collider,","venue":null,"work_id":null,"year":2008},"citing_paper":{"arxiv_id":"2507.22980","last_updated":"2025-07-30T18:00:01Z","snapshot_observed_at":"2026-08-07T23:42:10.881444Z","submitted_at":"2025-07-30T18:00:01Z","title":"Hidden Sector Custodial Naturalness","version":1},"reference_index":33,"source":"pdf_text","source_observed_at":"2026-08-06T11:19:54.756643Z"},"links":{"cited_paper":"/paper/0708.1463","citing_paper":"/paper/2507.22980"},"observation_digest":"sha256:086ebd2aeca82a837e4f046e6aa866bc9b37218d4529c02650736e435e002a22","observation_id":"0f39038d-61e0-40bc-80bb-f02ebeeb5b5d","resolution":{"observed_at":"2026-08-06T11:19:54.756643Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1209.3022","last_updated":"2013-06-24T04:54:31Z","snapshot_observed_at":"2026-07-06T02:55:35.722107Z","submitted_at":"2012-09-13T20:00:07Z","title":"Effective Theory of a Light Dilaton","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1209.3022","snapshot_observed_at":"2026-08-06T11:19:54.845993Z","title":"Effective Theory of a Light Dilaton,","venue":null,"work_id":null,"year":2013},"citing_paper":{"arxiv_id":"2507.22980","last_updated":"2025-07-30T18:00:01Z","snapshot_observed_at":"2026-08-07T23:42:10.881444Z","submitted_at":"2025-07-30T18:00:01Z","title":"Hidden Sector Custodial Naturalness","version":1},"reference_index":34,"source":"pdf_text","source_observed_at":"2026-08-06T11:19:54.845993Z"},"links":{"cited_paper":"/paper/1209.3022","citing_paper":"/paper/2507.22980"},"observation_digest":"sha256:55d99d0da92f6b2fe32fe60af1958169b584d24d84e3f73d0c7ecddd810f7a4e","observation_id":"ed64570b-1ab1-4c1c-93f6-91c4a9effe93","resolution":{"observed_at":"2026-08-06T11:19:54.845993Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1209.3299","last_updated":"2013-02-05T20:59:51Z","snapshot_observed_at":"2026-08-05T11:41:05.700663Z","submitted_at":"2012-09-14T19:55:54Z","title":"A Higgslike Dilaton","version":2},"cited_work":{"arxiv_id":"1209.3299","doi":null,"metadata_source":"pith","pith_arxiv_id":"1209.3299","snapshot_observed_at":"2026-08-06T11:19:56.539986Z","title":"A Higgslike Dilaton","venue":"hep-ph","work_id":"45ff22cc-2c5b-498d-a0ae-46e51f8d5bbe","year":2012},"citing_paper":{"arxiv_id":"2507.22980","last_updated":"2025-07-30T18:00:01Z","snapshot_observed_at":"2026-08-07T23:42:10.881444Z","submitted_at":"2025-07-30T18:00:01Z","title":"Hidden Sector Custodial Naturalness","version":1},"reference_index":35,"source":"pdf_text","source_observed_at":"2026-08-06T11:19:54.911078Z"},"links":{"cited_paper":"/paper/1209.3299","citing_paper":"/paper/2507.22980"},"observation_digest":"sha256:eccad317902266b6e73965e9a57da565d4431907e657838a8951bfc9eba91122","observation_id":"0f258ef4-e98e-4aec-a488-2480563d66b5","resolution":{"observed_at":"2026-08-06T11:19:56.544616Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1512.05771","last_updated":"2017-03-09T01:21:00Z","snapshot_observed_at":"2026-07-06T04:40:19.664205Z","submitted_at":"2015-12-17T20:50:37Z","title":"Implications of the absence of high-mass radion signals","version":4},"cited_work":{"arxiv_id":"1512.05771","doi":null,"metadata_source":"pith","pith_arxiv_id":"1512.05771","snapshot_observed_at":"2026-08-06T11:19:56.480113Z","title":"Implications of the absence of high-mass radion signals","venue":"hep-ph","work_id":"85995369-842b-427d-80ed-018015233712","year":2015},"citing_paper":{"arxiv_id":"2507.22980","last_updated":"2025-07-30T18:00:01Z","snapshot_observed_at":"2026-08-07T23:42:10.881444Z","submitted_at":"2025-07-30T18:00:01Z","title":"Hidden Sector Custodial Naturalness","version":1},"reference_index":36,"source":"pdf_text","source_observed_at":"2026-08-06T11:19:54.990265Z"},"links":{"cited_paper":"/paper/1512.05771","citing_paper":"/paper/2507.22980"},"observation_digest":"sha256:fc2530cb153a0e050a06a97e94df67e76256e3152e5db53a005f7eaac51404bb","observation_id":"68d7c08b-5542-45be-bf3e-b6acfee3bea9","resolution":{"observed_at":"2026-08-06T11:19:56.523333Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"1912.06645","last_updated":"2020-05-22T14:09:57Z","snapshot_observed_at":"2026-08-05T19:41:09.719486Z","submitted_at":"2019-12-13T18:44:46Z","title":"A light dilaton at the LHC","version":2},"cited_work":{"arxiv_id":"1912.06645","doi":null,"metadata_source":"pith","pith_arxiv_id":"1912.06645","snapshot_observed_at":"2026-08-06T11:19:56.277303Z","title":"A light dilaton at the LHC","venue":"hep-ph","work_id":"65dc2b48-8a58-4c8b-b093-3be205452715","year":2019},"citing_paper":{"arxiv_id":"2507.22980","last_updated":"2025-07-30T18:00:01Z","snapshot_observed_at":"2026-08-07T23:42:10.881444Z","submitted_at":"2025-07-30T18:00:01Z","title":"Hidden Sector Custodial Naturalness","version":1},"reference_index":37,"source":"pdf_text","source_observed_at":"2026-08-06T11:19:55.058257Z"},"links":{"cited_paper":"/paper/1912.06645","citing_paper":"/paper/2507.22980"},"observation_digest":"sha256:56edc8da016124f085d9408dcdf36c56dc6f070661f8508b9355aa0cef6d4001","observation_id":"296fccc4-5def-47df-bf76-e2a0a1a31f18","resolution":{"observed_at":"2026-08-06T11:19:56.357241Z","resolver_source":"local_arxiv","status":"verified_exact"},"standing_notice":{"events":[],"observation":"No event found in the named queried sources as of 2026-08-09T06:31:02.800959+00:00.","reason":null,"source_receipts":[{"observed_at":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"state":"measured"}},{"citation":{"cited_paper":{"arxiv_id":"2303.14729","last_updated":"2023-08-05T21:12:39Z","snapshot_observed_at":"2026-08-07T23:19:29.815985Z","submitted_at":"2023-03-26T14:13:02Z","title":"First Dark Matter Search with Nuclear Recoils from the XENONnT Experiment","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2303.14729","snapshot_observed_at":"2026-08-06T11:19:55.156102Z","title":"First Dark Matter Search with Nuclear Recoils from the XENONnT Experiment,","venue":null,"work_id":null,"year":2023},"citing_paper":{"arxiv_id":"2507.22980","last_updated":"2025-07-30T18:00:01Z","snapshot_observed_at":"2026-08-07T23:42:10.881444Z","submitted_at":"2025-07-30T18:00:01Z","title":"Hidden Sector Custodial Naturalness","version":1},"reference_index":38,"source":"pdf_text","source_observed_at":"2026-08-06T11:19:55.156102Z"},"links":{"cited_paper":"/paper/2303.14729","citing_paper":"/paper/2507.22980"},"observation_digest":"sha256:26670c87a2ec78a34a5f2aec0c915b078062b8458291e859296664e7a526f92b","observation_id":"1f7ed33d-8130-42b6-a042-b98a319836ca","resolution":{"observed_at":"2026-08-06T11:19:55.156102Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2410.17036","last_updated":"2025-07-01T14:32:43Z","snapshot_observed_at":"2026-07-06T19:37:52.003100Z","submitted_at":"2024-10-22T14:07:18Z","title":"Dark Matter Search Results from 4.2 Tonne-Years of Exposure of the LUX-ZEPLIN (LZ) Experiment","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2410.17036","snapshot_observed_at":"2026-08-06T11:19:55.238930Z","title":"Dark Matter Search Results from 4.2 Tonne-Years of Exposure of the LUX-ZEPLIN (LZ) Experiment,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2507.22980","last_updated":"2025-07-30T18:00:01Z","snapshot_observed_at":"2026-08-07T23:42:10.881444Z","submitted_at":"2025-07-30T18:00:01Z","title":"Hidden Sector Custodial Naturalness","version":1},"reference_index":39,"source":"pdf_text","source_observed_at":"2026-08-06T11:19:55.238930Z"},"links":{"cited_paper":"/paper/2410.17036","citing_paper":"/paper/2507.22980"},"observation_digest":"sha256:d85ddc4f745abd49a7a5fdfb9413aa1595756573109da54ba903739054fe9e26","observation_id":"5b69d846-5b5f-43f4-89fd-57624a0ce419","resolution":{"observed_at":"2026-08-06T11:19:55.238930Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2408.03649","last_updated":"2026-05-21T04:32:42Z","snapshot_observed_at":"2026-07-06T18:57:48.065595Z","submitted_at":"2024-08-07T09:24:07Z","title":"Probing radiative electroweak symmetry breaking with colliders and gravitational waves","version":4},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2408.03649","snapshot_observed_at":"2026-08-06T11:19:55.301534Z","title":"Probing radiative electroweak symmetry breaking with colliders and gravitational waves,","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2507.22980","last_updated":"2025-07-30T18:00:01Z","snapshot_observed_at":"2026-08-07T23:42:10.881444Z","submitted_at":"2025-07-30T18:00:01Z","title":"Hidden Sector Custodial Naturalness","version":1},"reference_index":40,"source":"pdf_text","source_observed_at":"2026-08-06T11:19:55.301534Z"},"links":{"cited_paper":"/paper/2408.03649","citing_paper":"/paper/2507.22980"},"observation_digest":"sha256:f83548cc4724571879b58ee016d0f0f5c6071807271a66b9319dbeb8d5f57e31","observation_id":"39318845-f03f-43b6-8627-c73e9331ef30","resolution":{"observed_at":"2026-08-06T11:19:55.301534Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2306.13061","last_updated":"2024-04-26T15:27:23Z","snapshot_observed_at":"2026-08-05T22:20:14.841500Z","submitted_at":"2023-06-22T17:30:14Z","title":"Freeze-in at stronger coupling","version":3},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2306.13061","snapshot_observed_at":"2026-08-06T11:19:55.370065Z","title":"Freeze-in at stronger coupling,","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2507.22980","last_updated":"2025-07-30T18:00:01Z","snapshot_observed_at":"2026-08-07T23:42:10.881444Z","submitted_at":"2025-07-30T18:00:01Z","title":"Hidden Sector Custodial Naturalness","version":1},"reference_index":41,"source":"pdf_text","source_observed_at":"2026-08-06T11:19:55.370065Z"},"links":{"cited_paper":"/paper/2306.13061","citing_paper":"/paper/2507.22980"},"observation_digest":"sha256:3a138fc99f3fa5290d24104bf9ff9a686ae19eaf3757bfffd7c65e8a849c01b8","observation_id":"c61b07de-9011-4219-a304-065dae8b7c04","resolution":{"observed_at":"2026-08-06T11:19:55.370065Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2402.04743","last_updated":"2024-05-17T14:31:30Z","snapshot_observed_at":"2026-08-06T15:02:37.946628Z","submitted_at":"2024-02-07T10:55:18Z","title":"Temperature evolution in the Early Universe and freeze-in at stronger coupling","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2402.04743","snapshot_observed_at":"2026-08-06T11:19:55.439785Z","title":"Temperature evolution in the Early Universe and freeze-in at stronger coupling,","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2507.22980","last_updated":"2025-07-30T18:00:01Z","snapshot_observed_at":"2026-08-07T23:42:10.881444Z","submitted_at":"2025-07-30T18:00:01Z","title":"Hidden Sector Custodial Naturalness","version":1},"reference_index":42,"source":"pdf_text","source_observed_at":"2026-08-06T11:19:55.439785Z"},"links":{"cited_paper":"/paper/2402.04743","citing_paper":"/paper/2507.22980"},"observation_digest":"sha256:91669728a31b23d794b4a87024684eaf96495ab3e763662b065a9ebd87dd78a6","observation_id":"00a50777-2bee-4e7b-9cd9-b53b417a852a","resolution":{"observed_at":"2026-08-06T11:19:55.439785Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2409.02191","last_updated":"2024-09-03T18:01:31Z","snapshot_observed_at":"2026-08-04T04:21:26.826456Z","submitted_at":"2024-09-03T18:01:31Z","title":"$Z^\\prime$-mediated dark matter freeze-in at stronger coupling","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2409.02191","snapshot_observed_at":"2026-08-06T11:19:55.508286Z","title":"Z’-mediated dark matter freeze-in at stronger coupling,","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2507.22980","last_updated":"2025-07-30T18:00:01Z","snapshot_observed_at":"2026-08-07T23:42:10.881444Z","submitted_at":"2025-07-30T18:00:01Z","title":"Hidden Sector Custodial Naturalness","version":1},"reference_index":43,"source":"pdf_text","source_observed_at":"2026-08-06T11:19:55.508286Z"},"links":{"cited_paper":"/paper/2409.02191","citing_paper":"/paper/2507.22980"},"observation_digest":"sha256:0bed28bc94278d52bf8bdb13d88dc51c98c6e9551aaea9ed489c2a8faaef76b3","observation_id":"ae616604-ed73-4d1f-8a57-dc5a3d5a05a0","resolution":{"observed_at":"2026-08-06T11:19:55.508286Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2405.03760","last_updated":"2024-05-06T18:01:06Z","snapshot_observed_at":"2026-08-06T05:33:32.308152Z","submitted_at":"2024-05-06T18:01:06Z","title":"Higgs Portal Dark Matter Freeze-in at Stronger Coupling: Observational Benchmarks","version":1},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2405.03760","snapshot_observed_at":"2026-08-06T11:19:55.600657Z","title":"Higgs portal dark matter freeze-in at stronger coupling: observational benchmarks,","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2507.22980","last_updated":"2025-07-30T18:00:01Z","snapshot_observed_at":"2026-08-07T23:42:10.881444Z","submitted_at":"2025-07-30T18:00:01Z","title":"Hidden Sector Custodial Naturalness","version":1},"reference_index":44,"source":"pdf_text","source_observed_at":"2026-08-06T11:19:55.600657Z"},"links":{"cited_paper":"/paper/2405.03760","citing_paper":"/paper/2507.22980"},"observation_digest":"sha256:990def243167362bf4b116bb8f686c1b465b3cd1d052d637102de3698b8e7d38","observation_id":"2891caa5-623e-4cb9-9405-1131b4174d58","resolution":{"observed_at":"2026-08-06T11:19:55.600657Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2410.21874","last_updated":"2024-10-30T11:28:18Z","snapshot_observed_at":"2026-07-06T19:41:24.411424Z","submitted_at":"2024-10-29T09:09:54Z","title":"Invisible Higgs decay from dark matter freeze-in at stronger coupling","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2410.21874","snapshot_observed_at":"2026-08-06T11:19:55.695381Z","title":"Invisible Higgs decay from dark matter freeze-in at stronger coupling,","venue":null,"work_id":null,"year":2025},"citing_paper":{"arxiv_id":"2507.22980","last_updated":"2025-07-30T18:00:01Z","snapshot_observed_at":"2026-08-07T23:42:10.881444Z","submitted_at":"2025-07-30T18:00:01Z","title":"Hidden Sector Custodial Naturalness","version":1},"reference_index":45,"source":"pdf_text","source_observed_at":"2026-08-06T11:19:55.695381Z"},"links":{"cited_paper":"/paper/2410.21874","citing_paper":"/paper/2507.22980"},"observation_digest":"sha256:8dd99af618de0d67d30748356cea9e75639afa111fb2a5ea72f157f17bf4e462","observation_id":"b8842f37-4341-4c96-bd63-b8dd47cc6a51","resolution":{"observed_at":"2026-08-06T11:19:55.695381Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2312.14894","last_updated":"2024-02-26T10:36:11Z","snapshot_observed_at":"2026-08-06T22:01:14.026511Z","submitted_at":"2023-12-22T18:16:08Z","title":"micrOMEGAs 6.0: N-component dark matter","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2312.14894","snapshot_observed_at":"2026-08-06T11:19:55.796107Z","title":"micrOMEGAs 6.0: N-component dark matter,","venue":null,"work_id":null,"year":2024},"citing_paper":{"arxiv_id":"2507.22980","last_updated":"2025-07-30T18:00:01Z","snapshot_observed_at":"2026-08-07T23:42:10.881444Z","submitted_at":"2025-07-30T18:00:01Z","title":"Hidden Sector Custodial Naturalness","version":1},"reference_index":46,"source":"pdf_text","source_observed_at":"2026-08-06T11:19:55.796107Z"},"links":{"cited_paper":"/paper/2312.14894","citing_paper":"/paper/2507.22980"},"observation_digest":"sha256:f530878e97a83d1127cefcab4838e92358106dd3116cf64531db8676bd82d1b0","observation_id":"985752d7-79b4-4d18-96c2-31f62c5e7f91","resolution":{"observed_at":"2026-08-06T11:19:55.796107Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"1309.7223","last_updated":"2014-02-14T10:03:23Z","snapshot_observed_at":"2026-07-06T03:24:09.535709Z","submitted_at":"2013-09-27T12:35:15Z","title":"SARAH 4: A tool for (not only SUSY) model builders","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"1309.7223","snapshot_observed_at":"2026-08-06T11:19:55.883759Z","title":"SARAH 4 : A tool for (not only SUSY) model builders,","venue":null,"work_id":null,"year":2014},"citing_paper":{"arxiv_id":"2507.22980","last_updated":"2025-07-30T18:00:01Z","snapshot_observed_at":"2026-08-07T23:42:10.881444Z","submitted_at":"2025-07-30T18:00:01Z","title":"Hidden Sector Custodial Naturalness","version":1},"reference_index":47,"source":"pdf_text","source_observed_at":"2026-08-06T11:19:55.883759Z"},"links":{"cited_paper":"/paper/1309.7223","citing_paper":"/paper/2507.22980"},"observation_digest":"sha256:4cc54f76c8a3157f26d074646660b27e9310f93785f263dbae2df1132c6c9589","observation_id":"fda3e1c1-786e-4a15-8fc7-04c89b774a0a","resolution":{"observed_at":"2026-08-06T11:19:55.883759Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}},{"citation":{"cited_paper":{"arxiv_id":"2506.15496","last_updated":"2026-05-22T14:57:53Z","snapshot_observed_at":"2026-07-06T02:11:23.670680Z","submitted_at":"2025-06-18T14:34:48Z","title":"Thermodynamical uncertainties for primordial black holes from cosmological phase transitions","version":2},"cited_work":{"arxiv_id":null,"doi":null,"metadata_source":null,"pith_arxiv_id":"2506.15496","snapshot_observed_at":"2026-08-06T11:19:55.961212Z","title":"Theoretical uncertainties for primordial black holes from cosmological phase transitions,","venue":null,"work_id":null,"year":null},"citing_paper":{"arxiv_id":"2507.22980","last_updated":"2025-07-30T18:00:01Z","snapshot_observed_at":"2026-08-07T23:42:10.881444Z","submitted_at":"2025-07-30T18:00:01Z","title":"Hidden Sector Custodial Naturalness","version":1},"reference_index":48,"source":"pdf_text","source_observed_at":"2026-08-06T11:19:55.961212Z"},"links":{"cited_paper":"/paper/2506.15496","citing_paper":"/paper/2507.22980"},"observation_digest":"sha256:117d8b4680ef0a803cfbaf9d3c5e8d13b74cb271868ef71acede0d8b47aed800","observation_id":"8d89824e-68f0-4950-adbd-bc7e62a3560f","resolution":{"observed_at":"2026-08-06T11:19:55.961212Z","resolver_source":null,"status":"unresolved"},"standing_notice":{"events":[],"reason":"canonical_work_link_unavailable","source_receipts":[],"state":"unavailable"}}],"paper":{"arxiv_id":"2507.22980","last_updated":"2025-07-30T18:00:01Z","latest_version":1,"primary_category":"hep-ph","snapshot_observed_at":"2026-08-07T23:42:10.881444Z","submitted_at":"2025-07-30T18:00:01Z","title":"Hidden Sector Custodial Naturalness"},"reference_resolution":{"displayed":48,"state_counts":{"malformed_identifier":0,"metadata_mismatch":0,"parse_uncertain":0,"unresolved":31,"verified_exact":11,"verified_fuzzy":6},"total_outbound_references":48},"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":"2026-08-09T06:31:02.800959+00:00","source":"crossref"},{"observed_at":"2026-08-09T06:30:57.326959+00:00","source":"retraction_watch"}],"thesis":"As of 10 August 2026, this Paper Citation Record lists 48 of 48 outbound references and 2 inbound Pith citation observations for arXiv:2507.22980."}