{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2026:EOEEIY6PTEGMGD5GS6QIITLDB7","short_pith_number":"pith:EOEEIY6P","schema_version":"1.0","canonical_sha256":"23884463cf990cc30fa697a0844d630fc7b1f2f3bb7809df07996d8be63d78c0","source":{"kind":"arxiv","id":"2608.12456","version":1},"attestation_state":"computed","paper":{"title":"Dark matter in scale-invariant gravity with hidden-sector condensation","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Jisuke Kubo, Juan P. Garc\\'es, Manfred Lindner, Markus Reinig","submitted_at":"2026-08-12T18:00:00Z","abstract_excerpt":"The origin of the electroweak scale, cosmic inflation, and dark matter are often treated as independent problems beyond the Standard Models of particle physics and cosmology. In this work, we explore the possibility that they instead arise from a common underlying framework based on classically scale-invariant quadratic gravity coupled to a strongly interacting hidden sector. The $R^2$ term naturally realizes Starobinsky inflation, while confinement in the hidden sector dynamically generates the Planck scale and triggers electroweak symmetry breaking through a gravitationally induced Higgs mas"},"verification_status":{"content_addressed":true,"pith_receipt":true,"author_attested":false,"weak_author_claims":0,"strong_author_claims":0,"externally_anchored":false,"storage_verified":false,"citation_signatures":0,"replication_records":0,"graph_snapshot":true,"references_resolved":false,"formal_links_present":false},"canonical_record":{"source":{"id":"2608.12456","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2026-08-12T18:00:00Z","cross_cats_sorted":[],"title_canon_sha256":"bfe7eca81bc57633f5fef9aa3a275f1f46b4a2cc6b332f61632aa07ee8ba4b1c","abstract_canon_sha256":"ae2bd4d51e014dcb48b15c64c9bcd645ea3624ea11e4a10eed0c96e16eed3f3a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-08-14T00:43:21.595557Z","signature_b64":"SDh/ORUBf5pVEL1DjvCCn3m8SLoxCBWmZGy6oIAyiXUk4WXufYKI5p66MS7RYjUnDWoMYdj0LNjXfKk7F/BXCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"23884463cf990cc30fa697a0844d630fc7b1f2f3bb7809df07996d8be63d78c0","last_reissued_at":"2026-08-14T00:43:21.579729Z","signature_status":"signed_v1","first_computed_at":"2026-08-14T00:43:21.579729Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Dark matter in scale-invariant gravity with hidden-sector condensation","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Jisuke Kubo, Juan P. Garc\\'es, Manfred Lindner, Markus Reinig","submitted_at":"2026-08-12T18:00:00Z","abstract_excerpt":"The origin of the electroweak scale, cosmic inflation, and dark matter are often treated as independent problems beyond the Standard Models of particle physics and cosmology. In this work, we explore the possibility that they instead arise from a common underlying framework based on classically scale-invariant quadratic gravity coupled to a strongly interacting hidden sector. The $R^2$ term naturally realizes Starobinsky inflation, while confinement in the hidden sector dynamically generates the Planck scale and triggers electroweak symmetry breaking through a gravitationally induced Higgs mas"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2608.12456","kind":"arxiv","version":1},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2608.12456/integrity.json","findings":[],"available":true,"detectors_run":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938"},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"aliases":[{"alias_kind":"arxiv","alias_value":"2608.12456","created_at":"2026-08-14T00:43:21.589907+00:00"},{"alias_kind":"arxiv_version","alias_value":"2608.12456v1","created_at":"2026-08-14T00:43:21.589907+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2608.12456","created_at":"2026-08-14T00:43:21.589907+00:00"},{"alias_kind":"pith_short_12","alias_value":"EOEEIY6PTEGM","created_at":"2026-08-14T00:43:21.589907+00:00"},{"alias_kind":"pith_short_16","alias_value":"EOEEIY6PTEGMGD5G","created_at":"2026-08-14T00:43:21.589907+00:00"},{"alias_kind":"pith_short_8","alias_value":"EOEEIY6P","created_at":"2026-08-14T00:43:21.589907+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/EOEEIY6PTEGMGD5GS6QIITLDB7","json":"https://pith.science/pith/EOEEIY6PTEGMGD5GS6QIITLDB7.json","graph_json":"https://pith.science/api/pith-number/EOEEIY6PTEGMGD5GS6QIITLDB7/graph.json","events_json":"https://pith.science/api/pith-number/EOEEIY6PTEGMGD5GS6QIITLDB7/events.json","paper":"https://pith.science/paper/EOEEIY6P"},"agent_actions":{"view_html":"https://pith.science/pith/EOEEIY6PTEGMGD5GS6QIITLDB7","download_json":"https://pith.science/pith/EOEEIY6PTEGMGD5GS6QIITLDB7.json","view_paper":"https://pith.science/paper/EOEEIY6P","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2608.12456&json=true","fetch_graph":"https://pith.science/api/pith-number/EOEEIY6PTEGMGD5GS6QIITLDB7/graph.json","fetch_events":"https://pith.science/api/pith-number/EOEEIY6PTEGMGD5GS6QIITLDB7/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/EOEEIY6PTEGMGD5GS6QIITLDB7/action/timestamp_anchor","attest_storage":"https://pith.science/pith/EOEEIY6PTEGMGD5GS6QIITLDB7/action/storage_attestation","attest_author":"https://pith.science/pith/EOEEIY6PTEGMGD5GS6QIITLDB7/action/author_attestation","sign_citation":"https://pith.science/pith/EOEEIY6PTEGMGD5GS6QIITLDB7/action/citation_signature","submit_replication":"https://pith.science/pith/EOEEIY6PTEGMGD5GS6QIITLDB7/action/replication_record"}},"created_at":"2026-08-14T00:43:21.589907+00:00","updated_at":"2026-08-14T00:43:21.589907+00:00"}