{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2022:DPVN6YTTM4QXDTXVK4K2XP2CKA","short_pith_number":"pith:DPVN6YTT","schema_version":"1.0","canonical_sha256":"1beadf6273672171cef55715abbf42503bedf80f57baab44278f129aa54ae035","source":{"kind":"arxiv","id":"2207.05094","version":1},"attestation_state":"computed","paper":{"title":"Chern-Simons Gravity and Neutrino Self-Interactions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc"],"primary_cat":"hep-ph","authors_text":"Cyril Creque-Sarbinowski, Stephon Alexander","submitted_at":"2022-07-11T18:00:02Z","abstract_excerpt":"Dynamical Chern-Simons gravity (dCS) is a four-dimensional parity-violating extension of general relativity. Current models predict the effect of this extension to be negligible due to large decay constants $f$ close to the scale of grand unified theories. Here, we present a construction of dCS allowing for much smaller decay constants, ranging from sub-eV to Planck scales. Specifically, we show that if there exists a fermion species with strong self-interactions, the short-wavelength fermion modes form a bound state. This bound state can then undergo dynamical symmetry breaking and the result"},"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":"2207.05094","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2022-07-11T18:00:02Z","cross_cats_sorted":["gr-qc"],"title_canon_sha256":"9802972a8a6eaba4d27b1c238609340f8e50f22e9f3b717380eb693ba93c7e26","abstract_canon_sha256":"e99f29b8d1d75a32f8baa818fcdd31174502910d2483054609a98d8c3374c9a0"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T04:39:09.069823Z","signature_b64":"Am9IN+QQFIL1HN701+L0h/Nk74JPFmGvq6rkaLiueUOGCyoMfTuo/yK/w8eTK7uNkgrvU9moDGKb8rhWotRgBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"1beadf6273672171cef55715abbf42503bedf80f57baab44278f129aa54ae035","last_reissued_at":"2026-07-05T04:39:09.068985Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T04:39:09.068985Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Chern-Simons Gravity and Neutrino Self-Interactions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc"],"primary_cat":"hep-ph","authors_text":"Cyril Creque-Sarbinowski, Stephon Alexander","submitted_at":"2022-07-11T18:00:02Z","abstract_excerpt":"Dynamical Chern-Simons gravity (dCS) is a four-dimensional parity-violating extension of general relativity. Current models predict the effect of this extension to be negligible due to large decay constants $f$ close to the scale of grand unified theories. Here, we present a construction of dCS allowing for much smaller decay constants, ranging from sub-eV to Planck scales. Specifically, we show that if there exists a fermion species with strong self-interactions, the short-wavelength fermion modes form a bound state. This bound state can then undergo dynamical symmetry breaking and the result"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2207.05094","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/2207.05094/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":"2207.05094","created_at":"2026-07-05T04:39:09.069040+00:00"},{"alias_kind":"arxiv_version","alias_value":"2207.05094v1","created_at":"2026-07-05T04:39:09.069040+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2207.05094","created_at":"2026-07-05T04:39:09.069040+00:00"},{"alias_kind":"pith_short_12","alias_value":"DPVN6YTTM4QX","created_at":"2026-07-05T04:39:09.069040+00:00"},{"alias_kind":"pith_short_16","alias_value":"DPVN6YTTM4QXDTXV","created_at":"2026-07-05T04:39:09.069040+00:00"},{"alias_kind":"pith_short_8","alias_value":"DPVN6YTT","created_at":"2026-07-05T04:39:09.069040+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2403.06053","citing_title":"Spinfoams, $\\gamma$-duality and parity violation in primordial gravitational waves","ref_index":36,"is_internal_anchor":false},{"citing_arxiv_id":"2604.21535","citing_title":"Fermion Condensate Inflation, Dynamical Waterfall Mechanism and Primordial Black Holes","ref_index":69,"is_internal_anchor":false},{"citing_arxiv_id":"2604.07332","citing_title":"Theoretical and Observational Bounds on Dynamical Chern-Simons Gravity as an Effective Field Theory","ref_index":55,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/DPVN6YTTM4QXDTXVK4K2XP2CKA","json":"https://pith.science/pith/DPVN6YTTM4QXDTXVK4K2XP2CKA.json","graph_json":"https://pith.science/api/pith-number/DPVN6YTTM4QXDTXVK4K2XP2CKA/graph.json","events_json":"https://pith.science/api/pith-number/DPVN6YTTM4QXDTXVK4K2XP2CKA/events.json","paper":"https://pith.science/paper/DPVN6YTT"},"agent_actions":{"view_html":"https://pith.science/pith/DPVN6YTTM4QXDTXVK4K2XP2CKA","download_json":"https://pith.science/pith/DPVN6YTTM4QXDTXVK4K2XP2CKA.json","view_paper":"https://pith.science/paper/DPVN6YTT","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2207.05094&json=true","fetch_graph":"https://pith.science/api/pith-number/DPVN6YTTM4QXDTXVK4K2XP2CKA/graph.json","fetch_events":"https://pith.science/api/pith-number/DPVN6YTTM4QXDTXVK4K2XP2CKA/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/DPVN6YTTM4QXDTXVK4K2XP2CKA/action/timestamp_anchor","attest_storage":"https://pith.science/pith/DPVN6YTTM4QXDTXVK4K2XP2CKA/action/storage_attestation","attest_author":"https://pith.science/pith/DPVN6YTTM4QXDTXVK4K2XP2CKA/action/author_attestation","sign_citation":"https://pith.science/pith/DPVN6YTTM4QXDTXVK4K2XP2CKA/action/citation_signature","submit_replication":"https://pith.science/pith/DPVN6YTTM4QXDTXVK4K2XP2CKA/action/replication_record"}},"created_at":"2026-07-05T04:39:09.069040+00:00","updated_at":"2026-07-05T04:39:09.069040+00:00"}