{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2025:DIAX5WQRQXCSAZDCYWG3S6NMNZ","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"ba1dbb1b48c184fc76e10e4cb99da208340c10aa31e4451d437aa446f70fefd2","cross_cats_sorted":["physics.plasm-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2025-07-18T18:00:00Z","title_canon_sha256":"ce117be90ac69b910b70594a2ce685229717cb6b5a99a6535d1ccbec1a1afd47"},"schema_version":"1.0","source":{"id":"2507.14277","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2507.14277","created_at":"2026-07-05T11:40:03Z"},{"alias_kind":"arxiv_version","alias_value":"2507.14277v1","created_at":"2026-07-05T11:40:03Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2507.14277","created_at":"2026-07-05T11:40:03Z"},{"alias_kind":"pith_short_12","alias_value":"DIAX5WQRQXCS","created_at":"2026-07-05T11:40:03Z"},{"alias_kind":"pith_short_16","alias_value":"DIAX5WQRQXCSAZDC","created_at":"2026-07-05T11:40:03Z"},{"alias_kind":"pith_short_8","alias_value":"DIAX5WQR","created_at":"2026-07-05T11:40:03Z"}],"graph_snapshots":[{"event_id":"sha256:d4d34e049fb4431a27f85a52b09d008071d48fca74e646d7b1ca0165bc9164fa","target":"graph","created_at":"2026-07-05T11:40:03Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"integrity":{"available":true,"clean":true,"detectors_run":[],"endpoint":"/pith/2507.14277/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"Quantifying the effects of finite temperature and density (FTD) on particle properties is essential for understanding phenomena within and beyond the Standard Model. In this work, we present a simplified framework for calculating particle production rates at FTD without resorting to a full thermal field theory calculation. We do so by relating the imaginary part of a particle's $n$-loop finite temperature self energy, which defines its in-medium damping rate, to a sum of thermally weighted tree-level vacuum rates. Such a mapping results in novel \"interference\" contributions to particle product","authors_text":"Hugo Sch\\'erer, Katelin Schutz, Nirmalya Brahma, Saniya Heeba","cross_cats":["physics.plasm-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2025-07-18T18:00:00Z","title":"Spectral Surgery in a Heat Bath: a finite-temperature guide to particle production for phenomenologists"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2507.14277","kind":"arxiv","version":1},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:d89e4ea1be986555799eadd4c83e385eaa477ca3cd853cc184c1febf40946c69","target":"record","created_at":"2026-07-05T11:40:03Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"ba1dbb1b48c184fc76e10e4cb99da208340c10aa31e4451d437aa446f70fefd2","cross_cats_sorted":["physics.plasm-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2025-07-18T18:00:00Z","title_canon_sha256":"ce117be90ac69b910b70594a2ce685229717cb6b5a99a6535d1ccbec1a1afd47"},"schema_version":"1.0","source":{"id":"2507.14277","kind":"arxiv","version":1}},"canonical_sha256":"1a017eda1185c5206462c58db979ac6e6a9aea1285ff069bac0734cc831d230e","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"1a017eda1185c5206462c58db979ac6e6a9aea1285ff069bac0734cc831d230e","first_computed_at":"2026-07-05T11:40:03.404013Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-07-05T11:40:03.404013Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"k2m4UfeRtvNKhA4VsgM4iSawhE37cFDQCTCyReDkEcvW/fHh4i5/vzQ5URA9fNTSNdEtOA9TovGYvBW76M3gBw==","signature_status":"signed_v1","signed_at":"2026-07-05T11:40:03.404475Z","signed_message":"canonical_sha256_bytes"},"source_id":"2507.14277","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:d89e4ea1be986555799eadd4c83e385eaa477ca3cd853cc184c1febf40946c69","sha256:d4d34e049fb4431a27f85a52b09d008071d48fca74e646d7b1ca0165bc9164fa"],"state_sha256":"8bd1a182500f544bd6b0be57e788c64290b3f4d501399702b2e7cba93f18d8ee"}