{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2025:FHHYLXMR5HNDJEG4FRDXO6E2VN","short_pith_number":"pith:FHHYLXMR","canonical_record":{"source":{"id":"2503.18904","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2025-03-24T17:16:28Z","cross_cats_sorted":[],"title_canon_sha256":"6df0f33df349275fc7d651ee15c1acf72cce34fa88014381ef9b726e715ebd7a","abstract_canon_sha256":"54a6c4b4f60b24c74d6d2af7a2a166b86038177f157f4b4e8558f3c4bf74fb8b"},"schema_version":"1.0"},"canonical_sha256":"29cf85dd91e9da3490dc2c4777789aab4c5e417f76fe08b41eec7feab289d19c","source":{"kind":"arxiv","id":"2503.18904","version":2},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2503.18904","created_at":"2026-06-02T01:03:30Z"},{"alias_kind":"arxiv_version","alias_value":"2503.18904v2","created_at":"2026-06-02T01:03:30Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2503.18904","created_at":"2026-06-02T01:03:30Z"},{"alias_kind":"pith_short_12","alias_value":"FHHYLXMR5HND","created_at":"2026-06-02T01:03:30Z"},{"alias_kind":"pith_short_16","alias_value":"FHHYLXMR5HNDJEG4","created_at":"2026-06-02T01:03:30Z"},{"alias_kind":"pith_short_8","alias_value":"FHHYLXMR","created_at":"2026-06-02T01:03:30Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2025:FHHYLXMR5HNDJEG4FRDXO6E2VN","target":"record","payload":{"canonical_record":{"source":{"id":"2503.18904","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2025-03-24T17:16:28Z","cross_cats_sorted":[],"title_canon_sha256":"6df0f33df349275fc7d651ee15c1acf72cce34fa88014381ef9b726e715ebd7a","abstract_canon_sha256":"54a6c4b4f60b24c74d6d2af7a2a166b86038177f157f4b4e8558f3c4bf74fb8b"},"schema_version":"1.0"},"canonical_sha256":"29cf85dd91e9da3490dc2c4777789aab4c5e417f76fe08b41eec7feab289d19c","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-06-02T01:03:30.913421Z","signature_b64":"pdtBK/7ZyGCXPDdT8nJvzXV7mwpu7fe/G1TPNXVriJOUtsGaHlfPtoiDglws2aL2ffm/BIvbDVKaaFifLBGUAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"29cf85dd91e9da3490dc2c4777789aab4c5e417f76fe08b41eec7feab289d19c","last_reissued_at":"2026-06-02T01:03:30.912899Z","signature_status":"signed_v1","first_computed_at":"2026-06-02T01:03:30.912899Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"2503.18904","source_version":2,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-06-02T01:03:30Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"fWrdZeaJvoPMy4BdfutRaIZJOefAkKBFW0NN9FyNt2QfnmW7vCcHmLUaDX1X6Di6G82AD+o9ixBHhkvOBTEcBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-07T07:19:37.582886Z"},"content_sha256":"d84264e0f194bbd5bb1ec7085fdf45a9702c18f4ab004d37f8610528a4849f6f","schema_version":"1.0","event_id":"sha256:d84264e0f194bbd5bb1ec7085fdf45a9702c18f4ab004d37f8610528a4849f6f"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2025:FHHYLXMR5HNDJEG4FRDXO6E2VN","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Higher-dimensional operators at finite-temperature affect gravitational-wave predictions","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Fabio Bernardo, Philipp Klose, Philipp Schicho, Tuomas V. I. Tenkanen","submitted_at":"2025-03-24T17:16:28Z","abstract_excerpt":"We investigate the effect of higher-dimensional marginal operators on the thermodynamics of cosmological phase transitions. Using the Abelian Higgs model as a representative for radiatively-generated one-step transitions, we systematically match these operators, which arise at higher orders in the underlying high-temperature expansion of thermal effective field theory, and use field redefinitions to construct a complete, minimal, and gauge-invariant operator basis. The Abelian Higgs model shares the essential infrared structure of more realistic gauge-Higgs theories at high temperatures, allow"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2503.18904","kind":"arxiv","version":2},"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/2503.18904/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"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-06-02T01:03:30Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"90znss+hcVfPX1FpTd1dNy0pSCGGYTAbwydRnC8nfoiLo0MR9p8DI1ftHbP2Ac2LFEwHy/PgChtfl/zP0JnmCw==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-06-07T07:19:37.583302Z"},"content_sha256":"4ddce2c07573ca5ed3df2534c002a17ce0aa906a09795b950296975147a3c237","schema_version":"1.0","event_id":"sha256:4ddce2c07573ca5ed3df2534c002a17ce0aa906a09795b950296975147a3c237"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/FHHYLXMR5HNDJEG4FRDXO6E2VN/bundle.json","state_url":"https://pith.science/pith/FHHYLXMR5HNDJEG4FRDXO6E2VN/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/FHHYLXMR5HNDJEG4FRDXO6E2VN/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-06-07T07:19:37Z","links":{"resolver":"https://pith.science/pith/FHHYLXMR5HNDJEG4FRDXO6E2VN","bundle":"https://pith.science/pith/FHHYLXMR5HNDJEG4FRDXO6E2VN/bundle.json","state":"https://pith.science/pith/FHHYLXMR5HNDJEG4FRDXO6E2VN/state.json","well_known_bundle":"https://pith.science/.well-known/pith/FHHYLXMR5HNDJEG4FRDXO6E2VN/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2025:FHHYLXMR5HNDJEG4FRDXO6E2VN","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":"54a6c4b4f60b24c74d6d2af7a2a166b86038177f157f4b4e8558f3c4bf74fb8b","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2025-03-24T17:16:28Z","title_canon_sha256":"6df0f33df349275fc7d651ee15c1acf72cce34fa88014381ef9b726e715ebd7a"},"schema_version":"1.0","source":{"id":"2503.18904","kind":"arxiv","version":2}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"2503.18904","created_at":"2026-06-02T01:03:30Z"},{"alias_kind":"arxiv_version","alias_value":"2503.18904v2","created_at":"2026-06-02T01:03:30Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2503.18904","created_at":"2026-06-02T01:03:30Z"},{"alias_kind":"pith_short_12","alias_value":"FHHYLXMR5HND","created_at":"2026-06-02T01:03:30Z"},{"alias_kind":"pith_short_16","alias_value":"FHHYLXMR5HNDJEG4","created_at":"2026-06-02T01:03:30Z"},{"alias_kind":"pith_short_8","alias_value":"FHHYLXMR","created_at":"2026-06-02T01:03:30Z"}],"graph_snapshots":[{"event_id":"sha256:4ddce2c07573ca5ed3df2534c002a17ce0aa906a09795b950296975147a3c237","target":"graph","created_at":"2026-06-02T01:03:30Z","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/2503.18904/integrity.json","findings":[],"snapshot_sha256":"c28c3603d3b5d939e8dc4c7e95fa8dfce3d595e45f758748cecf8e644a296938","summary":{"advisory":0,"by_detector":{},"critical":0,"informational":0}},"paper":{"abstract_excerpt":"We investigate the effect of higher-dimensional marginal operators on the thermodynamics of cosmological phase transitions. Using the Abelian Higgs model as a representative for radiatively-generated one-step transitions, we systematically match these operators, which arise at higher orders in the underlying high-temperature expansion of thermal effective field theory, and use field redefinitions to construct a complete, minimal, and gauge-invariant operator basis. The Abelian Higgs model shares the essential infrared structure of more realistic gauge-Higgs theories at high temperatures, allow","authors_text":"Fabio Bernardo, Philipp Klose, Philipp Schicho, Tuomas V. I. Tenkanen","cross_cats":[],"headline":"","license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2025-03-24T17:16:28Z","title":"Higher-dimensional operators at finite-temperature affect gravitational-wave predictions"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2503.18904","kind":"arxiv","version":2},"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:d84264e0f194bbd5bb1ec7085fdf45a9702c18f4ab004d37f8610528a4849f6f","target":"record","created_at":"2026-06-02T01:03:30Z","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":"54a6c4b4f60b24c74d6d2af7a2a166b86038177f157f4b4e8558f3c4bf74fb8b","cross_cats_sorted":[],"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2025-03-24T17:16:28Z","title_canon_sha256":"6df0f33df349275fc7d651ee15c1acf72cce34fa88014381ef9b726e715ebd7a"},"schema_version":"1.0","source":{"id":"2503.18904","kind":"arxiv","version":2}},"canonical_sha256":"29cf85dd91e9da3490dc2c4777789aab4c5e417f76fe08b41eec7feab289d19c","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"29cf85dd91e9da3490dc2c4777789aab4c5e417f76fe08b41eec7feab289d19c","first_computed_at":"2026-06-02T01:03:30.912899Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-06-02T01:03:30.912899Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"pdtBK/7ZyGCXPDdT8nJvzXV7mwpu7fe/G1TPNXVriJOUtsGaHlfPtoiDglws2aL2ffm/BIvbDVKaaFifLBGUAA==","signature_status":"signed_v1","signed_at":"2026-06-02T01:03:30.913421Z","signed_message":"canonical_sha256_bytes"},"source_id":"2503.18904","source_kind":"arxiv","source_version":2}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:d84264e0f194bbd5bb1ec7085fdf45a9702c18f4ab004d37f8610528a4849f6f","sha256:4ddce2c07573ca5ed3df2534c002a17ce0aa906a09795b950296975147a3c237"],"state_sha256":"ce882ac90cca77589676559218d133661684a36496e6068d825c720e994e0932"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"xRb+zlxbfItsdrvw9bHT6DEZ6Ba2wqKPrEehTEVsxCZQwvjYPDIp5qP+K/tjOB+Cx4TBCqz5EVivTgJJ2qNABQ==","signed_message":"bundle_sha256_bytes","signed_at":"2026-06-07T07:19:37.586361Z","bundle_sha256":"29fcc24406a0ebd95b925a547bbf0f3fb081af2a1734f670d1d89eaf66ec4c41"}}