{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2005:MYCFLSZEGC55ZDEYPYRYLU5Q6V","short_pith_number":"pith:MYCFLSZE","schema_version":"1.0","canonical_sha256":"660455cb2430bbdc8c987e2385d3b0f545c387de44652a2676311ca931078593","source":{"kind":"arxiv","id":"hep-ph/0512177","version":2},"attestation_state":"computed","paper":{"title":"Pressure of the Standard Model Near the Electroweak Phase Transition","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"A. Gynther, M. Vepsalainen","submitted_at":"2005-12-14T09:46:01Z","abstract_excerpt":"We extend our previous determination of the thermodynamic pressure of the Standard Model so that the result can be applied down to temperatures corresponding to the electroweak crossover. This requires a further resummation which can be cleanly organised within the effective theory framework. The result allows for a precise determination of the expansion rate of the Universe for temperatures around the electroweak crossover."},"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":"hep-ph/0512177","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2005-12-14T09:46:01Z","cross_cats_sorted":[],"title_canon_sha256":"67458600af97256212cde5901f7d3ae8dc00d6fefaf8180df8ed73492bdf876d","abstract_canon_sha256":"ec052fcc42e5b07f99e19ea891d8be354cf43a78128d921c098dbdf1a74e25d5"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:55:55.902063Z","signature_b64":"1G2paaN4wWHNPNQe2PCf4fSNJbthSrkBdZac5Igqe8iiRYIK2bASbh7b/ijHhRtdh/LO5V22SFtVk7uFKsJqBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"660455cb2430bbdc8c987e2385d3b0f545c387de44652a2676311ca931078593","last_reissued_at":"2026-07-04T16:55:55.901697Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:55:55.901697Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Pressure of the Standard Model Near the Electroweak Phase Transition","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"A. Gynther, M. Vepsalainen","submitted_at":"2005-12-14T09:46:01Z","abstract_excerpt":"We extend our previous determination of the thermodynamic pressure of the Standard Model so that the result can be applied down to temperatures corresponding to the electroweak crossover. This requires a further resummation which can be cleanly organised within the effective theory framework. The result allows for a precise determination of the expansion rate of the Universe for temperatures around the electroweak crossover."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0512177","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/hep-ph/0512177/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":"hep-ph/0512177","created_at":"2026-07-04T16:55:55.901758+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0512177v2","created_at":"2026-07-04T16:55:55.901758+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0512177","created_at":"2026-07-04T16:55:55.901758+00:00"},{"alias_kind":"pith_short_12","alias_value":"MYCFLSZEGC55","created_at":"2026-07-04T16:55:55.901758+00:00"},{"alias_kind":"pith_short_16","alias_value":"MYCFLSZEGC55ZDEY","created_at":"2026-07-04T16:55:55.901758+00:00"},{"alias_kind":"pith_short_8","alias_value":"MYCFLSZE","created_at":"2026-07-04T16:55:55.901758+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2507.07755","citing_title":"Entropy production at electroweak bubble walls from scalar field fluctuations","ref_index":56,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/MYCFLSZEGC55ZDEYPYRYLU5Q6V","json":"https://pith.science/pith/MYCFLSZEGC55ZDEYPYRYLU5Q6V.json","graph_json":"https://pith.science/api/pith-number/MYCFLSZEGC55ZDEYPYRYLU5Q6V/graph.json","events_json":"https://pith.science/api/pith-number/MYCFLSZEGC55ZDEYPYRYLU5Q6V/events.json","paper":"https://pith.science/paper/MYCFLSZE"},"agent_actions":{"view_html":"https://pith.science/pith/MYCFLSZEGC55ZDEYPYRYLU5Q6V","download_json":"https://pith.science/pith/MYCFLSZEGC55ZDEYPYRYLU5Q6V.json","view_paper":"https://pith.science/paper/MYCFLSZE","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/0512177&json=true","fetch_graph":"https://pith.science/api/pith-number/MYCFLSZEGC55ZDEYPYRYLU5Q6V/graph.json","fetch_events":"https://pith.science/api/pith-number/MYCFLSZEGC55ZDEYPYRYLU5Q6V/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/MYCFLSZEGC55ZDEYPYRYLU5Q6V/action/timestamp_anchor","attest_storage":"https://pith.science/pith/MYCFLSZEGC55ZDEYPYRYLU5Q6V/action/storage_attestation","attest_author":"https://pith.science/pith/MYCFLSZEGC55ZDEYPYRYLU5Q6V/action/author_attestation","sign_citation":"https://pith.science/pith/MYCFLSZEGC55ZDEYPYRYLU5Q6V/action/citation_signature","submit_replication":"https://pith.science/pith/MYCFLSZEGC55ZDEYPYRYLU5Q6V/action/replication_record"}},"created_at":"2026-07-04T16:55:55.901758+00:00","updated_at":"2026-07-04T16:55:55.901758+00:00"}