{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2012:Q3M7ZMZAH55F7KZ45YA354IDE5","short_pith_number":"pith:Q3M7ZMZA","schema_version":"1.0","canonical_sha256":"86d9fcb3203f7a5fab3cee01bef1032753eac618f02d0591dc4ed522efd2614e","source":{"kind":"arxiv","id":"1207.3941","version":1},"attestation_state":"computed","paper":{"title":"Hard Thermal Loops in the n-Dimensional phi3 Theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"F. T. Brandt, J. Frenkel","submitted_at":"2012-07-17T10:50:10Z","abstract_excerpt":"We derive a closed-form result for the leading thermal contributions which appear in the n-dimensional phi3 theory at high temperature. These contributions become local only in the long wavelength and in the static limits, being given by different expressions in these two limits."},"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":"1207.3941","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2012-07-17T10:50:10Z","cross_cats_sorted":[],"title_canon_sha256":"65f6973c3cf3c0cdc195dcf04ddc58421fcdb23738c33be37b08f2b2458b9ee1","abstract_canon_sha256":"885afc05cca0872381365450dfe1e8eba43198f775d499928ff68722aa3d1c30"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:41:20.034148Z","signature_b64":"uf06BgaTAaQc3SD177jiK+oH+PvyNfqRyg3Ig7E0J9foaQwMO0/DfaJNBV0HOBfQ3mowCs13mpcgTQz8aJfJAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"86d9fcb3203f7a5fab3cee01bef1032753eac618f02d0591dc4ed522efd2614e","last_reissued_at":"2026-05-18T03:41:20.033733Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:41:20.033733Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Hard Thermal Loops in the n-Dimensional phi3 Theory","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-th","authors_text":"F. T. Brandt, J. Frenkel","submitted_at":"2012-07-17T10:50:10Z","abstract_excerpt":"We derive a closed-form result for the leading thermal contributions which appear in the n-dimensional phi3 theory at high temperature. These contributions become local only in the long wavelength and in the static limits, being given by different expressions in these two limits."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1207.3941","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":""},"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":"1207.3941","created_at":"2026-05-18T03:41:20.033797+00:00"},{"alias_kind":"arxiv_version","alias_value":"1207.3941v1","created_at":"2026-05-18T03:41:20.033797+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1207.3941","created_at":"2026-05-18T03:41:20.033797+00:00"},{"alias_kind":"pith_short_12","alias_value":"Q3M7ZMZAH55F","created_at":"2026-05-18T12:27:18.751474+00:00"},{"alias_kind":"pith_short_16","alias_value":"Q3M7ZMZAH55F7KZ4","created_at":"2026-05-18T12:27:18.751474+00:00"},{"alias_kind":"pith_short_8","alias_value":"Q3M7ZMZA","created_at":"2026-05-18T12:27:18.751474+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/Q3M7ZMZAH55F7KZ45YA354IDE5","json":"https://pith.science/pith/Q3M7ZMZAH55F7KZ45YA354IDE5.json","graph_json":"https://pith.science/api/pith-number/Q3M7ZMZAH55F7KZ45YA354IDE5/graph.json","events_json":"https://pith.science/api/pith-number/Q3M7ZMZAH55F7KZ45YA354IDE5/events.json","paper":"https://pith.science/paper/Q3M7ZMZA"},"agent_actions":{"view_html":"https://pith.science/pith/Q3M7ZMZAH55F7KZ45YA354IDE5","download_json":"https://pith.science/pith/Q3M7ZMZAH55F7KZ45YA354IDE5.json","view_paper":"https://pith.science/paper/Q3M7ZMZA","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1207.3941&json=true","fetch_graph":"https://pith.science/api/pith-number/Q3M7ZMZAH55F7KZ45YA354IDE5/graph.json","fetch_events":"https://pith.science/api/pith-number/Q3M7ZMZAH55F7KZ45YA354IDE5/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/Q3M7ZMZAH55F7KZ45YA354IDE5/action/timestamp_anchor","attest_storage":"https://pith.science/pith/Q3M7ZMZAH55F7KZ45YA354IDE5/action/storage_attestation","attest_author":"https://pith.science/pith/Q3M7ZMZAH55F7KZ45YA354IDE5/action/author_attestation","sign_citation":"https://pith.science/pith/Q3M7ZMZAH55F7KZ45YA354IDE5/action/citation_signature","submit_replication":"https://pith.science/pith/Q3M7ZMZAH55F7KZ45YA354IDE5/action/replication_record"}},"created_at":"2026-05-18T03:41:20.033797+00:00","updated_at":"2026-05-18T03:41:20.033797+00:00"}