{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:4UNW5QSRSPKUF2STMEYGEMABKP","short_pith_number":"pith:4UNW5QSR","schema_version":"1.0","canonical_sha256":"e51b6ec25193d542ea53613062300153f66efca00b357764801fa985bdf67c7c","source":{"kind":"arxiv","id":"1807.08105","version":1},"attestation_state":"computed","paper":{"title":"Confinement Horizon and QCD Entropy","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc","hep-th"],"primary_cat":"hep-ph","authors_text":"Alfredo Iorio, Paolo Castorina","submitted_at":"2018-07-21T08:12:22Z","abstract_excerpt":"Within the picture of quark confinement as due to a \\textit{color event horizon}, and of hadronization as an instance of the Unruh radiation for the strong force, we show here that QCD entropy, evaluated by lattice simulations in the region $T_c < T < 1.3 T_c$, is in reasonable agreement with a melting color event horizon."},"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":"1807.08105","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-07-21T08:12:22Z","cross_cats_sorted":["gr-qc","hep-th"],"title_canon_sha256":"9ff6af62f1cd86e0779e85de26ddeee5556bc3adaabd4a324b14501124be2171","abstract_canon_sha256":"704f799558f768473e40ba8ec1908743877bfc0429da159aaf2d206177297d77"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:55:55.942779Z","signature_b64":"sk29efUSDFmmtmP4KODz2s4dYed3VuziC4JmXK9JcMBtDiqLbcWDc3jpDSLsYuXJ3Nf93jOY87W1qEJ+5ld1BA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"e51b6ec25193d542ea53613062300153f66efca00b357764801fa985bdf67c7c","last_reissued_at":"2026-05-17T23:55:55.942099Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:55:55.942099Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Confinement Horizon and QCD Entropy","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["gr-qc","hep-th"],"primary_cat":"hep-ph","authors_text":"Alfredo Iorio, Paolo Castorina","submitted_at":"2018-07-21T08:12:22Z","abstract_excerpt":"Within the picture of quark confinement as due to a \\textit{color event horizon}, and of hadronization as an instance of the Unruh radiation for the strong force, we show here that QCD entropy, evaluated by lattice simulations in the region $T_c < T < 1.3 T_c$, is in reasonable agreement with a melting color event horizon."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1807.08105","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":"1807.08105","created_at":"2026-05-17T23:55:55.942205+00:00"},{"alias_kind":"arxiv_version","alias_value":"1807.08105v1","created_at":"2026-05-17T23:55:55.942205+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1807.08105","created_at":"2026-05-17T23:55:55.942205+00:00"},{"alias_kind":"pith_short_12","alias_value":"4UNW5QSRSPKU","created_at":"2026-05-18T12:32:05.422762+00:00"},{"alias_kind":"pith_short_16","alias_value":"4UNW5QSRSPKUF2ST","created_at":"2026-05-18T12:32:05.422762+00:00"},{"alias_kind":"pith_short_8","alias_value":"4UNW5QSR","created_at":"2026-05-18T12:32:05.422762+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/4UNW5QSRSPKUF2STMEYGEMABKP","json":"https://pith.science/pith/4UNW5QSRSPKUF2STMEYGEMABKP.json","graph_json":"https://pith.science/api/pith-number/4UNW5QSRSPKUF2STMEYGEMABKP/graph.json","events_json":"https://pith.science/api/pith-number/4UNW5QSRSPKUF2STMEYGEMABKP/events.json","paper":"https://pith.science/paper/4UNW5QSR"},"agent_actions":{"view_html":"https://pith.science/pith/4UNW5QSRSPKUF2STMEYGEMABKP","download_json":"https://pith.science/pith/4UNW5QSRSPKUF2STMEYGEMABKP.json","view_paper":"https://pith.science/paper/4UNW5QSR","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1807.08105&json=true","fetch_graph":"https://pith.science/api/pith-number/4UNW5QSRSPKUF2STMEYGEMABKP/graph.json","fetch_events":"https://pith.science/api/pith-number/4UNW5QSRSPKUF2STMEYGEMABKP/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/4UNW5QSRSPKUF2STMEYGEMABKP/action/timestamp_anchor","attest_storage":"https://pith.science/pith/4UNW5QSRSPKUF2STMEYGEMABKP/action/storage_attestation","attest_author":"https://pith.science/pith/4UNW5QSRSPKUF2STMEYGEMABKP/action/author_attestation","sign_citation":"https://pith.science/pith/4UNW5QSRSPKUF2STMEYGEMABKP/action/citation_signature","submit_replication":"https://pith.science/pith/4UNW5QSRSPKUF2STMEYGEMABKP/action/replication_record"}},"created_at":"2026-05-17T23:55:55.942205+00:00","updated_at":"2026-05-17T23:55:55.942205+00:00"}