{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2021:M7OE45M6PTR6A63TMVYYL5ZIQC","short_pith_number":"pith:M7OE45M6","schema_version":"1.0","canonical_sha256":"67dc4e759e7ce3e07b73657185f72880afd2fcde4adcb7502d6fc1a7f14f9ed2","source":{"kind":"arxiv","id":"2107.02745","version":2},"attestation_state":"computed","paper":{"title":"Thermal monopole condensation in QCD with physical quark masses","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph","hep-th","nucl-th"],"primary_cat":"hep-lat","authors_text":"Andrea Pasqui, Marco Cardinali, Massimo D'Elia","submitted_at":"2021-07-06T17:21:57Z","abstract_excerpt":"Thermal monopoles, identified after Abelian projection as magnetic currents wrapping non-trivially around the thermal circle, are studied in $N_f = 2+1$ QCD at the physical point. The distribution in the number of wrappings, which in pure gauge theories points to a condensation temperature coinciding with deconfinement, points in this case to around 275 MeV, almost twice the QCD crossover temperature $T_c$; similar indications emerge looking for the formation of a percolating current cluster. The possible relation with other non-perturbative phenomena observed above $T_c$ is discussed."},"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":"2107.02745","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2021-07-06T17:21:57Z","cross_cats_sorted":["hep-ph","hep-th","nucl-th"],"title_canon_sha256":"ce4c9b6c4957ef3b569844815303dc6ba5b95b4fe13ebd1fe5d8b2e69e4143d9","abstract_canon_sha256":"542d5de8275036a0db599c7f4ef3d7551375e8b6ef1dee3442c41da3169b3e4b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T02:56:59.240925Z","signature_b64":"lC7mrewlM3obHy3gbf4ZKmmLafRtQSa0lfT4VZfuCLwmgqAzGT9/iCTbxhwbKsOHS5NuruIANox5JmD4nlteDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"67dc4e759e7ce3e07b73657185f72880afd2fcde4adcb7502d6fc1a7f14f9ed2","last_reissued_at":"2026-07-05T02:56:59.240427Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T02:56:59.240427Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Thermal monopole condensation in QCD with physical quark masses","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph","hep-th","nucl-th"],"primary_cat":"hep-lat","authors_text":"Andrea Pasqui, Marco Cardinali, Massimo D'Elia","submitted_at":"2021-07-06T17:21:57Z","abstract_excerpt":"Thermal monopoles, identified after Abelian projection as magnetic currents wrapping non-trivially around the thermal circle, are studied in $N_f = 2+1$ QCD at the physical point. The distribution in the number of wrappings, which in pure gauge theories points to a condensation temperature coinciding with deconfinement, points in this case to around 275 MeV, almost twice the QCD crossover temperature $T_c$; similar indications emerge looking for the formation of a percolating current cluster. The possible relation with other non-perturbative phenomena observed above $T_c$ is discussed."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2107.02745","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/2107.02745/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":"2107.02745","created_at":"2026-07-05T02:56:59.240484+00:00"},{"alias_kind":"arxiv_version","alias_value":"2107.02745v2","created_at":"2026-07-05T02:56:59.240484+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2107.02745","created_at":"2026-07-05T02:56:59.240484+00:00"},{"alias_kind":"pith_short_12","alias_value":"M7OE45M6PTR6","created_at":"2026-07-05T02:56:59.240484+00:00"},{"alias_kind":"pith_short_16","alias_value":"M7OE45M6PTR6A63T","created_at":"2026-07-05T02:56:59.240484+00:00"},{"alias_kind":"pith_short_8","alias_value":"M7OE45M6","created_at":"2026-07-05T02:56:59.240484+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2512.18830","citing_title":"Emergent chiral spin symmetry, non-perturbative dynamics and thermoparticles in hot QCD","ref_index":10,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/M7OE45M6PTR6A63TMVYYL5ZIQC","json":"https://pith.science/pith/M7OE45M6PTR6A63TMVYYL5ZIQC.json","graph_json":"https://pith.science/api/pith-number/M7OE45M6PTR6A63TMVYYL5ZIQC/graph.json","events_json":"https://pith.science/api/pith-number/M7OE45M6PTR6A63TMVYYL5ZIQC/events.json","paper":"https://pith.science/paper/M7OE45M6"},"agent_actions":{"view_html":"https://pith.science/pith/M7OE45M6PTR6A63TMVYYL5ZIQC","download_json":"https://pith.science/pith/M7OE45M6PTR6A63TMVYYL5ZIQC.json","view_paper":"https://pith.science/paper/M7OE45M6","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2107.02745&json=true","fetch_graph":"https://pith.science/api/pith-number/M7OE45M6PTR6A63TMVYYL5ZIQC/graph.json","fetch_events":"https://pith.science/api/pith-number/M7OE45M6PTR6A63TMVYYL5ZIQC/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/M7OE45M6PTR6A63TMVYYL5ZIQC/action/timestamp_anchor","attest_storage":"https://pith.science/pith/M7OE45M6PTR6A63TMVYYL5ZIQC/action/storage_attestation","attest_author":"https://pith.science/pith/M7OE45M6PTR6A63TMVYYL5ZIQC/action/author_attestation","sign_citation":"https://pith.science/pith/M7OE45M6PTR6A63TMVYYL5ZIQC/action/citation_signature","submit_replication":"https://pith.science/pith/M7OE45M6PTR6A63TMVYYL5ZIQC/action/replication_record"}},"created_at":"2026-07-05T02:56:59.240484+00:00","updated_at":"2026-07-05T02:56:59.240484+00:00"}