{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:B5ROWNYPXOVFSKNRLCTS7LZGBS","short_pith_number":"pith:B5ROWNYP","schema_version":"1.0","canonical_sha256":"0f62eb370fbbaa5929b158a72faf260c8c6488c698fd4fa8f90bcc5d4ace67cd","source":{"kind":"arxiv","id":"1505.01106","version":3},"attestation_state":"computed","paper":{"title":"Hagedorn spectrum and thermodynamics of SU(2) and SU(3) Yang-Mills theories","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th","nucl-th"],"primary_cat":"hep-lat","authors_text":"Alessandro Nada, Marco Panero, Michele Caselle","submitted_at":"2015-05-05T18:19:45Z","abstract_excerpt":"We present a high-precision lattice calculation of the equation of state in the confining phase of SU(2) Yang-Mills theory. We show that the results are described very well by a gas of massive, non-interacting glueballs, provided one assumes an exponentially growing Hagedorn spectrum. The latter can be derived within an effective bosonic closed-string model, leading to a parameter-free theoretical prediction, which is in perfect agreement with our lattice results. Furthermore, when applied to SU(3) Yang-Mills theory, this effective model accurately describes the lattice results reported by Bor"},"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":"1505.01106","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-lat","submitted_at":"2015-05-05T18:19:45Z","cross_cats_sorted":["hep-th","nucl-th"],"title_canon_sha256":"92eed47e814f5df366309ab7ea3df239f31cc09185dcaad981f3b28c04850c66","abstract_canon_sha256":"5b1b69b72eea0e5a81f02ab163d94602cfad2b0e3b02f44e03aa3ebf9261a9da"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:31:52.377364Z","signature_b64":"at6PRJSbfchte0f4Hw1sewDzFR53sF07ptFX9m4gr/s4RjEZ1QpiYT1b+xUcuDMpMupX/Zm5Ulrs2anK+4TLBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0f62eb370fbbaa5929b158a72faf260c8c6488c698fd4fa8f90bcc5d4ace67cd","last_reissued_at":"2026-05-18T00:31:52.376782Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:31:52.376782Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Hagedorn spectrum and thermodynamics of SU(2) and SU(3) Yang-Mills theories","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th","nucl-th"],"primary_cat":"hep-lat","authors_text":"Alessandro Nada, Marco Panero, Michele Caselle","submitted_at":"2015-05-05T18:19:45Z","abstract_excerpt":"We present a high-precision lattice calculation of the equation of state in the confining phase of SU(2) Yang-Mills theory. We show that the results are described very well by a gas of massive, non-interacting glueballs, provided one assumes an exponentially growing Hagedorn spectrum. The latter can be derived within an effective bosonic closed-string model, leading to a parameter-free theoretical prediction, which is in perfect agreement with our lattice results. Furthermore, when applied to SU(3) Yang-Mills theory, this effective model accurately describes the lattice results reported by Bor"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1505.01106","kind":"arxiv","version":3},"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":"1505.01106","created_at":"2026-05-18T00:31:52.376872+00:00"},{"alias_kind":"arxiv_version","alias_value":"1505.01106v3","created_at":"2026-05-18T00:31:52.376872+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1505.01106","created_at":"2026-05-18T00:31:52.376872+00:00"},{"alias_kind":"pith_short_12","alias_value":"B5ROWNYPXOVF","created_at":"2026-05-18T12:29:14.074870+00:00"},{"alias_kind":"pith_short_16","alias_value":"B5ROWNYPXOVFSKNR","created_at":"2026-05-18T12:29:14.074870+00:00"},{"alias_kind":"pith_short_8","alias_value":"B5ROWNYP","created_at":"2026-05-18T12:29:14.074870+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2506.00237","citing_title":"A New State of Matter between the Hadronic Phase and the Quark-Gluon Plasma?","ref_index":47,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/B5ROWNYPXOVFSKNRLCTS7LZGBS","json":"https://pith.science/pith/B5ROWNYPXOVFSKNRLCTS7LZGBS.json","graph_json":"https://pith.science/api/pith-number/B5ROWNYPXOVFSKNRLCTS7LZGBS/graph.json","events_json":"https://pith.science/api/pith-number/B5ROWNYPXOVFSKNRLCTS7LZGBS/events.json","paper":"https://pith.science/paper/B5ROWNYP"},"agent_actions":{"view_html":"https://pith.science/pith/B5ROWNYPXOVFSKNRLCTS7LZGBS","download_json":"https://pith.science/pith/B5ROWNYPXOVFSKNRLCTS7LZGBS.json","view_paper":"https://pith.science/paper/B5ROWNYP","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1505.01106&json=true","fetch_graph":"https://pith.science/api/pith-number/B5ROWNYPXOVFSKNRLCTS7LZGBS/graph.json","fetch_events":"https://pith.science/api/pith-number/B5ROWNYPXOVFSKNRLCTS7LZGBS/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/B5ROWNYPXOVFSKNRLCTS7LZGBS/action/timestamp_anchor","attest_storage":"https://pith.science/pith/B5ROWNYPXOVFSKNRLCTS7LZGBS/action/storage_attestation","attest_author":"https://pith.science/pith/B5ROWNYPXOVFSKNRLCTS7LZGBS/action/author_attestation","sign_citation":"https://pith.science/pith/B5ROWNYPXOVFSKNRLCTS7LZGBS/action/citation_signature","submit_replication":"https://pith.science/pith/B5ROWNYPXOVFSKNRLCTS7LZGBS/action/replication_record"}},"created_at":"2026-05-18T00:31:52.376872+00:00","updated_at":"2026-05-18T00:31:52.376872+00:00"}