{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2018:NZG745ZT2OFVS5XQK3BBYRS6QN","short_pith_number":"pith:NZG745ZT","schema_version":"1.0","canonical_sha256":"6e4dfe7733d38b5976f056c21c465e8370ff081c3d17cffc634b5819b8e756f2","source":{"kind":"arxiv","id":"1809.07730","version":2},"attestation_state":"computed","paper":{"title":"Glueballs and deconfinement temperature in AdS/QCD","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"hep-ph","authors_text":"A.D. Katanaeva, S.S. Afonin","submitted_at":"2018-09-20T16:45:41Z","abstract_excerpt":"We put forward an alternative way to estimate the deconfinement temperature in bottom-up holographic models. The deconfinement in AdS/QCD is related to the Hawking-Page phase transition, in which the critical Hawking temperature is identified with the deconfinement one in the gauge theory. The numeric estimation of the latter is only possible when the parameters of a $5D$ dual model are previously determined from consistency with other physical aspects, standardly, providing a description of the QCD resonances. The traditional way to fix parameters in the simplest AdS/QCD models is to reproduc"},"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":"1809.07730","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2018-09-20T16:45:41Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"99809b347dd654f1ba43d25666f3aaf4598ceb39b0208358530ca8e931044c7c","abstract_canon_sha256":"5f0eef5b895f067f88aa384388936bdf39769588334265524b2b222646b3a371"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:56:35.066252Z","signature_b64":"ttCb77j+lgmNp4/q/hzJrC63slBzgllmOmHqGNqyC8D2tGhYFkOiPgZVDIJMM1sNU/xZosgh/FrIBSN4IhOvDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6e4dfe7733d38b5976f056c21c465e8370ff081c3d17cffc634b5819b8e756f2","last_reissued_at":"2026-05-17T23:56:35.065695Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:56:35.065695Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Glueballs and deconfinement temperature in AdS/QCD","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"hep-ph","authors_text":"A.D. Katanaeva, S.S. Afonin","submitted_at":"2018-09-20T16:45:41Z","abstract_excerpt":"We put forward an alternative way to estimate the deconfinement temperature in bottom-up holographic models. The deconfinement in AdS/QCD is related to the Hawking-Page phase transition, in which the critical Hawking temperature is identified with the deconfinement one in the gauge theory. The numeric estimation of the latter is only possible when the parameters of a $5D$ dual model are previously determined from consistency with other physical aspects, standardly, providing a description of the QCD resonances. The traditional way to fix parameters in the simplest AdS/QCD models is to reproduc"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1809.07730","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":""},"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":"1809.07730","created_at":"2026-05-17T23:56:35.065791+00:00"},{"alias_kind":"arxiv_version","alias_value":"1809.07730v2","created_at":"2026-05-17T23:56:35.065791+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1809.07730","created_at":"2026-05-17T23:56:35.065791+00:00"},{"alias_kind":"pith_short_12","alias_value":"NZG745ZT2OFV","created_at":"2026-05-18T12:32:40.477152+00:00"},{"alias_kind":"pith_short_16","alias_value":"NZG745ZT2OFVS5XQ","created_at":"2026-05-18T12:32:40.477152+00:00"},{"alias_kind":"pith_short_8","alias_value":"NZG745ZT","created_at":"2026-05-18T12:32:40.477152+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/NZG745ZT2OFVS5XQK3BBYRS6QN","json":"https://pith.science/pith/NZG745ZT2OFVS5XQK3BBYRS6QN.json","graph_json":"https://pith.science/api/pith-number/NZG745ZT2OFVS5XQK3BBYRS6QN/graph.json","events_json":"https://pith.science/api/pith-number/NZG745ZT2OFVS5XQK3BBYRS6QN/events.json","paper":"https://pith.science/paper/NZG745ZT"},"agent_actions":{"view_html":"https://pith.science/pith/NZG745ZT2OFVS5XQK3BBYRS6QN","download_json":"https://pith.science/pith/NZG745ZT2OFVS5XQK3BBYRS6QN.json","view_paper":"https://pith.science/paper/NZG745ZT","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1809.07730&json=true","fetch_graph":"https://pith.science/api/pith-number/NZG745ZT2OFVS5XQK3BBYRS6QN/graph.json","fetch_events":"https://pith.science/api/pith-number/NZG745ZT2OFVS5XQK3BBYRS6QN/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/NZG745ZT2OFVS5XQK3BBYRS6QN/action/timestamp_anchor","attest_storage":"https://pith.science/pith/NZG745ZT2OFVS5XQK3BBYRS6QN/action/storage_attestation","attest_author":"https://pith.science/pith/NZG745ZT2OFVS5XQK3BBYRS6QN/action/author_attestation","sign_citation":"https://pith.science/pith/NZG745ZT2OFVS5XQK3BBYRS6QN/action/citation_signature","submit_replication":"https://pith.science/pith/NZG745ZT2OFVS5XQK3BBYRS6QN/action/replication_record"}},"created_at":"2026-05-17T23:56:35.065791+00:00","updated_at":"2026-05-17T23:56:35.065791+00:00"}