{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2026:KTFTRG4ICBRYCBJ7JAUESNCMXR","short_pith_number":"pith:KTFTRG4I","schema_version":"1.0","canonical_sha256":"54cb389b88106381053f482849344cbc4f125ec89c94d823a16719358ba632a9","source":{"kind":"arxiv","id":"2608.09489","version":1},"attestation_state":"computed","paper":{"title":"Effects of Born-Infeld Electrodynamics on Chiral Symmetry Restoration and Meson Susceptibilities in Holographic QCD","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-lat","hep-th"],"primary_cat":"hep-ph","authors_text":"Hiwa A. Ahmed, Peshwaz A. Abdoul","submitted_at":"2026-08-10T11:57:55Z","abstract_excerpt":"Within a holographic QCD framework, we numerically investigate chiral symmetry breaking and the associated phase transition at finite temperature and chemical potential. The model is constructed on a nonlinear charged Born-Infeld black hole background. The chiral condensate, extracted from the asymptotic behavior of the bulk scalar field, serves as the primary order parameter. At zero chemical potential, we find a chiral crossover transition for physical quark masses with a pseudocritical temperature of $T_{pc}=0.1477$ GeV. In the chiral limit, the transition becomes first-order with a critica"},"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":"2608.09489","kind":"arxiv","version":1},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2026-08-10T11:57:55Z","cross_cats_sorted":["hep-lat","hep-th"],"title_canon_sha256":"5ee06e7e6abf2b70edf0ec88a3563180f461dfc928737ff6af60698df6b5c62b","abstract_canon_sha256":"0fc0b91b0261038eb38dd254a9fa368b921fcd8c249e97ef28692a685fae1134"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-08-11T02:24:19.580800Z","signature_b64":"yGAtu+u/nSlHNg1+GqqogF19iX8RlTLvNXBBD0mFIq7TuzeLSbb0e/UQHPi8GIdE42glZ75yjssdPQeJV44OBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"54cb389b88106381053f482849344cbc4f125ec89c94d823a16719358ba632a9","last_reissued_at":"2026-08-11T02:24:19.579315Z","signature_status":"signed_v1","first_computed_at":"2026-08-11T02:24:19.579315Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Effects of Born-Infeld Electrodynamics on Chiral Symmetry Restoration and Meson Susceptibilities in Holographic QCD","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-lat","hep-th"],"primary_cat":"hep-ph","authors_text":"Hiwa A. Ahmed, Peshwaz A. Abdoul","submitted_at":"2026-08-10T11:57:55Z","abstract_excerpt":"Within a holographic QCD framework, we numerically investigate chiral symmetry breaking and the associated phase transition at finite temperature and chemical potential. The model is constructed on a nonlinear charged Born-Infeld black hole background. The chiral condensate, extracted from the asymptotic behavior of the bulk scalar field, serves as the primary order parameter. At zero chemical potential, we find a chiral crossover transition for physical quark masses with a pseudocritical temperature of $T_{pc}=0.1477$ GeV. In the chiral limit, the transition becomes first-order with a critica"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2608.09489","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2608.09489/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":"2608.09489","created_at":"2026-08-11T02:24:19.579890+00:00"},{"alias_kind":"arxiv_version","alias_value":"2608.09489v1","created_at":"2026-08-11T02:24:19.579890+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2608.09489","created_at":"2026-08-11T02:24:19.579890+00:00"},{"alias_kind":"pith_short_12","alias_value":"KTFTRG4ICBRY","created_at":"2026-08-11T02:24:19.579890+00:00"},{"alias_kind":"pith_short_16","alias_value":"KTFTRG4ICBRYCBJ7","created_at":"2026-08-11T02:24:19.579890+00:00"},{"alias_kind":"pith_short_8","alias_value":"KTFTRG4I","created_at":"2026-08-11T02:24:19.579890+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/KTFTRG4ICBRYCBJ7JAUESNCMXR","json":"https://pith.science/pith/KTFTRG4ICBRYCBJ7JAUESNCMXR.json","graph_json":"https://pith.science/api/pith-number/KTFTRG4ICBRYCBJ7JAUESNCMXR/graph.json","events_json":"https://pith.science/api/pith-number/KTFTRG4ICBRYCBJ7JAUESNCMXR/events.json","paper":"https://pith.science/paper/KTFTRG4I"},"agent_actions":{"view_html":"https://pith.science/pith/KTFTRG4ICBRYCBJ7JAUESNCMXR","download_json":"https://pith.science/pith/KTFTRG4ICBRYCBJ7JAUESNCMXR.json","view_paper":"https://pith.science/paper/KTFTRG4I","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2608.09489&json=true","fetch_graph":"https://pith.science/api/pith-number/KTFTRG4ICBRYCBJ7JAUESNCMXR/graph.json","fetch_events":"https://pith.science/api/pith-number/KTFTRG4ICBRYCBJ7JAUESNCMXR/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/KTFTRG4ICBRYCBJ7JAUESNCMXR/action/timestamp_anchor","attest_storage":"https://pith.science/pith/KTFTRG4ICBRYCBJ7JAUESNCMXR/action/storage_attestation","attest_author":"https://pith.science/pith/KTFTRG4ICBRYCBJ7JAUESNCMXR/action/author_attestation","sign_citation":"https://pith.science/pith/KTFTRG4ICBRYCBJ7JAUESNCMXR/action/citation_signature","submit_replication":"https://pith.science/pith/KTFTRG4ICBRYCBJ7JAUESNCMXR/action/replication_record"}},"created_at":"2026-08-11T02:24:19.579890+00:00","updated_at":"2026-08-11T02:24:19.579890+00:00"}