{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2008:V46QBAEZZARHCLRXE3WQEI5RTK","short_pith_number":"pith:V46QBAEZ","schema_version":"1.0","canonical_sha256":"af3d008099c822712e3726ed0223b19ab6457b62365ceb1222d748032bfe8f5f","source":{"kind":"arxiv","id":"0806.3830","version":2},"attestation_state":"computed","paper":{"title":"Dynamical holographic QCD with area-law confinement and linear Regge trajectories","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-lat","hep-th"],"primary_cat":"hep-ph","authors_text":"H. Forkel, M. Beyer, T. Frederico, W. de Paula","submitted_at":"2008-06-24T07:46:49Z","abstract_excerpt":"We construct a new solution of five-dimensional gravity coupled to a dilaton which encodes essential features of holographic QCD backgrounds dynamically. In particular, it implements linear confinement, i.e. the area law behavior of the Wilson loop, by means of a dynamically deformed anti-de Sitter metric. The predicted square masses of the light-flavored natural-parity mesons and their excitations lie on linear trajectories of approximately universal slope with respect to both radial and spin quantum numbers and are in satisfactory agreement with experimental data."},"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":"0806.3830","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2008-06-24T07:46:49Z","cross_cats_sorted":["hep-lat","hep-th"],"title_canon_sha256":"fbb25eac5638198caf2256a239f3898c40b357df9b49dfa28c94b5bf44a1058f","abstract_canon_sha256":"57ad2f0111e1c4078b96859ecd86aecf8248cc82d2b7721cca96ad645602f7c7"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:46:21.000571Z","signature_b64":"SvQXL1yLLBtbfcs2eD1gPpTPeCuVsU0yaUBH9q+n/C/P7p2wqNy1/S1nbsgQxXnN6eXTTIs9Vlvx6o7eGnhNAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"af3d008099c822712e3726ed0223b19ab6457b62365ceb1222d748032bfe8f5f","last_reissued_at":"2026-07-04T15:46:21.000105Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:46:21.000105Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Dynamical holographic QCD with area-law confinement and linear Regge trajectories","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-lat","hep-th"],"primary_cat":"hep-ph","authors_text":"H. Forkel, M. Beyer, T. Frederico, W. de Paula","submitted_at":"2008-06-24T07:46:49Z","abstract_excerpt":"We construct a new solution of five-dimensional gravity coupled to a dilaton which encodes essential features of holographic QCD backgrounds dynamically. In particular, it implements linear confinement, i.e. the area law behavior of the Wilson loop, by means of a dynamically deformed anti-de Sitter metric. The predicted square masses of the light-flavored natural-parity mesons and their excitations lie on linear trajectories of approximately universal slope with respect to both radial and spin quantum numbers and are in satisfactory agreement with experimental data."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"0806.3830","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/0806.3830/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":"0806.3830","created_at":"2026-07-04T15:46:21.000162+00:00"},{"alias_kind":"arxiv_version","alias_value":"0806.3830v2","created_at":"2026-07-04T15:46:21.000162+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.0806.3830","created_at":"2026-07-04T15:46:21.000162+00:00"},{"alias_kind":"pith_short_12","alias_value":"V46QBAEZZARH","created_at":"2026-07-04T15:46:21.000162+00:00"},{"alias_kind":"pith_short_16","alias_value":"V46QBAEZZARHCLRX","created_at":"2026-07-04T15:46:21.000162+00:00"},{"alias_kind":"pith_short_8","alias_value":"V46QBAEZ","created_at":"2026-07-04T15:46:21.000162+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2602.08605","citing_title":"Holographic information measures for spin-$3/2$ $\\Delta$ baryons in AdS/QCD","ref_index":16,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/V46QBAEZZARHCLRXE3WQEI5RTK","json":"https://pith.science/pith/V46QBAEZZARHCLRXE3WQEI5RTK.json","graph_json":"https://pith.science/api/pith-number/V46QBAEZZARHCLRXE3WQEI5RTK/graph.json","events_json":"https://pith.science/api/pith-number/V46QBAEZZARHCLRXE3WQEI5RTK/events.json","paper":"https://pith.science/paper/V46QBAEZ"},"agent_actions":{"view_html":"https://pith.science/pith/V46QBAEZZARHCLRXE3WQEI5RTK","download_json":"https://pith.science/pith/V46QBAEZZARHCLRXE3WQEI5RTK.json","view_paper":"https://pith.science/paper/V46QBAEZ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=0806.3830&json=true","fetch_graph":"https://pith.science/api/pith-number/V46QBAEZZARHCLRXE3WQEI5RTK/graph.json","fetch_events":"https://pith.science/api/pith-number/V46QBAEZZARHCLRXE3WQEI5RTK/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/V46QBAEZZARHCLRXE3WQEI5RTK/action/timestamp_anchor","attest_storage":"https://pith.science/pith/V46QBAEZZARHCLRXE3WQEI5RTK/action/storage_attestation","attest_author":"https://pith.science/pith/V46QBAEZZARHCLRXE3WQEI5RTK/action/author_attestation","sign_citation":"https://pith.science/pith/V46QBAEZZARHCLRXE3WQEI5RTK/action/citation_signature","submit_replication":"https://pith.science/pith/V46QBAEZZARHCLRXE3WQEI5RTK/action/replication_record"}},"created_at":"2026-07-04T15:46:21.000162+00:00","updated_at":"2026-07-04T15:46:21.000162+00:00"}