{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2004:CDC3J7VS3YEZRC2UEXYACPXZLU","short_pith_number":"pith:CDC3J7VS","schema_version":"1.0","canonical_sha256":"10c5b4feb2de09988b5425f0013ef95d304bd06f8ac6419c6dc5cfb3fc106aee","source":{"kind":"arxiv","id":"hep-th/0412141","version":5},"attestation_state":"computed","paper":{"title":"Low energy hadron physics in holographic QCD","license":"","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-th","authors_text":"Shigeki Sugimoto, Tadakatsu Sakai","submitted_at":"2004-12-14T13:04:16Z","abstract_excerpt":"We present a holographic dual of four-dimensional, large N_c QCD with massless flavors. This model is constructed by placing N_f probe D8-branes into a D4 background, where supersymmetry is completely broken. The chiral symmetry breaking in QCD is manifested as a smooth interpolation of D8 - anti-D8 pairs in the supergravity background. The meson spectrum is examined by analyzing a five-dimensional Yang-Mills theory that originates from the non-Abelian DBI action of the probe D8-brane. It is found that our model yields massless pions, which are identified with Nambu-Goldstone bosons associated"},"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":"hep-th/0412141","kind":"arxiv","version":5},"metadata":{"license":"","primary_cat":"hep-th","submitted_at":"2004-12-14T13:04:16Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"7dedbf293fa66f1798ecef97b60487c178c66238afb466cad913b4199c286cae","abstract_canon_sha256":"8b7802832993288c6bccad4d60ddade20cc6ad117371a347182038874d6833f6"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:22:51.431927Z","signature_b64":"gTRW7hXg37vXlMAdfS6kVZLlpIYOcjRmtg5jkHQ6rwS8HWV2PI/y7rwuEsDJ87EYPvvsKijwi6kVezkWaF76BQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"10c5b4feb2de09988b5425f0013ef95d304bd06f8ac6419c6dc5cfb3fc106aee","last_reissued_at":"2026-05-18T04:22:51.431211Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:22:51.431211Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Low energy hadron physics in holographic QCD","license":"","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-th","authors_text":"Shigeki Sugimoto, Tadakatsu Sakai","submitted_at":"2004-12-14T13:04:16Z","abstract_excerpt":"We present a holographic dual of four-dimensional, large N_c QCD with massless flavors. This model is constructed by placing N_f probe D8-branes into a D4 background, where supersymmetry is completely broken. The chiral symmetry breaking in QCD is manifested as a smooth interpolation of D8 - anti-D8 pairs in the supergravity background. The meson spectrum is examined by analyzing a five-dimensional Yang-Mills theory that originates from the non-Abelian DBI action of the probe D8-brane. It is found that our model yields massless pions, which are identified with Nambu-Goldstone bosons associated"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-th/0412141","kind":"arxiv","version":5},"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":"hep-th/0412141","created_at":"2026-05-18T04:22:51.431335+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-th/0412141v5","created_at":"2026-05-18T04:22:51.431335+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-th/0412141","created_at":"2026-05-18T04:22:51.431335+00:00"},{"alias_kind":"pith_short_12","alias_value":"CDC3J7VS3YEZ","created_at":"2026-05-18T12:25:52.051335+00:00"},{"alias_kind":"pith_short_16","alias_value":"CDC3J7VS3YEZRC2U","created_at":"2026-05-18T12:25:52.051335+00:00"},{"alias_kind":"pith_short_8","alias_value":"CDC3J7VS","created_at":"2026-05-18T12:25:52.051335+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":9,"internal_anchor_count":5,"sample":[{"citing_arxiv_id":"2509.19009","citing_title":"Finite-temperature Yang-Mills theories with the density of states method: towards the continuum limit","ref_index":144,"is_internal_anchor":true},{"citing_arxiv_id":"2512.02484","citing_title":"Properties of Stable Massive Quark Stars in Holography","ref_index":28,"is_internal_anchor":true},{"citing_arxiv_id":"2512.16450","citing_title":"Learning holographic QCD with unflavoured meson spectra","ref_index":4,"is_internal_anchor":true},{"citing_arxiv_id":"2512.18274","citing_title":"High-Energy Pion Scattering in Holographic QCD: A Comparison with Experimental Data","ref_index":6,"is_internal_anchor":true},{"citing_arxiv_id":"2603.27824","citing_title":"Holographic duality from a four-fermion interaction: emergent AdS$_3$/CFT$_2$, D-branes, and Einstein gravity","ref_index":126,"is_internal_anchor":true},{"citing_arxiv_id":"2604.24046","citing_title":"Low-energy hadronic physics in holographic $\\mathrm{QCD_{3}}$ with anisotropy","ref_index":40,"is_internal_anchor":false},{"citing_arxiv_id":"2605.00203","citing_title":"Topological charges and confined-deconfined phase transition in holography","ref_index":35,"is_internal_anchor":false},{"citing_arxiv_id":"2604.14741","citing_title":"The OPE Approach to Renormalization: Operator Mixing","ref_index":30,"is_internal_anchor":false},{"citing_arxiv_id":"2605.01573","citing_title":"The atomic nucleus as a bound system of $3A$ quarks","ref_index":52,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/CDC3J7VS3YEZRC2UEXYACPXZLU","json":"https://pith.science/pith/CDC3J7VS3YEZRC2UEXYACPXZLU.json","graph_json":"https://pith.science/api/pith-number/CDC3J7VS3YEZRC2UEXYACPXZLU/graph.json","events_json":"https://pith.science/api/pith-number/CDC3J7VS3YEZRC2UEXYACPXZLU/events.json","paper":"https://pith.science/paper/CDC3J7VS"},"agent_actions":{"view_html":"https://pith.science/pith/CDC3J7VS3YEZRC2UEXYACPXZLU","download_json":"https://pith.science/pith/CDC3J7VS3YEZRC2UEXYACPXZLU.json","view_paper":"https://pith.science/paper/CDC3J7VS","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-th/0412141&json=true","fetch_graph":"https://pith.science/api/pith-number/CDC3J7VS3YEZRC2UEXYACPXZLU/graph.json","fetch_events":"https://pith.science/api/pith-number/CDC3J7VS3YEZRC2UEXYACPXZLU/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/CDC3J7VS3YEZRC2UEXYACPXZLU/action/timestamp_anchor","attest_storage":"https://pith.science/pith/CDC3J7VS3YEZRC2UEXYACPXZLU/action/storage_attestation","attest_author":"https://pith.science/pith/CDC3J7VS3YEZRC2UEXYACPXZLU/action/author_attestation","sign_citation":"https://pith.science/pith/CDC3J7VS3YEZRC2UEXYACPXZLU/action/citation_signature","submit_replication":"https://pith.science/pith/CDC3J7VS3YEZRC2UEXYACPXZLU/action/replication_record"}},"created_at":"2026-05-18T04:22:51.431335+00:00","updated_at":"2026-05-18T04:22:51.431335+00:00"}