{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:JNBWMJUSFXSYXUI2V2LJMSDT7V","short_pith_number":"pith:JNBWMJUS","schema_version":"1.0","canonical_sha256":"4b436626922de58bd11aae96964873fd6cee4d8514dddb68b797ca82d6553331","source":{"kind":"arxiv","id":"1501.00959","version":2},"attestation_state":"computed","paper":{"title":"Superconformal Baryon-Meson Symmetry and Light-Front Holographic QCD","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-th","authors_text":"Guy F. de Teramond, Hans Gunter Dosch, Stanley J. Brodsky","submitted_at":"2015-01-05T20:03:21Z","abstract_excerpt":"We construct an effective QCD light-front Hamiltonian for both mesons and baryons in the chiral limit based on the generalized supercharges of a superconformal graded algebra. The superconformal construction is shown to be equivalent to a semi-classical approximation to light-front QCD and its embedding in AdS space. The specific breaking of conformal invariance inside the graded algebra uniquely determines the effective confinement potential. The generalized supercharges connect the baryon and meson spectra to each other in a remarkable manner. In particular, the $\\pi/b_1$ Regge trajectory is"},"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":"1501.00959","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2015-01-05T20:03:21Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"5f6966704930d7478fea0fba286e1566263b1f8a738c4a58c4b006bf952c6e75","abstract_canon_sha256":"6d4ef5cdeea4ec6d566ce11c46e770234361810dd62b03f5c9eb49c5c803eea4"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:18:43.016843Z","signature_b64":"18Ln0nKqBeF2O3Yb87N3spaBEypOOLBaRoXLQBLJb0aCrqWwNWyCADY93fcrkjYiDgPNhuoibNrl6wwQNpj6Bw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4b436626922de58bd11aae96964873fd6cee4d8514dddb68b797ca82d6553331","last_reissued_at":"2026-05-18T02:18:43.016120Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:18:43.016120Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Superconformal Baryon-Meson Symmetry and Light-Front Holographic QCD","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-th","authors_text":"Guy F. de Teramond, Hans Gunter Dosch, Stanley J. Brodsky","submitted_at":"2015-01-05T20:03:21Z","abstract_excerpt":"We construct an effective QCD light-front Hamiltonian for both mesons and baryons in the chiral limit based on the generalized supercharges of a superconformal graded algebra. The superconformal construction is shown to be equivalent to a semi-classical approximation to light-front QCD and its embedding in AdS space. The specific breaking of conformal invariance inside the graded algebra uniquely determines the effective confinement potential. The generalized supercharges connect the baryon and meson spectra to each other in a remarkable manner. In particular, the $\\pi/b_1$ Regge trajectory is"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1501.00959","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":"1501.00959","created_at":"2026-05-18T02:18:43.016224+00:00"},{"alias_kind":"arxiv_version","alias_value":"1501.00959v2","created_at":"2026-05-18T02:18:43.016224+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1501.00959","created_at":"2026-05-18T02:18:43.016224+00:00"},{"alias_kind":"pith_short_12","alias_value":"JNBWMJUSFXSY","created_at":"2026-05-18T12:29:27.538025+00:00"},{"alias_kind":"pith_short_16","alias_value":"JNBWMJUSFXSYXUI2","created_at":"2026-05-18T12:29:27.538025+00:00"},{"alias_kind":"pith_short_8","alias_value":"JNBWMJUS","created_at":"2026-05-18T12:29:27.538025+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":2,"sample":[{"citing_arxiv_id":"2601.19141","citing_title":"Origin of the nucleon gravitational form factor $B_N(t)$: Exposition in light-front holographic QCD","ref_index":52,"is_internal_anchor":true},{"citing_arxiv_id":"2603.23818","citing_title":"Regge spectral generator and form factors from hard exclusive amplitudes in holographic QCD","ref_index":13,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/JNBWMJUSFXSYXUI2V2LJMSDT7V","json":"https://pith.science/pith/JNBWMJUSFXSYXUI2V2LJMSDT7V.json","graph_json":"https://pith.science/api/pith-number/JNBWMJUSFXSYXUI2V2LJMSDT7V/graph.json","events_json":"https://pith.science/api/pith-number/JNBWMJUSFXSYXUI2V2LJMSDT7V/events.json","paper":"https://pith.science/paper/JNBWMJUS"},"agent_actions":{"view_html":"https://pith.science/pith/JNBWMJUSFXSYXUI2V2LJMSDT7V","download_json":"https://pith.science/pith/JNBWMJUSFXSYXUI2V2LJMSDT7V.json","view_paper":"https://pith.science/paper/JNBWMJUS","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1501.00959&json=true","fetch_graph":"https://pith.science/api/pith-number/JNBWMJUSFXSYXUI2V2LJMSDT7V/graph.json","fetch_events":"https://pith.science/api/pith-number/JNBWMJUSFXSYXUI2V2LJMSDT7V/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/JNBWMJUSFXSYXUI2V2LJMSDT7V/action/timestamp_anchor","attest_storage":"https://pith.science/pith/JNBWMJUSFXSYXUI2V2LJMSDT7V/action/storage_attestation","attest_author":"https://pith.science/pith/JNBWMJUSFXSYXUI2V2LJMSDT7V/action/author_attestation","sign_citation":"https://pith.science/pith/JNBWMJUSFXSYXUI2V2LJMSDT7V/action/citation_signature","submit_replication":"https://pith.science/pith/JNBWMJUSFXSYXUI2V2LJMSDT7V/action/replication_record"}},"created_at":"2026-05-18T02:18:43.016224+00:00","updated_at":"2026-05-18T02:18:43.016224+00:00"}