{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2019:ODYVFR5ZKL5SPKIOMCYR45GLHZ","short_pith_number":"pith:ODYVFR5Z","schema_version":"1.0","canonical_sha256":"70f152c7b952fb27a90e60b11e74cb3e598ecf6d3d4362898b582ebad54dd865","source":{"kind":"arxiv","id":"1907.11809","version":2},"attestation_state":"computed","paper":{"title":"Tensor mesons, AdS/QCD and information","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-th","authors_text":"Luiz F. Ferreira, Roldao da Rocha","submitted_at":"2019-07-26T22:47:24Z","abstract_excerpt":"The Kaluza-Klein tower of higher spin-$S$ tensor meson resonances is here scrutinized in the AdS/QCD hard wall model, encompassing the already established resonances $\\rho(770)$, $f_2(1270)$, $\\omega_3(1670)$, $f_4(2050)$, $\\rho_5(2350)$, $f_6(2510)$ in PDG. A hybrid model employs both information theory and AdS/QCD, where configurational-entropic Regge trajectories, relating the configurational entropy of the tensor mesons family to their $S$ spin, and also to their experimental mass spectra, are derived and analyzed. Therefore, the mass spectra of higher spin-$S$ tensor meson resonances is o"},"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":"1907.11809","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-th","submitted_at":"2019-07-26T22:47:24Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"a5bad2b2f85b639fa2f53ec75e4f60467e1d5ca99580594ef33a095852f90962","abstract_canon_sha256":"90ba260c5d5787cc895a66829a39d24f4800d6c7127a5188c9011ba1cc1d9e01"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T01:01:20.336599Z","signature_b64":"qAwAb8iDNGhgrCtqQiUEtWc/pnH4hNTBTBlL6A8XeSMPcm5S3nNeXdqAQwrQDEGYEjbBH4UhMiXH0vWJGO8BBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"70f152c7b952fb27a90e60b11e74cb3e598ecf6d3d4362898b582ebad54dd865","last_reissued_at":"2026-07-05T01:01:20.336177Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T01:01:20.336177Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Tensor mesons, AdS/QCD and information","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"hep-th","authors_text":"Luiz F. Ferreira, Roldao da Rocha","submitted_at":"2019-07-26T22:47:24Z","abstract_excerpt":"The Kaluza-Klein tower of higher spin-$S$ tensor meson resonances is here scrutinized in the AdS/QCD hard wall model, encompassing the already established resonances $\\rho(770)$, $f_2(1270)$, $\\omega_3(1670)$, $f_4(2050)$, $\\rho_5(2350)$, $f_6(2510)$ in PDG. A hybrid model employs both information theory and AdS/QCD, where configurational-entropic Regge trajectories, relating the configurational entropy of the tensor mesons family to their $S$ spin, and also to their experimental mass spectra, are derived and analyzed. Therefore, the mass spectra of higher spin-$S$ tensor meson resonances is o"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1907.11809","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/1907.11809/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":"1907.11809","created_at":"2026-07-05T01:01:20.336236+00:00"},{"alias_kind":"arxiv_version","alias_value":"1907.11809v2","created_at":"2026-07-05T01:01:20.336236+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1907.11809","created_at":"2026-07-05T01:01:20.336236+00:00"},{"alias_kind":"pith_short_12","alias_value":"ODYVFR5ZKL5S","created_at":"2026-07-05T01:01:20.336236+00:00"},{"alias_kind":"pith_short_16","alias_value":"ODYVFR5ZKL5SPKIO","created_at":"2026-07-05T01:01:20.336236+00:00"},{"alias_kind":"pith_short_8","alias_value":"ODYVFR5Z","created_at":"2026-07-05T01:01:20.336236+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2501.01755","citing_title":"Confining potential in holographic bottom-up QCD from WKB","ref_index":35,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/ODYVFR5ZKL5SPKIOMCYR45GLHZ","json":"https://pith.science/pith/ODYVFR5ZKL5SPKIOMCYR45GLHZ.json","graph_json":"https://pith.science/api/pith-number/ODYVFR5ZKL5SPKIOMCYR45GLHZ/graph.json","events_json":"https://pith.science/api/pith-number/ODYVFR5ZKL5SPKIOMCYR45GLHZ/events.json","paper":"https://pith.science/paper/ODYVFR5Z"},"agent_actions":{"view_html":"https://pith.science/pith/ODYVFR5ZKL5SPKIOMCYR45GLHZ","download_json":"https://pith.science/pith/ODYVFR5ZKL5SPKIOMCYR45GLHZ.json","view_paper":"https://pith.science/paper/ODYVFR5Z","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1907.11809&json=true","fetch_graph":"https://pith.science/api/pith-number/ODYVFR5ZKL5SPKIOMCYR45GLHZ/graph.json","fetch_events":"https://pith.science/api/pith-number/ODYVFR5ZKL5SPKIOMCYR45GLHZ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ODYVFR5ZKL5SPKIOMCYR45GLHZ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ODYVFR5ZKL5SPKIOMCYR45GLHZ/action/storage_attestation","attest_author":"https://pith.science/pith/ODYVFR5ZKL5SPKIOMCYR45GLHZ/action/author_attestation","sign_citation":"https://pith.science/pith/ODYVFR5ZKL5SPKIOMCYR45GLHZ/action/citation_signature","submit_replication":"https://pith.science/pith/ODYVFR5ZKL5SPKIOMCYR45GLHZ/action/replication_record"}},"created_at":"2026-07-05T01:01:20.336236+00:00","updated_at":"2026-07-05T01:01:20.336236+00:00"}