{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:KUCPY4ZZFHU73A7PYNBDJ5YFUS","short_pith_number":"pith:KUCPY4ZZ","schema_version":"1.0","canonical_sha256":"5504fc733929e9fd83efc34234f705a4bd966ce70af7f1deb41b3d0db19af732","source":{"kind":"arxiv","id":"2402.11959","version":1},"attestation_state":"computed","paper":{"title":"Hybrid spectroscopy within the Graviton Soft-Wall model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Matteo Rinaldi, Vicente Vento","submitted_at":"2024-02-19T09:01:03Z","abstract_excerpt":"In this analysis, the so-called holographic graviton soft-wall model (GSW), first developed to investigate the glueball spectrum, has been adopted to predict the masses of hybrids with different quantum numbers. Results have been compared with other models and lattice calculations. We have extended the GSW model by introducing two modifications based on anomalous dimensions in order to improve our agreement with other calculations and to remove the initial degeneracy not accounted for by lattice predictions. These modifications do not involve new parameters. The next step has been to identify "},"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":"2402.11959","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2024-02-19T09:01:03Z","cross_cats_sorted":[],"title_canon_sha256":"ee7311caf09e227a479384f24cfe4dd96edf658e8d2abcd007e9bccf69213529","abstract_canon_sha256":"828e75b7dcc9736aa2a2b5555bd72f342096ace1beea8960339b7dc4c4319d35"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T07:46:46.599923Z","signature_b64":"QbWELKGHOqdXZ44CRByfS/iZzlx8lmYKyZKep4WVy1KYE0jGlD4W9QYN+ijxpjJAdNWNtGxSbPO4JyX0H7/lAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"5504fc733929e9fd83efc34234f705a4bd966ce70af7f1deb41b3d0db19af732","last_reissued_at":"2026-07-05T07:46:46.599405Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T07:46:46.599405Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Hybrid spectroscopy within the Graviton Soft-Wall model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Matteo Rinaldi, Vicente Vento","submitted_at":"2024-02-19T09:01:03Z","abstract_excerpt":"In this analysis, the so-called holographic graviton soft-wall model (GSW), first developed to investigate the glueball spectrum, has been adopted to predict the masses of hybrids with different quantum numbers. Results have been compared with other models and lattice calculations. We have extended the GSW model by introducing two modifications based on anomalous dimensions in order to improve our agreement with other calculations and to remove the initial degeneracy not accounted for by lattice predictions. These modifications do not involve new parameters. The next step has been to identify "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2402.11959","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/2402.11959/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":"2402.11959","created_at":"2026-07-05T07:46:46.599477+00:00"},{"alias_kind":"arxiv_version","alias_value":"2402.11959v1","created_at":"2026-07-05T07:46:46.599477+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2402.11959","created_at":"2026-07-05T07:46:46.599477+00:00"},{"alias_kind":"pith_short_12","alias_value":"KUCPY4ZZFHU7","created_at":"2026-07-05T07:46:46.599477+00:00"},{"alias_kind":"pith_short_16","alias_value":"KUCPY4ZZFHU73A7P","created_at":"2026-07-05T07:46:46.599477+00:00"},{"alias_kind":"pith_short_8","alias_value":"KUCPY4ZZ","created_at":"2026-07-05T07:46:46.599477+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2602.08605","citing_title":"Holographic information measures for spin-$3/2$ $\\Delta$ baryons in AdS/QCD","ref_index":18,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/KUCPY4ZZFHU73A7PYNBDJ5YFUS","json":"https://pith.science/pith/KUCPY4ZZFHU73A7PYNBDJ5YFUS.json","graph_json":"https://pith.science/api/pith-number/KUCPY4ZZFHU73A7PYNBDJ5YFUS/graph.json","events_json":"https://pith.science/api/pith-number/KUCPY4ZZFHU73A7PYNBDJ5YFUS/events.json","paper":"https://pith.science/paper/KUCPY4ZZ"},"agent_actions":{"view_html":"https://pith.science/pith/KUCPY4ZZFHU73A7PYNBDJ5YFUS","download_json":"https://pith.science/pith/KUCPY4ZZFHU73A7PYNBDJ5YFUS.json","view_paper":"https://pith.science/paper/KUCPY4ZZ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2402.11959&json=true","fetch_graph":"https://pith.science/api/pith-number/KUCPY4ZZFHU73A7PYNBDJ5YFUS/graph.json","fetch_events":"https://pith.science/api/pith-number/KUCPY4ZZFHU73A7PYNBDJ5YFUS/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/KUCPY4ZZFHU73A7PYNBDJ5YFUS/action/timestamp_anchor","attest_storage":"https://pith.science/pith/KUCPY4ZZFHU73A7PYNBDJ5YFUS/action/storage_attestation","attest_author":"https://pith.science/pith/KUCPY4ZZFHU73A7PYNBDJ5YFUS/action/author_attestation","sign_citation":"https://pith.science/pith/KUCPY4ZZFHU73A7PYNBDJ5YFUS/action/citation_signature","submit_replication":"https://pith.science/pith/KUCPY4ZZFHU73A7PYNBDJ5YFUS/action/replication_record"}},"created_at":"2026-07-05T07:46:46.599477+00:00","updated_at":"2026-07-05T07:46:46.599477+00:00"}