{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1999:TMBZE6LWUYMFY5RYYVLXVF36XF","short_pith_number":"pith:TMBZE6LW","schema_version":"1.0","canonical_sha256":"9b03927976a6185c7638c5577a977eb950bcc0e38ba66b11709889392d628e25","source":{"kind":"arxiv","id":"nucl-th/9905056","version":2},"attestation_state":"computed","paper":{"title":"Bethe-Salpeter Study of Vector Meson Masses and Decay Constants","license":"","headline":"","cross_cats":["hep-ph"],"primary_cat":"nucl-th","authors_text":"Peter. C. Tandy (Kent State University), Pieter Maris","submitted_at":"1999-05-26T21:51:48Z","abstract_excerpt":"The masses and decay constants of the light vector mesons $\\rho/\\omega$, $\\phi$ and $K^\\star$ are studied within a ladder-rainbow truncation of the coupled Dyson-Schwinger and Bethe-Salpeter equations of QCD with a model 2-point gluon function. The approach is consistent with quark and gluon confinement, reproduces the correct one-loop renormalization group behavior of QCD, generates dynamical chiral symmetry breaking, and preserves the relevant Ward identities. The one phenomenological parameter and two current quark masses are fixed by requiring that the calculated $f_\\pi, m_\\pi$ and $m_K$ a"},"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":"nucl-th/9905056","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"nucl-th","submitted_at":"1999-05-26T21:51:48Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"531c215abb760cf88f51afed3a5b53df6f0338f840f06bf59a9ae708503f268c","abstract_canon_sha256":"4d9c156ec13c076fd6283f636ad5b59a42bfb8cb19469fc868755934f7ec8835"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:15:23.385204Z","signature_b64":"j1Q3k7gKaw7bW29WhXpMAItmE4n2YmDeCzf0Bo8JeixUNrvo04fkyXt724Jz6GOvlW2Id9aaRnqIWM1fS6dyCg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9b03927976a6185c7638c5577a977eb950bcc0e38ba66b11709889392d628e25","last_reissued_at":"2026-07-04T16:15:23.384796Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:15:23.384796Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Bethe-Salpeter Study of Vector Meson Masses and Decay Constants","license":"","headline":"","cross_cats":["hep-ph"],"primary_cat":"nucl-th","authors_text":"Peter. C. Tandy (Kent State University), Pieter Maris","submitted_at":"1999-05-26T21:51:48Z","abstract_excerpt":"The masses and decay constants of the light vector mesons $\\rho/\\omega$, $\\phi$ and $K^\\star$ are studied within a ladder-rainbow truncation of the coupled Dyson-Schwinger and Bethe-Salpeter equations of QCD with a model 2-point gluon function. The approach is consistent with quark and gluon confinement, reproduces the correct one-loop renormalization group behavior of QCD, generates dynamical chiral symmetry breaking, and preserves the relevant Ward identities. The one phenomenological parameter and two current quark masses are fixed by requiring that the calculated $f_\\pi, m_\\pi$ and $m_K$ a"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"nucl-th/9905056","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/nucl-th/9905056/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":"nucl-th/9905056","created_at":"2026-07-04T16:15:23.384854+00:00"},{"alias_kind":"arxiv_version","alias_value":"nucl-th/9905056v2","created_at":"2026-07-04T16:15:23.384854+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.nucl-th/9905056","created_at":"2026-07-04T16:15:23.384854+00:00"},{"alias_kind":"pith_short_12","alias_value":"TMBZE6LWUYMF","created_at":"2026-07-04T16:15:23.384854+00:00"},{"alias_kind":"pith_short_16","alias_value":"TMBZE6LWUYMFY5RY","created_at":"2026-07-04T16:15:23.384854+00:00"},{"alias_kind":"pith_short_8","alias_value":"TMBZE6LW","created_at":"2026-07-04T16:15:23.384854+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":3,"sample":[{"citing_arxiv_id":"2607.06138","citing_title":"Vector-Meson Spin Alignment from Anisotropic Quark or Hadron Coalescence","ref_index":46,"is_internal_anchor":true},{"citing_arxiv_id":"2602.10775","citing_title":"Unified Description of Pseudoscalar Meson Structure from Light to Heavy Quarks","ref_index":17,"is_internal_anchor":true},{"citing_arxiv_id":"2602.17456","citing_title":"Chiral symmetry restoration effects onto the meson spectrum from a Dyson-Schwinger and Bethe-Salpeter approach","ref_index":17,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/TMBZE6LWUYMFY5RYYVLXVF36XF","json":"https://pith.science/pith/TMBZE6LWUYMFY5RYYVLXVF36XF.json","graph_json":"https://pith.science/api/pith-number/TMBZE6LWUYMFY5RYYVLXVF36XF/graph.json","events_json":"https://pith.science/api/pith-number/TMBZE6LWUYMFY5RYYVLXVF36XF/events.json","paper":"https://pith.science/paper/TMBZE6LW"},"agent_actions":{"view_html":"https://pith.science/pith/TMBZE6LWUYMFY5RYYVLXVF36XF","download_json":"https://pith.science/pith/TMBZE6LWUYMFY5RYYVLXVF36XF.json","view_paper":"https://pith.science/paper/TMBZE6LW","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=nucl-th/9905056&json=true","fetch_graph":"https://pith.science/api/pith-number/TMBZE6LWUYMFY5RYYVLXVF36XF/graph.json","fetch_events":"https://pith.science/api/pith-number/TMBZE6LWUYMFY5RYYVLXVF36XF/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/TMBZE6LWUYMFY5RYYVLXVF36XF/action/timestamp_anchor","attest_storage":"https://pith.science/pith/TMBZE6LWUYMFY5RYYVLXVF36XF/action/storage_attestation","attest_author":"https://pith.science/pith/TMBZE6LWUYMFY5RYYVLXVF36XF/action/author_attestation","sign_citation":"https://pith.science/pith/TMBZE6LWUYMFY5RYYVLXVF36XF/action/citation_signature","submit_replication":"https://pith.science/pith/TMBZE6LWUYMFY5RYYVLXVF36XF/action/replication_record"}},"created_at":"2026-07-04T16:15:23.384854+00:00","updated_at":"2026-07-04T16:15:23.384854+00:00"}