{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:CC6HBH4T4U5QVX2UOHEHPZ2ZFH","short_pith_number":"pith:CC6HBH4T","schema_version":"1.0","canonical_sha256":"10bc709f93e53b0adf5471c877e75929fdd465cabc053bce5e3c00e96c696cd6","source":{"kind":"arxiv","id":"2405.07815","version":2},"attestation_state":"computed","paper":{"title":"Gravitational form factors of the pion and meson dominance","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-lat"],"primary_cat":"hep-ph","authors_text":"Enrique Ruiz Arriola, Wojciech Broniowski","submitted_at":"2024-05-13T14:58:46Z","abstract_excerpt":"We show that the recent MIT lattice QCD data for the pion's gravitational form factors are, in the covered momentum transfer range, fully consistent with the meson dominance principle. In particular, the $2^{++}$ component can be accurately saturated with the $f_2(1270)$ meson, whereas the $0^{++}$ component with the $\\sigma$ meson. To incorporate the large width of the $\\sigma$, we use the dispersion relation with the spectral density obtained from analyses of the physical pion scattering data. Effects of the pion mass are estimated within Chiral Perturbation Theory and are found to be small "},"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":"2405.07815","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2024-05-13T14:58:46Z","cross_cats_sorted":["hep-lat"],"title_canon_sha256":"d7b1c48d4f5960918a9b871151b9808658da63f94fb5ed20638ca45fbc1a4f11","abstract_canon_sha256":"e0e1f6f17adb2d7507629b7561b400a040d9ee6c4fbbb11e3737174ecdd3127d"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T09:19:57.224669Z","signature_b64":"qh1e4L6ETiNwxcWCpBayJD0z5amg7L+7MXEWXSbxe0V1klxaz65FsTJd3bqnSW8542MArUiRgs1wxNjCroLMAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"10bc709f93e53b0adf5471c877e75929fdd465cabc053bce5e3c00e96c696cd6","last_reissued_at":"2026-07-05T09:19:57.224236Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T09:19:57.224236Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Gravitational form factors of the pion and meson dominance","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-lat"],"primary_cat":"hep-ph","authors_text":"Enrique Ruiz Arriola, Wojciech Broniowski","submitted_at":"2024-05-13T14:58:46Z","abstract_excerpt":"We show that the recent MIT lattice QCD data for the pion's gravitational form factors are, in the covered momentum transfer range, fully consistent with the meson dominance principle. In particular, the $2^{++}$ component can be accurately saturated with the $f_2(1270)$ meson, whereas the $0^{++}$ component with the $\\sigma$ meson. To incorporate the large width of the $\\sigma$, we use the dispersion relation with the spectral density obtained from analyses of the physical pion scattering data. Effects of the pion mass are estimated within Chiral Perturbation Theory and are found to be small "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2405.07815","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/2405.07815/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":"2405.07815","created_at":"2026-07-05T09:19:57.224289+00:00"},{"alias_kind":"arxiv_version","alias_value":"2405.07815v2","created_at":"2026-07-05T09:19:57.224289+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2405.07815","created_at":"2026-07-05T09:19:57.224289+00:00"},{"alias_kind":"pith_short_12","alias_value":"CC6HBH4T4U5Q","created_at":"2026-07-05T09:19:57.224289+00:00"},{"alias_kind":"pith_short_16","alias_value":"CC6HBH4T4U5QVX2U","created_at":"2026-07-05T09:19:57.224289+00:00"},{"alias_kind":"pith_short_8","alias_value":"CC6HBH4T","created_at":"2026-07-05T09:19:57.224289+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":5,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.07073","citing_title":"Mechanical distribution of the pseudoscalar charmonium and bottomonium on the light-front","ref_index":52,"is_internal_anchor":false},{"citing_arxiv_id":"2512.12315","citing_title":"Gluon Gravitational $ D$-Form Factor: The $\\sigma$-Meson as a Dilaton Confronted with Lattice Data II","ref_index":24,"is_internal_anchor":false},{"citing_arxiv_id":"2605.18350","citing_title":"Gravitational form factors of light mesons from Basis Light-Front Quantization","ref_index":31,"is_internal_anchor":false},{"citing_arxiv_id":"2604.26537","citing_title":"Particle seismology: mechanical and gravitational properties from parton-hadron duality","ref_index":91,"is_internal_anchor":false},{"citing_arxiv_id":"2604.09185","citing_title":"Hadronic form factors in QCD and the incompleteness problem in the time-like region","ref_index":11,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/CC6HBH4T4U5QVX2UOHEHPZ2ZFH","json":"https://pith.science/pith/CC6HBH4T4U5QVX2UOHEHPZ2ZFH.json","graph_json":"https://pith.science/api/pith-number/CC6HBH4T4U5QVX2UOHEHPZ2ZFH/graph.json","events_json":"https://pith.science/api/pith-number/CC6HBH4T4U5QVX2UOHEHPZ2ZFH/events.json","paper":"https://pith.science/paper/CC6HBH4T"},"agent_actions":{"view_html":"https://pith.science/pith/CC6HBH4T4U5QVX2UOHEHPZ2ZFH","download_json":"https://pith.science/pith/CC6HBH4T4U5QVX2UOHEHPZ2ZFH.json","view_paper":"https://pith.science/paper/CC6HBH4T","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2405.07815&json=true","fetch_graph":"https://pith.science/api/pith-number/CC6HBH4T4U5QVX2UOHEHPZ2ZFH/graph.json","fetch_events":"https://pith.science/api/pith-number/CC6HBH4T4U5QVX2UOHEHPZ2ZFH/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/CC6HBH4T4U5QVX2UOHEHPZ2ZFH/action/timestamp_anchor","attest_storage":"https://pith.science/pith/CC6HBH4T4U5QVX2UOHEHPZ2ZFH/action/storage_attestation","attest_author":"https://pith.science/pith/CC6HBH4T4U5QVX2UOHEHPZ2ZFH/action/author_attestation","sign_citation":"https://pith.science/pith/CC6HBH4T4U5QVX2UOHEHPZ2ZFH/action/citation_signature","submit_replication":"https://pith.science/pith/CC6HBH4T4U5QVX2UOHEHPZ2ZFH/action/replication_record"}},"created_at":"2026-07-05T09:19:57.224289+00:00","updated_at":"2026-07-05T09:19:57.224289+00:00"}