{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2025:2UYN4A4Z4Q6KSDBXYWWVTR43LD","short_pith_number":"pith:2UYN4A4Z","schema_version":"1.0","canonical_sha256":"d530de0399e43ca90c37c5ad59c79b58d3ea3ea3aeb1d76ab3476407a5f30ad0","source":{"kind":"arxiv","id":"2502.16689","version":3},"attestation_state":"computed","paper":{"title":"Mechanical properties of proton using flavor-decomposed gravitational form factors","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ex","hep-lat","nucl-th"],"primary_cat":"hep-ph","authors_text":"F. Almaksusi, K. Azizi, Zeinab Dehghan","submitted_at":"2025-02-23T19:05:04Z","abstract_excerpt":"We investigate the mechanical properties of the proton by extracting its flavor-decomposed gravitational form factors (GFFs) using Light-Cone QCD sum rules (LCSR). These form factors encode critical information about the internal dynamics and spatial distribution of energy, momentum, and internal forces within the proton. The flavor decomposition of the quark sector indicates the role of each flavor in the proton's pressure and shear force distributions. Our results show that the up quark contributes more significantly compared to the down quark in the three conserved proton GFFs, as well as i"},"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":"2502.16689","kind":"arxiv","version":3},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2025-02-23T19:05:04Z","cross_cats_sorted":["hep-ex","hep-lat","nucl-th"],"title_canon_sha256":"ef7dcf7b912547066dde8d22b03d8c3daa7ccda7985d6d9f1eb6d2dc57245894","abstract_canon_sha256":"47a9f69664c33d07e9f716e4dfe506e27964dcb83c1e32cb4927690978319822"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T11:51:22.460958Z","signature_b64":"TIr3uB8rXGkV5g6CqDsiZryPjyGbRb7aFS3A0ZgLESsMRG97TTM96KNHF/5rKBYnJofgUhG51UTrIMNwoKPkAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d530de0399e43ca90c37c5ad59c79b58d3ea3ea3aeb1d76ab3476407a5f30ad0","last_reissued_at":"2026-07-05T11:51:22.460419Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T11:51:22.460419Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Mechanical properties of proton using flavor-decomposed gravitational form factors","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ex","hep-lat","nucl-th"],"primary_cat":"hep-ph","authors_text":"F. Almaksusi, K. Azizi, Zeinab Dehghan","submitted_at":"2025-02-23T19:05:04Z","abstract_excerpt":"We investigate the mechanical properties of the proton by extracting its flavor-decomposed gravitational form factors (GFFs) using Light-Cone QCD sum rules (LCSR). These form factors encode critical information about the internal dynamics and spatial distribution of energy, momentum, and internal forces within the proton. The flavor decomposition of the quark sector indicates the role of each flavor in the proton's pressure and shear force distributions. Our results show that the up quark contributes more significantly compared to the down quark in the three conserved proton GFFs, as well as i"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2502.16689","kind":"arxiv","version":3},"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/2502.16689/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":"2502.16689","created_at":"2026-07-05T11:51:22.460490+00:00"},{"alias_kind":"arxiv_version","alias_value":"2502.16689v3","created_at":"2026-07-05T11:51:22.460490+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2502.16689","created_at":"2026-07-05T11:51:22.460490+00:00"},{"alias_kind":"pith_short_12","alias_value":"2UYN4A4Z4Q6K","created_at":"2026-07-05T11:51:22.460490+00:00"},{"alias_kind":"pith_short_16","alias_value":"2UYN4A4Z4Q6KSDBX","created_at":"2026-07-05T11:51:22.460490+00:00"},{"alias_kind":"pith_short_8","alias_value":"2UYN4A4Z","created_at":"2026-07-05T11:51:22.460490+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":5,"internal_anchor_count":0,"sample":[{"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":22,"is_internal_anchor":false},{"citing_arxiv_id":"2601.17948","citing_title":"Tensor form factors of decuplet hyperons in QCD","ref_index":13,"is_internal_anchor":false},{"citing_arxiv_id":"2605.13701","citing_title":"Constraints on the mass of the dark antibaryon using $B_d\\rightarrow \\Lambda \\psi_{DS}$ channel in light cone QCD","ref_index":75,"is_internal_anchor":false},{"citing_arxiv_id":"2604.03832","citing_title":"Gravitational transverse momentum distribution of proton","ref_index":65,"is_internal_anchor":false},{"citing_arxiv_id":"2604.26537","citing_title":"Particle seismology: mechanical and gravitational properties from parton-hadron duality","ref_index":80,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/2UYN4A4Z4Q6KSDBXYWWVTR43LD","json":"https://pith.science/pith/2UYN4A4Z4Q6KSDBXYWWVTR43LD.json","graph_json":"https://pith.science/api/pith-number/2UYN4A4Z4Q6KSDBXYWWVTR43LD/graph.json","events_json":"https://pith.science/api/pith-number/2UYN4A4Z4Q6KSDBXYWWVTR43LD/events.json","paper":"https://pith.science/paper/2UYN4A4Z"},"agent_actions":{"view_html":"https://pith.science/pith/2UYN4A4Z4Q6KSDBXYWWVTR43LD","download_json":"https://pith.science/pith/2UYN4A4Z4Q6KSDBXYWWVTR43LD.json","view_paper":"https://pith.science/paper/2UYN4A4Z","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2502.16689&json=true","fetch_graph":"https://pith.science/api/pith-number/2UYN4A4Z4Q6KSDBXYWWVTR43LD/graph.json","fetch_events":"https://pith.science/api/pith-number/2UYN4A4Z4Q6KSDBXYWWVTR43LD/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/2UYN4A4Z4Q6KSDBXYWWVTR43LD/action/timestamp_anchor","attest_storage":"https://pith.science/pith/2UYN4A4Z4Q6KSDBXYWWVTR43LD/action/storage_attestation","attest_author":"https://pith.science/pith/2UYN4A4Z4Q6KSDBXYWWVTR43LD/action/author_attestation","sign_citation":"https://pith.science/pith/2UYN4A4Z4Q6KSDBXYWWVTR43LD/action/citation_signature","submit_replication":"https://pith.science/pith/2UYN4A4Z4Q6KSDBXYWWVTR43LD/action/replication_record"}},"created_at":"2026-07-05T11:51:22.460490+00:00","updated_at":"2026-07-05T11:51:22.460490+00:00"}