{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2006:ORKAJGHUZV5FF4CDSNE5A3JOX5","short_pith_number":"pith:ORKAJGHU","schema_version":"1.0","canonical_sha256":"74540498f4cd7a52f0439349d06d2ebf5f87a0d080daaeb1c1ae7fcdcc2b2c63","source":{"kind":"arxiv","id":"nucl-th/0604012","version":2},"attestation_state":"computed","paper":{"title":"Evidence for the Strong Dominance of Proton-Neutron Correlations in Nuclei","license":"","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"E. Piasetzky, J. W. Watson, L. Frankfurt, M. Sargsian, M. Strikman","submitted_at":"2006-04-04T21:18:16Z","abstract_excerpt":"We analyze recent data from high-momentum-transfer $(p,pp)$ and $(p,ppn)$ reactions on Carbon. For this analysis, the two-nucleon short-range correlation (NN-SRC) model for backward nucleon emission is extended to include the motion of the NN-pair in the mean field. The model is found to describe major characteristics of the data. Our analysis demonstrates that the removal of a proton from the nucleus with initial momentum 275-550 MeV/c is $92^{+8}_{-18}%$ of the time accompanied by the emission of a correlated neutron that carries momentum roughly equal and opposite to the initial proton mome"},"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/0604012","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"nucl-th","submitted_at":"2006-04-04T21:18:16Z","cross_cats_sorted":[],"title_canon_sha256":"88ff4d7293ec9dfb1d13c76e3c0358ce1171309e1fd39ce10a36a2e8c054bbee","abstract_canon_sha256":"be6e3ddab395210f0723963b78d1bf03e46dad5070d94892658a32b0edd80227"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T17:02:20.890505Z","signature_b64":"7r16DRkhAerzPzDNX1cMKj+gRx0B15qGZcUHJqyS4iSxYum/JOUD1lnWv5jxccI2JWJoXpUiK/p8du7xI5AGCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"74540498f4cd7a52f0439349d06d2ebf5f87a0d080daaeb1c1ae7fcdcc2b2c63","last_reissued_at":"2026-07-04T17:02:20.890165Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T17:02:20.890165Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Evidence for the Strong Dominance of Proton-Neutron Correlations in Nuclei","license":"","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"E. Piasetzky, J. W. Watson, L. Frankfurt, M. Sargsian, M. Strikman","submitted_at":"2006-04-04T21:18:16Z","abstract_excerpt":"We analyze recent data from high-momentum-transfer $(p,pp)$ and $(p,ppn)$ reactions on Carbon. For this analysis, the two-nucleon short-range correlation (NN-SRC) model for backward nucleon emission is extended to include the motion of the NN-pair in the mean field. The model is found to describe major characteristics of the data. Our analysis demonstrates that the removal of a proton from the nucleus with initial momentum 275-550 MeV/c is $92^{+8}_{-18}%$ of the time accompanied by the emission of a correlated neutron that carries momentum roughly equal and opposite to the initial proton mome"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"nucl-th/0604012","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/0604012/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/0604012","created_at":"2026-07-04T17:02:20.890220+00:00"},{"alias_kind":"arxiv_version","alias_value":"nucl-th/0604012v2","created_at":"2026-07-04T17:02:20.890220+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.nucl-th/0604012","created_at":"2026-07-04T17:02:20.890220+00:00"},{"alias_kind":"pith_short_12","alias_value":"ORKAJGHUZV5F","created_at":"2026-07-04T17:02:20.890220+00:00"},{"alias_kind":"pith_short_16","alias_value":"ORKAJGHUZV5FF4CD","created_at":"2026-07-04T17:02:20.890220+00:00"},{"alias_kind":"pith_short_8","alias_value":"ORKAJGHU","created_at":"2026-07-04T17:02:20.890220+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":2,"internal_anchor_count":2,"sample":[{"citing_arxiv_id":"2606.17133","citing_title":"Short-Range Correlations Between Partons in a Proton","ref_index":30,"is_internal_anchor":true},{"citing_arxiv_id":"2508.04550","citing_title":"Experimental Study of Bremsstrahlung Gamma Ray Emission and Short-Range Correlations in $^{124}$Sn+$^{124}$Sn Collisions at 25 MeV/u","ref_index":17,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/ORKAJGHUZV5FF4CDSNE5A3JOX5","json":"https://pith.science/pith/ORKAJGHUZV5FF4CDSNE5A3JOX5.json","graph_json":"https://pith.science/api/pith-number/ORKAJGHUZV5FF4CDSNE5A3JOX5/graph.json","events_json":"https://pith.science/api/pith-number/ORKAJGHUZV5FF4CDSNE5A3JOX5/events.json","paper":"https://pith.science/paper/ORKAJGHU"},"agent_actions":{"view_html":"https://pith.science/pith/ORKAJGHUZV5FF4CDSNE5A3JOX5","download_json":"https://pith.science/pith/ORKAJGHUZV5FF4CDSNE5A3JOX5.json","view_paper":"https://pith.science/paper/ORKAJGHU","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=nucl-th/0604012&json=true","fetch_graph":"https://pith.science/api/pith-number/ORKAJGHUZV5FF4CDSNE5A3JOX5/graph.json","fetch_events":"https://pith.science/api/pith-number/ORKAJGHUZV5FF4CDSNE5A3JOX5/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ORKAJGHUZV5FF4CDSNE5A3JOX5/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ORKAJGHUZV5FF4CDSNE5A3JOX5/action/storage_attestation","attest_author":"https://pith.science/pith/ORKAJGHUZV5FF4CDSNE5A3JOX5/action/author_attestation","sign_citation":"https://pith.science/pith/ORKAJGHUZV5FF4CDSNE5A3JOX5/action/citation_signature","submit_replication":"https://pith.science/pith/ORKAJGHUZV5FF4CDSNE5A3JOX5/action/replication_record"}},"created_at":"2026-07-04T17:02:20.890220+00:00","updated_at":"2026-07-04T17:02:20.890220+00:00"}