{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2012:XFLKGC2O47NXUWRKN5XTIQRG5T","short_pith_number":"pith:XFLKGC2O","schema_version":"1.0","canonical_sha256":"b956a30b4ee7db7a5a2a6f6f344226ece47691b4f109571219254151af32c05a","source":{"kind":"arxiv","id":"1209.2853","version":2},"attestation_state":"computed","paper":{"title":"Forward dihadron correlations in deuteron-gold collisions with a Gaussian approximation of JIMWLK","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"H. M\\\"antysaari, T. Lappi","submitted_at":"2012-09-13T11:16:12Z","abstract_excerpt":"We compute dihadron correlations in forward deuteron-gold or proton-gold collisions. The running coupling BK equation is used to calculate the energy dependence of the dipole cross sections and extended to higher point Wilson line correlators using a factorized Gaussian approximation. Unlike some earlier works we include both the \"inelastic\" and \"elastic\" contributions to the dihadron cross section. We show that the double parton scattering contribution is included in our calculation and obtain both an away side peak that roughly agrees with experimental observations and an estimate for the az"},"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":"1209.2853","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2012-09-13T11:16:12Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"9e38086df9fb09439c12aa6a878d80299c8e77060a405d328a99f6dd53cc60a3","abstract_canon_sha256":"335dcb49e47377962acc5ed04e9eb10679af8dd641d4e9505688021dfdf1b96b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:28:29.461514Z","signature_b64":"M/CDehXqQe1t+97BmUpDEEQ8OsBk/bGQdv41KmxSxrev//mG7sDvXSySqb5qSQ93ICPnCJKjAydDL3+Y7ocUBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b956a30b4ee7db7a5a2a6f6f344226ece47691b4f109571219254151af32c05a","last_reissued_at":"2026-05-18T03:28:29.460914Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:28:29.460914Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Forward dihadron correlations in deuteron-gold collisions with a Gaussian approximation of JIMWLK","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"H. M\\\"antysaari, T. Lappi","submitted_at":"2012-09-13T11:16:12Z","abstract_excerpt":"We compute dihadron correlations in forward deuteron-gold or proton-gold collisions. The running coupling BK equation is used to calculate the energy dependence of the dipole cross sections and extended to higher point Wilson line correlators using a factorized Gaussian approximation. Unlike some earlier works we include both the \"inelastic\" and \"elastic\" contributions to the dihadron cross section. We show that the double parton scattering contribution is included in our calculation and obtain both an away side peak that roughly agrees with experimental observations and an estimate for the az"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1209.2853","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":""},"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":"1209.2853","created_at":"2026-05-18T03:28:29.461016+00:00"},{"alias_kind":"arxiv_version","alias_value":"1209.2853v2","created_at":"2026-05-18T03:28:29.461016+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1209.2853","created_at":"2026-05-18T03:28:29.461016+00:00"},{"alias_kind":"pith_short_12","alias_value":"XFLKGC2O47NX","created_at":"2026-05-18T12:27:27.928770+00:00"},{"alias_kind":"pith_short_16","alias_value":"XFLKGC2O47NXUWRK","created_at":"2026-05-18T12:27:27.928770+00:00"},{"alias_kind":"pith_short_8","alias_value":"XFLKGC2O","created_at":"2026-05-18T12:27:27.928770+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":4,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2605.15494","citing_title":"Forward hadron production in pp collisions at LHC energies from an event generator based on the color glass condensate framework","ref_index":51,"is_internal_anchor":true},{"citing_arxiv_id":"2604.26123","citing_title":"When JIMWLK evolution really matters: the example of incoherent diffraction","ref_index":22,"is_internal_anchor":false},{"citing_arxiv_id":"2605.01527","citing_title":"Probing Saturation Effect in Heavy Meson Pair Correlation in Forward $pA$ Collisions","ref_index":28,"is_internal_anchor":false},{"citing_arxiv_id":"2604.07509","citing_title":"Forward trijet production in proton-nucleus collisions: gluon initiated channel","ref_index":45,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/XFLKGC2O47NXUWRKN5XTIQRG5T","json":"https://pith.science/pith/XFLKGC2O47NXUWRKN5XTIQRG5T.json","graph_json":"https://pith.science/api/pith-number/XFLKGC2O47NXUWRKN5XTIQRG5T/graph.json","events_json":"https://pith.science/api/pith-number/XFLKGC2O47NXUWRKN5XTIQRG5T/events.json","paper":"https://pith.science/paper/XFLKGC2O"},"agent_actions":{"view_html":"https://pith.science/pith/XFLKGC2O47NXUWRKN5XTIQRG5T","download_json":"https://pith.science/pith/XFLKGC2O47NXUWRKN5XTIQRG5T.json","view_paper":"https://pith.science/paper/XFLKGC2O","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1209.2853&json=true","fetch_graph":"https://pith.science/api/pith-number/XFLKGC2O47NXUWRKN5XTIQRG5T/graph.json","fetch_events":"https://pith.science/api/pith-number/XFLKGC2O47NXUWRKN5XTIQRG5T/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/XFLKGC2O47NXUWRKN5XTIQRG5T/action/timestamp_anchor","attest_storage":"https://pith.science/pith/XFLKGC2O47NXUWRKN5XTIQRG5T/action/storage_attestation","attest_author":"https://pith.science/pith/XFLKGC2O47NXUWRKN5XTIQRG5T/action/author_attestation","sign_citation":"https://pith.science/pith/XFLKGC2O47NXUWRKN5XTIQRG5T/action/citation_signature","submit_replication":"https://pith.science/pith/XFLKGC2O47NXUWRKN5XTIQRG5T/action/replication_record"}},"created_at":"2026-05-18T03:28:29.461016+00:00","updated_at":"2026-05-18T03:28:29.461016+00:00"}