{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2011:VS3VWMMCFRNWCDGTF5FKTCP3O6","short_pith_number":"pith:VS3VWMMC","schema_version":"1.0","canonical_sha256":"acb75b31822c5b610cd32f4aa989fb778647b5226e37e69d55b3204cb22feebf","source":{"kind":"arxiv","id":"1109.0347","version":1},"attestation_state":"computed","paper":{"title":"On Angular Correlations and High Energy Evolution","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"Alex Kovner, Michael Lublinsky","submitted_at":"2011-09-02T03:07:54Z","abstract_excerpt":"We address the question to what extent JIMWLK evolution is capable of taking into account angular correlations in a high energy hadronic wave function. Our conclusion is that angular (and indeed other) correlations in the wave function cannot be reliably calculated without taking into account Pomeron loops in the evolution. As an example we study numerically the energy evolution of angular correlations between dipole scattering amplitudes in the framework of the large $N_c$ approximation to JIMWLK evolution (the \"`projectile dipole model\"'). Target correlations are introduced via averaging ove"},"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":"1109.0347","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2011-09-02T03:07:54Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"9a50caefd04f6e40576dc0db28b895dd4836ce40f4c06d69fce2cab9b7086070","abstract_canon_sha256":"b6cab924a9a9a0fddc996749d1643497b0d9ec85b063352bd8b91bf5ee66e9e0"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:23:21.468465Z","signature_b64":"fB0KNrpQoZVFDVX6ePQjUKwWcMV5aWFtJYcKi3TYVtHv3XX0YK99b54T4x9LoXugvb6BM6zWUcX/E9PLOwEPAA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"acb75b31822c5b610cd32f4aa989fb778647b5226e37e69d55b3204cb22feebf","last_reissued_at":"2026-05-18T03:23:21.467864Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:23:21.467864Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"On Angular Correlations and High Energy Evolution","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"Alex Kovner, Michael Lublinsky","submitted_at":"2011-09-02T03:07:54Z","abstract_excerpt":"We address the question to what extent JIMWLK evolution is capable of taking into account angular correlations in a high energy hadronic wave function. Our conclusion is that angular (and indeed other) correlations in the wave function cannot be reliably calculated without taking into account Pomeron loops in the evolution. As an example we study numerically the energy evolution of angular correlations between dipole scattering amplitudes in the framework of the large $N_c$ approximation to JIMWLK evolution (the \"`projectile dipole model\"'). Target correlations are introduced via averaging ove"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1109.0347","kind":"arxiv","version":1},"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":"1109.0347","created_at":"2026-05-18T03:23:21.467967+00:00"},{"alias_kind":"arxiv_version","alias_value":"1109.0347v1","created_at":"2026-05-18T03:23:21.467967+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1109.0347","created_at":"2026-05-18T03:23:21.467967+00:00"},{"alias_kind":"pith_short_12","alias_value":"VS3VWMMCFRNW","created_at":"2026-05-18T12:26:44.992195+00:00"},{"alias_kind":"pith_short_16","alias_value":"VS3VWMMCFRNWCDGT","created_at":"2026-05-18T12:26:44.992195+00:00"},{"alias_kind":"pith_short_8","alias_value":"VS3VWMMC","created_at":"2026-05-18T12:26:44.992195+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"1908.06212","citing_title":"Hybrid Color Glass Condensate and hydrodynamic description of the Relativistic Heavy Ion Collider small system scan","ref_index":8,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/VS3VWMMCFRNWCDGTF5FKTCP3O6","json":"https://pith.science/pith/VS3VWMMCFRNWCDGTF5FKTCP3O6.json","graph_json":"https://pith.science/api/pith-number/VS3VWMMCFRNWCDGTF5FKTCP3O6/graph.json","events_json":"https://pith.science/api/pith-number/VS3VWMMCFRNWCDGTF5FKTCP3O6/events.json","paper":"https://pith.science/paper/VS3VWMMC"},"agent_actions":{"view_html":"https://pith.science/pith/VS3VWMMCFRNWCDGTF5FKTCP3O6","download_json":"https://pith.science/pith/VS3VWMMCFRNWCDGTF5FKTCP3O6.json","view_paper":"https://pith.science/paper/VS3VWMMC","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1109.0347&json=true","fetch_graph":"https://pith.science/api/pith-number/VS3VWMMCFRNWCDGTF5FKTCP3O6/graph.json","fetch_events":"https://pith.science/api/pith-number/VS3VWMMCFRNWCDGTF5FKTCP3O6/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/VS3VWMMCFRNWCDGTF5FKTCP3O6/action/timestamp_anchor","attest_storage":"https://pith.science/pith/VS3VWMMCFRNWCDGTF5FKTCP3O6/action/storage_attestation","attest_author":"https://pith.science/pith/VS3VWMMCFRNWCDGTF5FKTCP3O6/action/author_attestation","sign_citation":"https://pith.science/pith/VS3VWMMCFRNWCDGTF5FKTCP3O6/action/citation_signature","submit_replication":"https://pith.science/pith/VS3VWMMCFRNWCDGTF5FKTCP3O6/action/replication_record"}},"created_at":"2026-05-18T03:23:21.467967+00:00","updated_at":"2026-05-18T03:23:21.467967+00:00"}