{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1997:O7MURZKUBUWP6QSQTVR3OKSDZX","short_pith_number":"pith:O7MURZKU","schema_version":"1.0","canonical_sha256":"77d948e5540d2cff42509d63b72a43cdf88f6d677550e2a0cc54ff70c1eedcde","source":{"kind":"arxiv","id":"hep-ph/9709432","version":2},"attestation_state":"computed","paper":{"title":"The Wilson renormalization group for low x physics: Gluon evolution at finite parton density","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Alex Kovner, Heribert Weigert, Jamal Jalilian-Marian","submitted_at":"1997-09-23T16:06:18Z","abstract_excerpt":"We derive the complete Wilson renormalization group equation which governs the evolution of the gluon distribution and other gluonic observables at low $x$ and arbitrary density."},"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":"hep-ph/9709432","kind":"arxiv","version":2},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1997-09-23T16:06:18Z","cross_cats_sorted":[],"title_canon_sha256":"18d79161fa0071f6663a1fb2703fbc6852bcc16860220ae40872bec5ee2886e9","abstract_canon_sha256":"dc3da004a4997a0e162547b92b88a062a54a5b96a57d2bfb220bf392adc23496"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T15:20:50.752885Z","signature_b64":"VKZpuq75Dof9QNfKB7jr83sbVaXIN/g3WVavQvxqWbmFJ0/SvIKvsYYL1/hDryynP6ud/LUx3XOkQYjPXecgAw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"77d948e5540d2cff42509d63b72a43cdf88f6d677550e2a0cc54ff70c1eedcde","last_reissued_at":"2026-07-04T15:20:50.752480Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T15:20:50.752480Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The Wilson renormalization group for low x physics: Gluon evolution at finite parton density","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Alex Kovner, Heribert Weigert, Jamal Jalilian-Marian","submitted_at":"1997-09-23T16:06:18Z","abstract_excerpt":"We derive the complete Wilson renormalization group equation which governs the evolution of the gluon distribution and other gluonic observables at low $x$ and arbitrary density."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9709432","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/hep-ph/9709432/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":"hep-ph/9709432","created_at":"2026-07-04T15:20:50.752533+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9709432v2","created_at":"2026-07-04T15:20:50.752533+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9709432","created_at":"2026-07-04T15:20:50.752533+00:00"},{"alias_kind":"pith_short_12","alias_value":"O7MURZKUBUWP","created_at":"2026-07-04T15:20:50.752533+00:00"},{"alias_kind":"pith_short_16","alias_value":"O7MURZKUBUWP6QSQ","created_at":"2026-07-04T15:20:50.752533+00:00"},{"alias_kind":"pith_short_8","alias_value":"O7MURZKU","created_at":"2026-07-04T15:20:50.752533+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":10,"internal_anchor_count":7,"sample":[{"citing_arxiv_id":"2606.25685","citing_title":"Quark Reggeization in QCD from the Wilson line formalism","ref_index":24,"is_internal_anchor":true},{"citing_arxiv_id":"2606.17993","citing_title":"From target to projectile: CSS evolution of quark TMD in different light-cone gauges","ref_index":36,"is_internal_anchor":true},{"citing_arxiv_id":"2606.31754","citing_title":"Emergent Local Phase-Space Scaling in Small-x Gluon Evolution","ref_index":10,"is_internal_anchor":true},{"citing_arxiv_id":"2606.31712","citing_title":"Collinearly Improved Balitsky-Kovchegov Evolution of the Gluon Wigner Distribution","ref_index":12,"is_internal_anchor":true},{"citing_arxiv_id":"2506.17454","citing_title":"Nuclear Cold QCD: Review and Future Strategy","ref_index":247,"is_internal_anchor":true},{"citing_arxiv_id":"2512.10086","citing_title":"Unpolarized GPDs at small $x$ and non-zero skewness","ref_index":85,"is_internal_anchor":true},{"citing_arxiv_id":"2603.23428","citing_title":"Sub-eikonal Structure of High-Energy Deep-Inelastic Scattering","ref_index":32,"is_internal_anchor":true},{"citing_arxiv_id":"2604.24629","citing_title":"On the Two $R$-Factors in the Small-$x$ Shockwave Formalism","ref_index":113,"is_internal_anchor":false},{"citing_arxiv_id":"2605.03038","citing_title":"Squeezed-state radiation in shockwave scattering: QCD-Gravity double copy","ref_index":58,"is_internal_anchor":false},{"citing_arxiv_id":"2604.07509","citing_title":"Forward trijet production in proton-nucleus collisions: gluon initiated channel","ref_index":12,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/O7MURZKUBUWP6QSQTVR3OKSDZX","json":"https://pith.science/pith/O7MURZKUBUWP6QSQTVR3OKSDZX.json","graph_json":"https://pith.science/api/pith-number/O7MURZKUBUWP6QSQTVR3OKSDZX/graph.json","events_json":"https://pith.science/api/pith-number/O7MURZKUBUWP6QSQTVR3OKSDZX/events.json","paper":"https://pith.science/paper/O7MURZKU"},"agent_actions":{"view_html":"https://pith.science/pith/O7MURZKUBUWP6QSQTVR3OKSDZX","download_json":"https://pith.science/pith/O7MURZKUBUWP6QSQTVR3OKSDZX.json","view_paper":"https://pith.science/paper/O7MURZKU","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/9709432&json=true","fetch_graph":"https://pith.science/api/pith-number/O7MURZKUBUWP6QSQTVR3OKSDZX/graph.json","fetch_events":"https://pith.science/api/pith-number/O7MURZKUBUWP6QSQTVR3OKSDZX/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/O7MURZKUBUWP6QSQTVR3OKSDZX/action/timestamp_anchor","attest_storage":"https://pith.science/pith/O7MURZKUBUWP6QSQTVR3OKSDZX/action/storage_attestation","attest_author":"https://pith.science/pith/O7MURZKUBUWP6QSQTVR3OKSDZX/action/author_attestation","sign_citation":"https://pith.science/pith/O7MURZKUBUWP6QSQTVR3OKSDZX/action/citation_signature","submit_replication":"https://pith.science/pith/O7MURZKUBUWP6QSQTVR3OKSDZX/action/replication_record"}},"created_at":"2026-07-04T15:20:50.752533+00:00","updated_at":"2026-07-04T15:20:50.752533+00:00"}