{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2012:HTGCWE4WSZFBVPOUTTWWFMGTG7","short_pith_number":"pith:HTGCWE4W","schema_version":"1.0","canonical_sha256":"3ccc2b1396964a1abdd49ced62b0d337f341a1fb7e30fe617a8116d6565717f2","source":{"kind":"arxiv","id":"1212.1656","version":2},"attestation_state":"computed","paper":{"title":"Testing the Gaussian Approximation to the JIMWLK Equation","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"D. N. Triantafyllopoulos, G. Soyez, M. Alvioli","submitted_at":"2012-12-07T16:59:07Z","abstract_excerpt":"In processes involving small-x partons, like in deep inelastic scattering and in hadronic collisions at high energy, the final state can be expressed in terms of correlators of Wilson lines. We study such high-point correlators evolving according to the JIMWLK equation and we confirm the results of previous numerical and analytic work, by using an independent method, that the solution to the JIMWLK equation can be very well approximated by an appropriate Gaussian wavefunction. We explore both fixed and running coupling evolution, where in the latter the scale is set according to various prescr"},"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":"1212.1656","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2012-12-07T16:59:07Z","cross_cats_sorted":[],"title_canon_sha256":"33ed06a6a67a47d8625bbd247f870ea71d8e0c83edbee8ddd2bbe9a4a4555bdd","abstract_canon_sha256":"2bc638a106a8c3c5fbfc723c46757e9b9a96d7e085cdfba7eeed7a79c580b8ef"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:34:35.105751Z","signature_b64":"AWukhWijuxFLcwKVjX3Ki/9SOBEwooPksHybwoiLIJqN8hWjt6MNiHSZiSfzOE/5YjtCi9UeGyriFs+/QD7eCA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"3ccc2b1396964a1abdd49ced62b0d337f341a1fb7e30fe617a8116d6565717f2","last_reissued_at":"2026-05-18T03:34:35.105019Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:34:35.105019Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Testing the Gaussian Approximation to the JIMWLK Equation","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"D. N. Triantafyllopoulos, G. Soyez, M. Alvioli","submitted_at":"2012-12-07T16:59:07Z","abstract_excerpt":"In processes involving small-x partons, like in deep inelastic scattering and in hadronic collisions at high energy, the final state can be expressed in terms of correlators of Wilson lines. We study such high-point correlators evolving according to the JIMWLK equation and we confirm the results of previous numerical and analytic work, by using an independent method, that the solution to the JIMWLK equation can be very well approximated by an appropriate Gaussian wavefunction. We explore both fixed and running coupling evolution, where in the latter the scale is set according to various prescr"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1212.1656","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":"1212.1656","created_at":"2026-05-18T03:34:35.105127+00:00"},{"alias_kind":"arxiv_version","alias_value":"1212.1656v2","created_at":"2026-05-18T03:34:35.105127+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1212.1656","created_at":"2026-05-18T03:34:35.105127+00:00"},{"alias_kind":"pith_short_12","alias_value":"HTGCWE4WSZFB","created_at":"2026-05-18T12:27:09.501522+00:00"},{"alias_kind":"pith_short_16","alias_value":"HTGCWE4WSZFBVPOU","created_at":"2026-05-18T12:27:09.501522+00:00"},{"alias_kind":"pith_short_8","alias_value":"HTGCWE4W","created_at":"2026-05-18T12:27:09.501522+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2604.26123","citing_title":"When JIMWLK evolution really matters: the example of incoherent diffraction","ref_index":42,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/HTGCWE4WSZFBVPOUTTWWFMGTG7","json":"https://pith.science/pith/HTGCWE4WSZFBVPOUTTWWFMGTG7.json","graph_json":"https://pith.science/api/pith-number/HTGCWE4WSZFBVPOUTTWWFMGTG7/graph.json","events_json":"https://pith.science/api/pith-number/HTGCWE4WSZFBVPOUTTWWFMGTG7/events.json","paper":"https://pith.science/paper/HTGCWE4W"},"agent_actions":{"view_html":"https://pith.science/pith/HTGCWE4WSZFBVPOUTTWWFMGTG7","download_json":"https://pith.science/pith/HTGCWE4WSZFBVPOUTTWWFMGTG7.json","view_paper":"https://pith.science/paper/HTGCWE4W","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1212.1656&json=true","fetch_graph":"https://pith.science/api/pith-number/HTGCWE4WSZFBVPOUTTWWFMGTG7/graph.json","fetch_events":"https://pith.science/api/pith-number/HTGCWE4WSZFBVPOUTTWWFMGTG7/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/HTGCWE4WSZFBVPOUTTWWFMGTG7/action/timestamp_anchor","attest_storage":"https://pith.science/pith/HTGCWE4WSZFBVPOUTTWWFMGTG7/action/storage_attestation","attest_author":"https://pith.science/pith/HTGCWE4WSZFBVPOUTTWWFMGTG7/action/author_attestation","sign_citation":"https://pith.science/pith/HTGCWE4WSZFBVPOUTTWWFMGTG7/action/citation_signature","submit_replication":"https://pith.science/pith/HTGCWE4WSZFBVPOUTTWWFMGTG7/action/replication_record"}},"created_at":"2026-05-18T03:34:35.105127+00:00","updated_at":"2026-05-18T03:34:35.105127+00:00"}