{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2013:2WNIUWNW3M2H57SR77SGVSSS5M","short_pith_number":"pith:2WNIUWNW","schema_version":"1.0","canonical_sha256":"d59a8a59b6db347efe51ffe46aca52eb342433ba1b02725b0f87baf587944655","source":{"kind":"arxiv","id":"1310.6935","version":4},"attestation_state":"computed","paper":{"title":"High Energy Collisions of Dense Hadrons in Quantum Chromodynamics : LHC Phenomenology and Universality of Parton Distributions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"hep-ph","authors_text":"Julien Laidet","submitted_at":"2013-10-25T14:33:52Z","abstract_excerpt":"As the value of the longitudinal momentum carried by partons in a ultra-relativistic hadron becomes small, one observes a growth of their density. When the parton density becomes close to a value of order $1/\\alpha_s$, it does not grow any longer, it saturates. These high density effects seem to be well described by the Color Glass Condensate effective field theory. On the experimental side, the LHC provides the best tool ever for reaching the saturated phase of hadronic matter. For this reason saturation physics is a very active branch of QCD during these past and coming years since saturatio"},"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":"1310.6935","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2013-10-25T14:33:52Z","cross_cats_sorted":["hep-th"],"title_canon_sha256":"cb81cee8e539334582464801c884dacb67e64eaf14819ae339d9b1e01b1dcd2d","abstract_canon_sha256":"764732ee35820a7bbc4b58ce9f05170ccb4204131fc6cabdbafb516d9fd607c9"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:21:45.358819Z","signature_b64":"peM2SVPLdHkbMfv5Fg71a2IzT+TqVOtCUepqH1J1XWf6agv9ja6/IrxFWqoUGDZkQcKeLd1HBNQmlJ/yJr52Aw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d59a8a59b6db347efe51ffe46aca52eb342433ba1b02725b0f87baf587944655","last_reissued_at":"2026-05-18T01:21:45.358112Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:21:45.358112Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"High Energy Collisions of Dense Hadrons in Quantum Chromodynamics : LHC Phenomenology and Universality of Parton Distributions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-th"],"primary_cat":"hep-ph","authors_text":"Julien Laidet","submitted_at":"2013-10-25T14:33:52Z","abstract_excerpt":"As the value of the longitudinal momentum carried by partons in a ultra-relativistic hadron becomes small, one observes a growth of their density. When the parton density becomes close to a value of order $1/\\alpha_s$, it does not grow any longer, it saturates. These high density effects seem to be well described by the Color Glass Condensate effective field theory. On the experimental side, the LHC provides the best tool ever for reaching the saturated phase of hadronic matter. For this reason saturation physics is a very active branch of QCD during these past and coming years since saturatio"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1310.6935","kind":"arxiv","version":4},"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":"1310.6935","created_at":"2026-05-18T01:21:45.358216+00:00"},{"alias_kind":"arxiv_version","alias_value":"1310.6935v4","created_at":"2026-05-18T01:21:45.358216+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1310.6935","created_at":"2026-05-18T01:21:45.358216+00:00"},{"alias_kind":"pith_short_12","alias_value":"2WNIUWNW3M2H","created_at":"2026-05-18T12:27:32.513160+00:00"},{"alias_kind":"pith_short_16","alias_value":"2WNIUWNW3M2H57SR","created_at":"2026-05-18T12:27:32.513160+00:00"},{"alias_kind":"pith_short_8","alias_value":"2WNIUWNW","created_at":"2026-05-18T12:27:32.513160+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":0,"internal_anchor_count":0,"sample":[]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/2WNIUWNW3M2H57SR77SGVSSS5M","json":"https://pith.science/pith/2WNIUWNW3M2H57SR77SGVSSS5M.json","graph_json":"https://pith.science/api/pith-number/2WNIUWNW3M2H57SR77SGVSSS5M/graph.json","events_json":"https://pith.science/api/pith-number/2WNIUWNW3M2H57SR77SGVSSS5M/events.json","paper":"https://pith.science/paper/2WNIUWNW"},"agent_actions":{"view_html":"https://pith.science/pith/2WNIUWNW3M2H57SR77SGVSSS5M","download_json":"https://pith.science/pith/2WNIUWNW3M2H57SR77SGVSSS5M.json","view_paper":"https://pith.science/paper/2WNIUWNW","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1310.6935&json=true","fetch_graph":"https://pith.science/api/pith-number/2WNIUWNW3M2H57SR77SGVSSS5M/graph.json","fetch_events":"https://pith.science/api/pith-number/2WNIUWNW3M2H57SR77SGVSSS5M/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/2WNIUWNW3M2H57SR77SGVSSS5M/action/timestamp_anchor","attest_storage":"https://pith.science/pith/2WNIUWNW3M2H57SR77SGVSSS5M/action/storage_attestation","attest_author":"https://pith.science/pith/2WNIUWNW3M2H57SR77SGVSSS5M/action/author_attestation","sign_citation":"https://pith.science/pith/2WNIUWNW3M2H57SR77SGVSSS5M/action/citation_signature","submit_replication":"https://pith.science/pith/2WNIUWNW3M2H57SR77SGVSSS5M/action/replication_record"}},"created_at":"2026-05-18T01:21:45.358216+00:00","updated_at":"2026-05-18T01:21:45.358216+00:00"}