{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:3XQSBVIMTMMOYYNZOYCFXCZ2CK","short_pith_number":"pith:3XQSBVIM","schema_version":"1.0","canonical_sha256":"dde120d50c9b18ec61b976045b8b3a128c60ac6bb10deb16a21af71dae6c4cee","source":{"kind":"arxiv","id":"1506.03327","version":2},"attestation_state":"computed","paper":{"title":"Quark production in heavy ion collisions I. Formalism and boost invariant fermionic light-cone mode functions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"F. Gelis, N. Tanji","submitted_at":"2015-06-10T14:36:42Z","abstract_excerpt":"We revisit the problem of quark production in high energy heavy ion collisions, at leading order in $\\alpha_s$ in the color glass condensate framework. In this first paper, we setup the formalism and express the quark spectrum in terms of a set of mode functions of the Dirac equation. We determine analytically their initial value in the Fock-Schwinger gauge on a proper time surface $Q_s\\tau_0\\ll 1$, in a basis which makes manifest the boost invariance properties of this problem. We also describe a statistical algorithm to perform the sampling of the mode functions."},"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":"1506.03327","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2015-06-10T14:36:42Z","cross_cats_sorted":["nucl-th"],"title_canon_sha256":"e46ef422d07b9ccedbad5b5355859f60f85a26881eaf9c480c8d59f70ee3cf2f","abstract_canon_sha256":"5513cc11859e64af29973008326412937a7d768b5ce8bf235279689cc866af3b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:18:44.679704Z","signature_b64":"VIIrEPx1dKu3ZXOkIb2dM/njMlTUrbixFdBPVr1TrF/pxH1tcEmvth/3nApYSTS85PoyvMp7AiMSW7adBMi6BQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"dde120d50c9b18ec61b976045b8b3a128c60ac6bb10deb16a21af71dae6c4cee","last_reissued_at":"2026-05-18T01:18:44.679132Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:18:44.679132Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Quark production in heavy ion collisions I. Formalism and boost invariant fermionic light-cone mode functions","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["nucl-th"],"primary_cat":"hep-ph","authors_text":"F. Gelis, N. Tanji","submitted_at":"2015-06-10T14:36:42Z","abstract_excerpt":"We revisit the problem of quark production in high energy heavy ion collisions, at leading order in $\\alpha_s$ in the color glass condensate framework. In this first paper, we setup the formalism and express the quark spectrum in terms of a set of mode functions of the Dirac equation. We determine analytically their initial value in the Fock-Schwinger gauge on a proper time surface $Q_s\\tau_0\\ll 1$, in a basis which makes manifest the boost invariance properties of this problem. We also describe a statistical algorithm to perform the sampling of the mode functions."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1506.03327","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":"1506.03327","created_at":"2026-05-18T01:18:44.679243+00:00"},{"alias_kind":"arxiv_version","alias_value":"1506.03327v2","created_at":"2026-05-18T01:18:44.679243+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1506.03327","created_at":"2026-05-18T01:18:44.679243+00:00"},{"alias_kind":"pith_short_12","alias_value":"3XQSBVIMTMMO","created_at":"2026-05-18T12:29:02.477457+00:00"},{"alias_kind":"pith_short_16","alias_value":"3XQSBVIMTMMOYYNZ","created_at":"2026-05-18T12:29:02.477457+00:00"},{"alias_kind":"pith_short_8","alias_value":"3XQSBVIM","created_at":"2026-05-18T12:29:02.477457+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2605.10413","citing_title":"Light-front Hamiltonian jet evolution in the Glasma","ref_index":59,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/3XQSBVIMTMMOYYNZOYCFXCZ2CK","json":"https://pith.science/pith/3XQSBVIMTMMOYYNZOYCFXCZ2CK.json","graph_json":"https://pith.science/api/pith-number/3XQSBVIMTMMOYYNZOYCFXCZ2CK/graph.json","events_json":"https://pith.science/api/pith-number/3XQSBVIMTMMOYYNZOYCFXCZ2CK/events.json","paper":"https://pith.science/paper/3XQSBVIM"},"agent_actions":{"view_html":"https://pith.science/pith/3XQSBVIMTMMOYYNZOYCFXCZ2CK","download_json":"https://pith.science/pith/3XQSBVIMTMMOYYNZOYCFXCZ2CK.json","view_paper":"https://pith.science/paper/3XQSBVIM","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1506.03327&json=true","fetch_graph":"https://pith.science/api/pith-number/3XQSBVIMTMMOYYNZOYCFXCZ2CK/graph.json","fetch_events":"https://pith.science/api/pith-number/3XQSBVIMTMMOYYNZOYCFXCZ2CK/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/3XQSBVIMTMMOYYNZOYCFXCZ2CK/action/timestamp_anchor","attest_storage":"https://pith.science/pith/3XQSBVIMTMMOYYNZOYCFXCZ2CK/action/storage_attestation","attest_author":"https://pith.science/pith/3XQSBVIMTMMOYYNZOYCFXCZ2CK/action/author_attestation","sign_citation":"https://pith.science/pith/3XQSBVIMTMMOYYNZOYCFXCZ2CK/action/citation_signature","submit_replication":"https://pith.science/pith/3XQSBVIMTMMOYYNZOYCFXCZ2CK/action/replication_record"}},"created_at":"2026-05-18T01:18:44.679243+00:00","updated_at":"2026-05-18T01:18:44.679243+00:00"}