{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:EI42OU3H6DR6NNAGNSLSROBL3R","short_pith_number":"pith:EI42OU3H","schema_version":"1.0","canonical_sha256":"2239a75367f0e3e6b4066c9728b82bdc762fa9ebcf8ab6889e920bd4fc1d6878","source":{"kind":"arxiv","id":"1604.06346","version":3},"attestation_state":"computed","paper":{"title":"Electromagnetic probes of a pure-glue initial state in nucleus-nucleus collisions at energies available at the CERN Large Hadron Collider","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"nucl-th","authors_text":"B. K\\\"ampfer, H. Stoecker, I. N. Mishustin, Iu. A. Karpenko, L. M. Satarov, M. I. Gorenstein, V. Vovchenko","submitted_at":"2016-04-21T14:58:39Z","abstract_excerpt":"Partonic matter produced in the early stage of ultrarelativistic nucleus-nucleus collisions is assumed to be composed mainly of gluons, and quarks and antiquarks are produced at later times. To study the implications of such a scenario, the dynamical evolution of a chemically nonequilibrated system is described by the ideal (2+1)-dimensional hydrodynamics with a time dependent (anti)quark fugacity. The equation of state interpolates linearly between the lattice data for the pure gluonic matter and the lattice data for the chemically equilibrated quark-gluon plasma. The spectra and elliptic flo"},"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":"1604.06346","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2016-04-21T14:58:39Z","cross_cats_sorted":["hep-ph"],"title_canon_sha256":"e99a65d5e7af68dec8debc258df5a21d91ea297b14c64688cc8ba2c507c25c39","abstract_canon_sha256":"e9b14d7e6b44b0c9db341d863046814d7276268dd1f7886b8454f1ed1b4f42e0"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T01:09:06.498005Z","signature_b64":"860AaUDclIjOBcK3JS5Hpj6VgyorY4BArsG8mJZ04kUY8QlAw8GqAGn6MmDELD0xvvhqst/gHoifRkCYqe86BQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"2239a75367f0e3e6b4066c9728b82bdc762fa9ebcf8ab6889e920bd4fc1d6878","last_reissued_at":"2026-05-18T01:09:06.497492Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T01:09:06.497492Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Electromagnetic probes of a pure-glue initial state in nucleus-nucleus collisions at energies available at the CERN Large Hadron Collider","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ph"],"primary_cat":"nucl-th","authors_text":"B. K\\\"ampfer, H. Stoecker, I. N. Mishustin, Iu. A. Karpenko, L. M. Satarov, M. I. Gorenstein, V. Vovchenko","submitted_at":"2016-04-21T14:58:39Z","abstract_excerpt":"Partonic matter produced in the early stage of ultrarelativistic nucleus-nucleus collisions is assumed to be composed mainly of gluons, and quarks and antiquarks are produced at later times. To study the implications of such a scenario, the dynamical evolution of a chemically nonequilibrated system is described by the ideal (2+1)-dimensional hydrodynamics with a time dependent (anti)quark fugacity. The equation of state interpolates linearly between the lattice data for the pure gluonic matter and the lattice data for the chemically equilibrated quark-gluon plasma. The spectra and elliptic flo"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1604.06346","kind":"arxiv","version":3},"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":"1604.06346","created_at":"2026-05-18T01:09:06.497572+00:00"},{"alias_kind":"arxiv_version","alias_value":"1604.06346v3","created_at":"2026-05-18T01:09:06.497572+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1604.06346","created_at":"2026-05-18T01:09:06.497572+00:00"},{"alias_kind":"pith_short_12","alias_value":"EI42OU3H6DR6","created_at":"2026-05-18T12:30:12.583610+00:00"},{"alias_kind":"pith_short_16","alias_value":"EI42OU3H6DR6NNAG","created_at":"2026-05-18T12:30:12.583610+00:00"},{"alias_kind":"pith_short_8","alias_value":"EI42OU3H","created_at":"2026-05-18T12:30:12.583610+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/EI42OU3H6DR6NNAGNSLSROBL3R","json":"https://pith.science/pith/EI42OU3H6DR6NNAGNSLSROBL3R.json","graph_json":"https://pith.science/api/pith-number/EI42OU3H6DR6NNAGNSLSROBL3R/graph.json","events_json":"https://pith.science/api/pith-number/EI42OU3H6DR6NNAGNSLSROBL3R/events.json","paper":"https://pith.science/paper/EI42OU3H"},"agent_actions":{"view_html":"https://pith.science/pith/EI42OU3H6DR6NNAGNSLSROBL3R","download_json":"https://pith.science/pith/EI42OU3H6DR6NNAGNSLSROBL3R.json","view_paper":"https://pith.science/paper/EI42OU3H","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1604.06346&json=true","fetch_graph":"https://pith.science/api/pith-number/EI42OU3H6DR6NNAGNSLSROBL3R/graph.json","fetch_events":"https://pith.science/api/pith-number/EI42OU3H6DR6NNAGNSLSROBL3R/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/EI42OU3H6DR6NNAGNSLSROBL3R/action/timestamp_anchor","attest_storage":"https://pith.science/pith/EI42OU3H6DR6NNAGNSLSROBL3R/action/storage_attestation","attest_author":"https://pith.science/pith/EI42OU3H6DR6NNAGNSLSROBL3R/action/author_attestation","sign_citation":"https://pith.science/pith/EI42OU3H6DR6NNAGNSLSROBL3R/action/citation_signature","submit_replication":"https://pith.science/pith/EI42OU3H6DR6NNAGNSLSROBL3R/action/replication_record"}},"created_at":"2026-05-18T01:09:06.497572+00:00","updated_at":"2026-05-18T01:09:06.497572+00:00"}