{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2019:P7A7TO7D7ZKMUXBAJ6VENWTO3R","short_pith_number":"pith:P7A7TO7D","schema_version":"1.0","canonical_sha256":"7fc1f9bbe3fe54ca5c204faa46da6edc529b3457c57ae007a9b1976be4c3af07","source":{"kind":"arxiv","id":"1902.06254","version":2},"attestation_state":"computed","paper":{"title":"Impact of Glasma on heavy quark observables in nucleus-nucleus collisions at LHC","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"Gabriele Coci, Marco Ruggieri, Salvatore Plumari, Santosh Kumar Das, Vincenzo Greco, Yifeng Sun","submitted_at":"2019-02-17T13:06:11Z","abstract_excerpt":"In the pre-thermal equilibrium stage of relativistic heavy-ion collisions, a strong quasi-classical transverse gluon field emerges at about $\\tau_0 \\simeq 0.1 \\, \\rm fm/c$ and evolves together with their longitudinal counterparts according to the classical Yang-Mills (CYM) equations. Recently it has been shown that these fields induce a diffusion of charm quarks in momentum space resulting in a tilt of their spectrum without a significant drag. We find that in nucleus-nucleus collisions at LHC such a novel dynamics of charm quarks leads to an initial enhancement of the nuclear modification fac"},"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":"1902.06254","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"nucl-th","submitted_at":"2019-02-17T13:06:11Z","cross_cats_sorted":[],"title_canon_sha256":"328774d7916bb006ecc6b33c9abacb1532351b3393859be5ca5952578238cc01","abstract_canon_sha256":"24a87dfd2adf8850fe102c7712a9b4724cd4890fc4eb28714658e618a5745417"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T00:05:33.947160Z","signature_b64":"m0nCmiK8tuL/DD35xRIMErZC8Prhtz2nOFkBXvrAdsojFyfAD9h+xVDlb+ilmhVC59Y9E7tnE6OiohRG/IpWDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"7fc1f9bbe3fe54ca5c204faa46da6edc529b3457c57ae007a9b1976be4c3af07","last_reissued_at":"2026-07-05T00:05:33.946697Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T00:05:33.946697Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Impact of Glasma on heavy quark observables in nucleus-nucleus collisions at LHC","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"nucl-th","authors_text":"Gabriele Coci, Marco Ruggieri, Salvatore Plumari, Santosh Kumar Das, Vincenzo Greco, Yifeng Sun","submitted_at":"2019-02-17T13:06:11Z","abstract_excerpt":"In the pre-thermal equilibrium stage of relativistic heavy-ion collisions, a strong quasi-classical transverse gluon field emerges at about $\\tau_0 \\simeq 0.1 \\, \\rm fm/c$ and evolves together with their longitudinal counterparts according to the classical Yang-Mills (CYM) equations. Recently it has been shown that these fields induce a diffusion of charm quarks in momentum space resulting in a tilt of their spectrum without a significant drag. We find that in nucleus-nucleus collisions at LHC such a novel dynamics of charm quarks leads to an initial enhancement of the nuclear modification fac"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1902.06254","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/1902.06254/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":"1902.06254","created_at":"2026-07-05T00:05:33.946753+00:00"},{"alias_kind":"arxiv_version","alias_value":"1902.06254v2","created_at":"2026-07-05T00:05:33.946753+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1902.06254","created_at":"2026-07-05T00:05:33.946753+00:00"},{"alias_kind":"pith_short_12","alias_value":"P7A7TO7D7ZKM","created_at":"2026-07-05T00:05:33.946753+00:00"},{"alias_kind":"pith_short_16","alias_value":"P7A7TO7D7ZKMUXBA","created_at":"2026-07-05T00:05:33.946753+00:00"},{"alias_kind":"pith_short_8","alias_value":"P7A7TO7D","created_at":"2026-07-05T00:05:33.946753+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":4,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2607.07796","citing_title":"Azimuthal momentum isotropization in the Quark-Gluon Plasma thermalization","ref_index":28,"is_internal_anchor":true},{"citing_arxiv_id":"2605.26766","citing_title":"Sensitivity of Heavy-Quark Dipolar Flow to its Initial Spatial Distributions in Cu+Au Collisions","ref_index":34,"is_internal_anchor":false},{"citing_arxiv_id":"2605.10413","citing_title":"Light-front Hamiltonian jet evolution in the Glasma","ref_index":47,"is_internal_anchor":false},{"citing_arxiv_id":"2604.08520","citing_title":"Kinetic and canonical momentum broadening in the Glasma","ref_index":23,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/P7A7TO7D7ZKMUXBAJ6VENWTO3R","json":"https://pith.science/pith/P7A7TO7D7ZKMUXBAJ6VENWTO3R.json","graph_json":"https://pith.science/api/pith-number/P7A7TO7D7ZKMUXBAJ6VENWTO3R/graph.json","events_json":"https://pith.science/api/pith-number/P7A7TO7D7ZKMUXBAJ6VENWTO3R/events.json","paper":"https://pith.science/paper/P7A7TO7D"},"agent_actions":{"view_html":"https://pith.science/pith/P7A7TO7D7ZKMUXBAJ6VENWTO3R","download_json":"https://pith.science/pith/P7A7TO7D7ZKMUXBAJ6VENWTO3R.json","view_paper":"https://pith.science/paper/P7A7TO7D","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1902.06254&json=true","fetch_graph":"https://pith.science/api/pith-number/P7A7TO7D7ZKMUXBAJ6VENWTO3R/graph.json","fetch_events":"https://pith.science/api/pith-number/P7A7TO7D7ZKMUXBAJ6VENWTO3R/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/P7A7TO7D7ZKMUXBAJ6VENWTO3R/action/timestamp_anchor","attest_storage":"https://pith.science/pith/P7A7TO7D7ZKMUXBAJ6VENWTO3R/action/storage_attestation","attest_author":"https://pith.science/pith/P7A7TO7D7ZKMUXBAJ6VENWTO3R/action/author_attestation","sign_citation":"https://pith.science/pith/P7A7TO7D7ZKMUXBAJ6VENWTO3R/action/citation_signature","submit_replication":"https://pith.science/pith/P7A7TO7D7ZKMUXBAJ6VENWTO3R/action/replication_record"}},"created_at":"2026-07-05T00:05:33.946753+00:00","updated_at":"2026-07-05T00:05:33.946753+00:00"}