{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2023:SZEWHD2LAQMEYLLX53XSIAVHXT","short_pith_number":"pith:SZEWHD2L","schema_version":"1.0","canonical_sha256":"9649638f4b04184c2d77eeef2402a7bceca1ffbbf9ce12c7b21b44d0947034a6","source":{"kind":"arxiv","id":"2306.09619","version":2},"attestation_state":"computed","paper":{"title":"Early-times Yang-Mills dynamics and the characterization of strongly interacting matter with statistical learning","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ph","nucl-ex"],"primary_cat":"nucl-th","authors_text":"Charles Gale, Jean-Fran\\c{c}ois Paquet, Matthew R. Heffernan, Sangyong Jeon","submitted_at":"2023-06-16T04:22:57Z","abstract_excerpt":"In ultrarelativistic heavy-ion collisions, a plasma of deconfined quarks and gluons is formed within $1$ fm/c of the nuclei's impact. The complex dynamics of the collision before $\\approx 1$ fm/c is often described with parametric models, which affect the predictivity of calculations. In this work, we perform a systematic analysis of LHC measurements from Pb-Pb collisions, by combining an \\emph{ab-initio} model of the early stage of the collisions with a hydrodynamic model of the plasma. We obtain state-of-the-art constraints on the shear and bulk viscosity of quark-gluon plasma. We mitigate t"},"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":"2306.09619","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"nucl-th","submitted_at":"2023-06-16T04:22:57Z","cross_cats_sorted":["hep-ph","nucl-ex"],"title_canon_sha256":"8ec6b1c619d024cbd8c874d3d3fba1a758eed52896dca547db310d2cc1065651","abstract_canon_sha256":"7591c35f016277c9328d37cfdfd0b8d367ebc22e3597772a92e31853ec89a1de"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T08:34:55.123801Z","signature_b64":"3vc9rbcQAfu9ozWPs3Yi808WAN7ALt7alu6ARcPlF2dMm6+PnO/1p6rfrVJKK1OBbHgBJiPPBfUsUC8kiQ45Ag==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9649638f4b04184c2d77eeef2402a7bceca1ffbbf9ce12c7b21b44d0947034a6","last_reissued_at":"2026-07-05T08:34:55.123381Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T08:34:55.123381Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Early-times Yang-Mills dynamics and the characterization of strongly interacting matter with statistical learning","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ph","nucl-ex"],"primary_cat":"nucl-th","authors_text":"Charles Gale, Jean-Fran\\c{c}ois Paquet, Matthew R. Heffernan, Sangyong Jeon","submitted_at":"2023-06-16T04:22:57Z","abstract_excerpt":"In ultrarelativistic heavy-ion collisions, a plasma of deconfined quarks and gluons is formed within $1$ fm/c of the nuclei's impact. The complex dynamics of the collision before $\\approx 1$ fm/c is often described with parametric models, which affect the predictivity of calculations. In this work, we perform a systematic analysis of LHC measurements from Pb-Pb collisions, by combining an \\emph{ab-initio} model of the early stage of the collisions with a hydrodynamic model of the plasma. We obtain state-of-the-art constraints on the shear and bulk viscosity of quark-gluon plasma. We mitigate t"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2306.09619","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/2306.09619/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":"2306.09619","created_at":"2026-07-05T08:34:55.123438+00:00"},{"alias_kind":"arxiv_version","alias_value":"2306.09619v2","created_at":"2026-07-05T08:34:55.123438+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2306.09619","created_at":"2026-07-05T08:34:55.123438+00:00"},{"alias_kind":"pith_short_12","alias_value":"SZEWHD2LAQME","created_at":"2026-07-05T08:34:55.123438+00:00"},{"alias_kind":"pith_short_16","alias_value":"SZEWHD2LAQMEYLLX","created_at":"2026-07-05T08:34:55.123438+00:00"},{"alias_kind":"pith_short_8","alias_value":"SZEWHD2L","created_at":"2026-07-05T08:34:55.123438+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2509.10743","citing_title":"Glauber quark and gluon contributions to quark energy loss at next-to-leading order and next-to-leading twist","ref_index":21,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/SZEWHD2LAQMEYLLX53XSIAVHXT","json":"https://pith.science/pith/SZEWHD2LAQMEYLLX53XSIAVHXT.json","graph_json":"https://pith.science/api/pith-number/SZEWHD2LAQMEYLLX53XSIAVHXT/graph.json","events_json":"https://pith.science/api/pith-number/SZEWHD2LAQMEYLLX53XSIAVHXT/events.json","paper":"https://pith.science/paper/SZEWHD2L"},"agent_actions":{"view_html":"https://pith.science/pith/SZEWHD2LAQMEYLLX53XSIAVHXT","download_json":"https://pith.science/pith/SZEWHD2LAQMEYLLX53XSIAVHXT.json","view_paper":"https://pith.science/paper/SZEWHD2L","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2306.09619&json=true","fetch_graph":"https://pith.science/api/pith-number/SZEWHD2LAQMEYLLX53XSIAVHXT/graph.json","fetch_events":"https://pith.science/api/pith-number/SZEWHD2LAQMEYLLX53XSIAVHXT/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/SZEWHD2LAQMEYLLX53XSIAVHXT/action/timestamp_anchor","attest_storage":"https://pith.science/pith/SZEWHD2LAQMEYLLX53XSIAVHXT/action/storage_attestation","attest_author":"https://pith.science/pith/SZEWHD2LAQMEYLLX53XSIAVHXT/action/author_attestation","sign_citation":"https://pith.science/pith/SZEWHD2LAQMEYLLX53XSIAVHXT/action/citation_signature","submit_replication":"https://pith.science/pith/SZEWHD2LAQMEYLLX53XSIAVHXT/action/replication_record"}},"created_at":"2026-07-05T08:34:55.123438+00:00","updated_at":"2026-07-05T08:34:55.123438+00:00"}