{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2002:ZYXQNEFURKIL3H2VBD4VJIROR5","short_pith_number":"pith:ZYXQNEFU","schema_version":"1.0","canonical_sha256":"ce2f0690b48a90bd9f5508f954a22e8f5d0b89b267f5cfb7163d773b66dc21c3","source":{"kind":"arxiv","id":"hep-ex/0206052","version":1},"attestation_state":"computed","paper":{"title":"Determination of alphaS from Hadronic Event Shapes in e+e- Annihilation at 192 < sqrt(s) < 208 GeV","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"L3 Collaboration","submitted_at":"2002-06-20T18:48:06Z","abstract_excerpt":"Results are presented from a study of the structure of high energy hadronic events recorded by the L3 detector at sqrt(s)>192 GeV. The distributions of several event shape variables are compared to resummed O(alphaS^2) QCD calculations. We determine the strong coupling constant at three average centre-of-mass energies: 194.4, 200.2 and 206.2 GeV. These measurements, combined with previous L3 measurements at lower energies, demonstrate the running of alphaS as expected in QCD and yield alphaS(mZ) = 0.1227 +- 0.0012 +- 0.0058, where the first uncertainty is experimental and the second is theoret"},"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":"hep-ex/0206052","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ex","submitted_at":"2002-06-20T18:48:06Z","cross_cats_sorted":[],"title_canon_sha256":"bf5fc2181ec7a8ad986b1e3f16d26c3e240df178ff15790733d71437cfee23f5","abstract_canon_sha256":"30ce95a70d6a36392e92328cc83b5a3c89f15785e4d0eb8c871f01ce2d41b966"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T03:47:32.391020Z","signature_b64":"yxDN35OlL+YoDS/1lc6P1+xKUoLpEXQ32u05PqKpS9Ebssl49GN6LCIgSnnBEeSqTDAE6ULm7oH1MwXGNJYJAg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ce2f0690b48a90bd9f5508f954a22e8f5d0b89b267f5cfb7163d773b66dc21c3","last_reissued_at":"2026-05-18T03:47:32.390551Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T03:47:32.390551Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Determination of alphaS from Hadronic Event Shapes in e+e- Annihilation at 192 < sqrt(s) < 208 GeV","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"L3 Collaboration","submitted_at":"2002-06-20T18:48:06Z","abstract_excerpt":"Results are presented from a study of the structure of high energy hadronic events recorded by the L3 detector at sqrt(s)>192 GeV. The distributions of several event shape variables are compared to resummed O(alphaS^2) QCD calculations. We determine the strong coupling constant at three average centre-of-mass energies: 194.4, 200.2 and 206.2 GeV. These measurements, combined with previous L3 measurements at lower energies, demonstrate the running of alphaS as expected in QCD and yield alphaS(mZ) = 0.1227 +- 0.0012 +- 0.0058, where the first uncertainty is experimental and the second is theoret"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ex/0206052","kind":"arxiv","version":1},"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":"hep-ex/0206052","created_at":"2026-05-18T03:47:32.390615+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ex/0206052v1","created_at":"2026-05-18T03:47:32.390615+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ex/0206052","created_at":"2026-05-18T03:47:32.390615+00:00"},{"alias_kind":"pith_short_12","alias_value":"ZYXQNEFURKIL","created_at":"2026-05-18T12:25:51.375804+00:00"},{"alias_kind":"pith_short_16","alias_value":"ZYXQNEFURKIL3H2V","created_at":"2026-05-18T12:25:51.375804+00:00"},{"alias_kind":"pith_short_8","alias_value":"ZYXQNEFU","created_at":"2026-05-18T12:25:51.375804+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2501.18173","citing_title":"Fits of $\\alpha_s$ from event-shapes in the three-jet region: extension to all energies","ref_index":25,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/ZYXQNEFURKIL3H2VBD4VJIROR5","json":"https://pith.science/pith/ZYXQNEFURKIL3H2VBD4VJIROR5.json","graph_json":"https://pith.science/api/pith-number/ZYXQNEFURKIL3H2VBD4VJIROR5/graph.json","events_json":"https://pith.science/api/pith-number/ZYXQNEFURKIL3H2VBD4VJIROR5/events.json","paper":"https://pith.science/paper/ZYXQNEFU"},"agent_actions":{"view_html":"https://pith.science/pith/ZYXQNEFURKIL3H2VBD4VJIROR5","download_json":"https://pith.science/pith/ZYXQNEFURKIL3H2VBD4VJIROR5.json","view_paper":"https://pith.science/paper/ZYXQNEFU","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ex/0206052&json=true","fetch_graph":"https://pith.science/api/pith-number/ZYXQNEFURKIL3H2VBD4VJIROR5/graph.json","fetch_events":"https://pith.science/api/pith-number/ZYXQNEFURKIL3H2VBD4VJIROR5/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/ZYXQNEFURKIL3H2VBD4VJIROR5/action/timestamp_anchor","attest_storage":"https://pith.science/pith/ZYXQNEFURKIL3H2VBD4VJIROR5/action/storage_attestation","attest_author":"https://pith.science/pith/ZYXQNEFURKIL3H2VBD4VJIROR5/action/author_attestation","sign_citation":"https://pith.science/pith/ZYXQNEFURKIL3H2VBD4VJIROR5/action/citation_signature","submit_replication":"https://pith.science/pith/ZYXQNEFURKIL3H2VBD4VJIROR5/action/replication_record"}},"created_at":"2026-05-18T03:47:32.390615+00:00","updated_at":"2026-05-18T03:47:32.390615+00:00"}