{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2001:WO7N3KMBS23ZRSQ2I2P777WCA2","short_pith_number":"pith:WO7N3KMB","schema_version":"1.0","canonical_sha256":"b3bedda98196b798ca1a469ffffec206852147e2606e32ea55c7b5aa19bf6402","source":{"kind":"arxiv","id":"hep-ph/0103217","version":3},"attestation_state":"computed","paper":{"title":"Renormalon resummation and exponentiation of soft and collinear gluon radiation in the thrust distribution","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Einan Gardi, Johan Rathsman","submitted_at":"2001-03-20T21:42:24Z","abstract_excerpt":"The thrust distribution in e+e- annihilation is calculated exploiting its exponentiation property in the two-jet region t = 1-T << 1. We present a general method (DGE) to calculate a large class of logarithmically enhanced terms, using the dispersive approach in renormalon calculus. Dressed Gluon Exponentiation is based on the fact that the exponentiation kernel is associated primarily with a single gluon emission, and therefore the exponent is naturally represented as an integral over the running coupling. Fixing the definition of Lambda is enough to guarantee consistency with the exact expon"},"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-ph/0103217","kind":"arxiv","version":3},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"2001-03-20T21:42:24Z","cross_cats_sorted":[],"title_canon_sha256":"3930628d272c417db800df7af9d486c59ba5a3d5e37e5ad4eddb34d1902a1033","abstract_canon_sha256":"9ab799eac38b9f8c513d212b43d2a432a95a3b4eb815710a9b38a828820846fa"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T16:27:17.337946Z","signature_b64":"5ekBVMUw0gj2y+eXy3fMM3Y3YW5kjSuLp+09GpqKVyANfrYHLYJHH353annX3PXWhVUvU9+Leqw7PjnJrjnyDg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b3bedda98196b798ca1a469ffffec206852147e2606e32ea55c7b5aa19bf6402","last_reissued_at":"2026-07-04T16:27:17.337550Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T16:27:17.337550Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Renormalon resummation and exponentiation of soft and collinear gluon radiation in the thrust distribution","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Einan Gardi, Johan Rathsman","submitted_at":"2001-03-20T21:42:24Z","abstract_excerpt":"The thrust distribution in e+e- annihilation is calculated exploiting its exponentiation property in the two-jet region t = 1-T << 1. We present a general method (DGE) to calculate a large class of logarithmically enhanced terms, using the dispersive approach in renormalon calculus. Dressed Gluon Exponentiation is based on the fact that the exponentiation kernel is associated primarily with a single gluon emission, and therefore the exponent is naturally represented as an integral over the running coupling. Fixing the definition of Lambda is enough to guarantee consistency with the exact expon"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/0103217","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/hep-ph/0103217/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":"hep-ph/0103217","created_at":"2026-07-04T16:27:17.337625+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/0103217v3","created_at":"2026-07-04T16:27:17.337625+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/0103217","created_at":"2026-07-04T16:27:17.337625+00:00"},{"alias_kind":"pith_short_12","alias_value":"WO7N3KMBS23Z","created_at":"2026-07-04T16:27:17.337625+00:00"},{"alias_kind":"pith_short_16","alias_value":"WO7N3KMBS23ZRSQ2","created_at":"2026-07-04T16:27:17.337625+00:00"},{"alias_kind":"pith_short_8","alias_value":"WO7N3KMB","created_at":"2026-07-04T16:27:17.337625+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2506.09130","citing_title":"Precision $e^+e^-$ Hemisphere Masses in the Dijet Region with Power Corrections","ref_index":84,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/WO7N3KMBS23ZRSQ2I2P777WCA2","json":"https://pith.science/pith/WO7N3KMBS23ZRSQ2I2P777WCA2.json","graph_json":"https://pith.science/api/pith-number/WO7N3KMBS23ZRSQ2I2P777WCA2/graph.json","events_json":"https://pith.science/api/pith-number/WO7N3KMBS23ZRSQ2I2P777WCA2/events.json","paper":"https://pith.science/paper/WO7N3KMB"},"agent_actions":{"view_html":"https://pith.science/pith/WO7N3KMBS23ZRSQ2I2P777WCA2","download_json":"https://pith.science/pith/WO7N3KMBS23ZRSQ2I2P777WCA2.json","view_paper":"https://pith.science/paper/WO7N3KMB","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/0103217&json=true","fetch_graph":"https://pith.science/api/pith-number/WO7N3KMBS23ZRSQ2I2P777WCA2/graph.json","fetch_events":"https://pith.science/api/pith-number/WO7N3KMBS23ZRSQ2I2P777WCA2/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/WO7N3KMBS23ZRSQ2I2P777WCA2/action/timestamp_anchor","attest_storage":"https://pith.science/pith/WO7N3KMBS23ZRSQ2I2P777WCA2/action/storage_attestation","attest_author":"https://pith.science/pith/WO7N3KMBS23ZRSQ2I2P777WCA2/action/author_attestation","sign_citation":"https://pith.science/pith/WO7N3KMBS23ZRSQ2I2P777WCA2/action/citation_signature","submit_replication":"https://pith.science/pith/WO7N3KMBS23ZRSQ2I2P777WCA2/action/replication_record"}},"created_at":"2026-07-04T16:27:17.337625+00:00","updated_at":"2026-07-04T16:27:17.337625+00:00"}