{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2016:I4Y3LDTDA2K7JTV2HAT2CALFKH","short_pith_number":"pith:I4Y3LDTD","schema_version":"1.0","canonical_sha256":"4731b58e630695f4ceba3827a1016551fc91dd523c4ab9393f6bfaa6f72cc461","source":{"kind":"arxiv","id":"1611.08610","version":2},"attestation_state":"computed","paper":{"title":"Resummation of Transverse Momentum Distributions in Distribution Space","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Frank J. Tackmann, Markus A. Ebert","submitted_at":"2016-11-25T21:00:06Z","abstract_excerpt":"Differential spectra in observables that resolve additional soft or collinear QCD emissions exhibit Sudakov double logarithms in the form of logarithmic plus distributions. Important examples are the total transverse momentum $q_T$ in color-singlet production, N-jettiness (with thrust or beam thrust as special cases), but also jet mass and more complicated jet substructure observables. The all-order logarithmic structure of such distributions is often fully encoded in differential equations, so-called (renormalization group) evolution equations. We introduce a well-defined technique of distrib"},"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":"1611.08610","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2016-11-25T21:00:06Z","cross_cats_sorted":[],"title_canon_sha256":"d61513b0d52cfc0daa1d34858659872e407ec3ec9b2ef1863b780edb76129486","abstract_canon_sha256":"e1e1528945e0c97160d2f2a8f74e587043fe8ef1e67dd6145fbddf8b84dfec52"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:50:09.233627Z","signature_b64":"IUm5GeDu57yYH6JD+iPOoPtmFv+E1CDc55fpIWyGRF6kk0TYmypD31fvflEKT2/Ti8nuQzOwO5nVd4Lcpt7zDw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4731b58e630695f4ceba3827a1016551fc91dd523c4ab9393f6bfaa6f72cc461","last_reissued_at":"2026-05-18T00:50:09.232983Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:50:09.232983Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Resummation of Transverse Momentum Distributions in Distribution Space","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Frank J. Tackmann, Markus A. Ebert","submitted_at":"2016-11-25T21:00:06Z","abstract_excerpt":"Differential spectra in observables that resolve additional soft or collinear QCD emissions exhibit Sudakov double logarithms in the form of logarithmic plus distributions. Important examples are the total transverse momentum $q_T$ in color-singlet production, N-jettiness (with thrust or beam thrust as special cases), but also jet mass and more complicated jet substructure observables. The all-order logarithmic structure of such distributions is often fully encoded in differential equations, so-called (renormalization group) evolution equations. We introduce a well-defined technique of distrib"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1611.08610","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":""},"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":"1611.08610","created_at":"2026-05-18T00:50:09.233099+00:00"},{"alias_kind":"arxiv_version","alias_value":"1611.08610v2","created_at":"2026-05-18T00:50:09.233099+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1611.08610","created_at":"2026-05-18T00:50:09.233099+00:00"},{"alias_kind":"pith_short_12","alias_value":"I4Y3LDTDA2K7","created_at":"2026-05-18T12:30:22.444734+00:00"},{"alias_kind":"pith_short_16","alias_value":"I4Y3LDTDA2K7JTV2","created_at":"2026-05-18T12:30:22.444734+00:00"},{"alias_kind":"pith_short_8","alias_value":"I4Y3LDTD","created_at":"2026-05-18T12:30:22.444734+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/I4Y3LDTDA2K7JTV2HAT2CALFKH","json":"https://pith.science/pith/I4Y3LDTDA2K7JTV2HAT2CALFKH.json","graph_json":"https://pith.science/api/pith-number/I4Y3LDTDA2K7JTV2HAT2CALFKH/graph.json","events_json":"https://pith.science/api/pith-number/I4Y3LDTDA2K7JTV2HAT2CALFKH/events.json","paper":"https://pith.science/paper/I4Y3LDTD"},"agent_actions":{"view_html":"https://pith.science/pith/I4Y3LDTDA2K7JTV2HAT2CALFKH","download_json":"https://pith.science/pith/I4Y3LDTDA2K7JTV2HAT2CALFKH.json","view_paper":"https://pith.science/paper/I4Y3LDTD","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1611.08610&json=true","fetch_graph":"https://pith.science/api/pith-number/I4Y3LDTDA2K7JTV2HAT2CALFKH/graph.json","fetch_events":"https://pith.science/api/pith-number/I4Y3LDTDA2K7JTV2HAT2CALFKH/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/I4Y3LDTDA2K7JTV2HAT2CALFKH/action/timestamp_anchor","attest_storage":"https://pith.science/pith/I4Y3LDTDA2K7JTV2HAT2CALFKH/action/storage_attestation","attest_author":"https://pith.science/pith/I4Y3LDTDA2K7JTV2HAT2CALFKH/action/author_attestation","sign_citation":"https://pith.science/pith/I4Y3LDTDA2K7JTV2HAT2CALFKH/action/citation_signature","submit_replication":"https://pith.science/pith/I4Y3LDTDA2K7JTV2HAT2CALFKH/action/replication_record"}},"created_at":"2026-05-18T00:50:09.233099+00:00","updated_at":"2026-05-18T00:50:09.233099+00:00"}