{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:GH2NB633XMSWSF7223WI4V6WIR","short_pith_number":"pith:GH2NB633","schema_version":"1.0","canonical_sha256":"31f4d0fb7bbb256917fad6ec8e57d644732656a9fa1bbbb786f2d715d6eae5ff","source":{"kind":"arxiv","id":"1511.06039","version":4},"attestation_state":"computed","paper":{"title":"Combining $Q_T$ and small-$x$ resummations","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Simone Marzani","submitted_at":"2015-11-19T01:28:05Z","abstract_excerpt":"We analyze transverse momentum ($Q_T$) resummation of a colorless final state, e.g. Higgs production in gluon fusion or the production of a lepton pair via the Drell-Yan mechanism, in the limit where the invariant mass of the final state is much less then the center-of-mass energy, i.e. $Q^2\\ll s$. We show how the traditional resummation of logarithms of $Q_T/Q$ can be supplemented with the resummation of the leading logarithmic contributions at small $x=Q^2/s$ and we compute the necessary ingredients to perform such joint resummation."},"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":"1511.06039","kind":"arxiv","version":4},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2015-11-19T01:28:05Z","cross_cats_sorted":[],"title_canon_sha256":"9e9a37bfd294b07e902ac0745a239d87173ee734563735a258fe07ec137fd589","abstract_canon_sha256":"7c7c079bde65ae839d14c5922f188ad9adfedb0abbfeb50cddf2b2d03b0c821a"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T01:58:38.178002Z","signature_b64":"GIpeDUswkORfZdo+KUXn0SahyhT6BgzK4Swje6SuiQ/Iz7yJ0U07HSMxgTVO8rXmfKVsMWatxn/xZJA3xj+wBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"31f4d0fb7bbb256917fad6ec8e57d644732656a9fa1bbbb786f2d715d6eae5ff","last_reissued_at":"2026-07-05T01:58:38.177587Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T01:58:38.177587Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Combining $Q_T$ and small-$x$ resummations","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Simone Marzani","submitted_at":"2015-11-19T01:28:05Z","abstract_excerpt":"We analyze transverse momentum ($Q_T$) resummation of a colorless final state, e.g. Higgs production in gluon fusion or the production of a lepton pair via the Drell-Yan mechanism, in the limit where the invariant mass of the final state is much less then the center-of-mass energy, i.e. $Q^2\\ll s$. We show how the traditional resummation of logarithms of $Q_T/Q$ can be supplemented with the resummation of the leading logarithmic contributions at small $x=Q^2/s$ and we compute the necessary ingredients to perform such joint resummation."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1511.06039","kind":"arxiv","version":4},"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/1511.06039/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":"1511.06039","created_at":"2026-07-05T01:58:38.177645+00:00"},{"alias_kind":"arxiv_version","alias_value":"1511.06039v4","created_at":"2026-07-05T01:58:38.177645+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1511.06039","created_at":"2026-07-05T01:58:38.177645+00:00"},{"alias_kind":"pith_short_12","alias_value":"GH2NB633XMSW","created_at":"2026-07-05T01:58:38.177645+00:00"},{"alias_kind":"pith_short_16","alias_value":"GH2NB633XMSWSF72","created_at":"2026-07-05T01:58:38.177645+00:00"},{"alias_kind":"pith_short_8","alias_value":"GH2NB633","created_at":"2026-07-05T01:58:38.177645+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":3,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.20063","citing_title":"Toward Precision Fragmentation of $\\Omega_{3Q}$ Baryons: The OMG3Q1.1 Framework","ref_index":271,"is_internal_anchor":false},{"citing_arxiv_id":"2509.01703","citing_title":"The N$^3$LO Twist-2 Matching of Linearly Polarized Gluon TMDs","ref_index":42,"is_internal_anchor":false},{"citing_arxiv_id":"2605.01539","citing_title":"Multimodal Fragmentation of All-Heavy Pentaquarks: Uncertainty-Aware Predictions for Hadron Colliders","ref_index":228,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/GH2NB633XMSWSF7223WI4V6WIR","json":"https://pith.science/pith/GH2NB633XMSWSF7223WI4V6WIR.json","graph_json":"https://pith.science/api/pith-number/GH2NB633XMSWSF7223WI4V6WIR/graph.json","events_json":"https://pith.science/api/pith-number/GH2NB633XMSWSF7223WI4V6WIR/events.json","paper":"https://pith.science/paper/GH2NB633"},"agent_actions":{"view_html":"https://pith.science/pith/GH2NB633XMSWSF7223WI4V6WIR","download_json":"https://pith.science/pith/GH2NB633XMSWSF7223WI4V6WIR.json","view_paper":"https://pith.science/paper/GH2NB633","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1511.06039&json=true","fetch_graph":"https://pith.science/api/pith-number/GH2NB633XMSWSF7223WI4V6WIR/graph.json","fetch_events":"https://pith.science/api/pith-number/GH2NB633XMSWSF7223WI4V6WIR/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/GH2NB633XMSWSF7223WI4V6WIR/action/timestamp_anchor","attest_storage":"https://pith.science/pith/GH2NB633XMSWSF7223WI4V6WIR/action/storage_attestation","attest_author":"https://pith.science/pith/GH2NB633XMSWSF7223WI4V6WIR/action/author_attestation","sign_citation":"https://pith.science/pith/GH2NB633XMSWSF7223WI4V6WIR/action/citation_signature","submit_replication":"https://pith.science/pith/GH2NB633XMSWSF7223WI4V6WIR/action/replication_record"}},"created_at":"2026-07-05T01:58:38.177645+00:00","updated_at":"2026-07-05T01:58:38.177645+00:00"}