{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2024:JYYA5RSI6HNTUC7FT77ARMZ2RA","short_pith_number":"pith:JYYA5RSI","schema_version":"1.0","canonical_sha256":"4e300ec648f1db3a0be59ffe08b33a880fdf79933497e4b1281a471340dc6cb8","source":{"kind":"arxiv","id":"2403.06929","version":2},"attestation_state":"computed","paper":{"title":"NLO+NLL' accurate predictions for three-jet event shapes in hadronic Higgs decays","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Aude Gehrmann-De Ridder, Christian T Preuss, Daniel Reichelt, Steffen Schumann","submitted_at":"2024-03-11T17:17:08Z","abstract_excerpt":"We present resummed predictions at next-to-leading logarithmic accuracy matched to the exact next-to-leading order results for a set of classical event-shape observables in hadronic Higgs decays, i.e., for the channels $H\\to gg$ and $H\\to b\\bar{b}$. We furthermore consider soft-drop grooming of the hadronic final states and derive corresponding $\\text{NLO}+\\text{NLL}^\\prime$ predictions for the groomed thrust observable. Differences in the QCD radiation pattern of gluon- and quark-initiated final states are imprinted in the event-shape distributions, offering separation power for the two decay"},"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":"2403.06929","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2024-03-11T17:17:08Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"64c58491fab5aac9ca7dccbce6877c127a8a775eb7523e70a16a38e6a7a5c295","abstract_canon_sha256":"247ae1680cca87935ff36030a6a16be1d20c2c508a4e3001bcd41ff8d81d04f1"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T08:38:07.257952Z","signature_b64":"MeTemXh4VhiXeY99R3RoY3GO3ZYyLcH5CqJ1rWFftF/8Jilz4kWExv7pexGR+qlU4t+TZZdUwh0RoWqgCJcOBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4e300ec648f1db3a0be59ffe08b33a880fdf79933497e4b1281a471340dc6cb8","last_reissued_at":"2026-07-05T08:38:07.257482Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T08:38:07.257482Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"NLO+NLL' accurate predictions for three-jet event shapes in hadronic Higgs decays","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Aude Gehrmann-De Ridder, Christian T Preuss, Daniel Reichelt, Steffen Schumann","submitted_at":"2024-03-11T17:17:08Z","abstract_excerpt":"We present resummed predictions at next-to-leading logarithmic accuracy matched to the exact next-to-leading order results for a set of classical event-shape observables in hadronic Higgs decays, i.e., for the channels $H\\to gg$ and $H\\to b\\bar{b}$. We furthermore consider soft-drop grooming of the hadronic final states and derive corresponding $\\text{NLO}+\\text{NLL}^\\prime$ predictions for the groomed thrust observable. Differences in the QCD radiation pattern of gluon- and quark-initiated final states are imprinted in the event-shape distributions, offering separation power for the two decay"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2403.06929","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/2403.06929/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":"2403.06929","created_at":"2026-07-05T08:38:07.257541+00:00"},{"alias_kind":"arxiv_version","alias_value":"2403.06929v2","created_at":"2026-07-05T08:38:07.257541+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2403.06929","created_at":"2026-07-05T08:38:07.257541+00:00"},{"alias_kind":"pith_short_12","alias_value":"JYYA5RSI6HNT","created_at":"2026-07-05T08:38:07.257541+00:00"},{"alias_kind":"pith_short_16","alias_value":"JYYA5RSI6HNTUC7F","created_at":"2026-07-05T08:38:07.257541+00:00"},{"alias_kind":"pith_short_8","alias_value":"JYYA5RSI","created_at":"2026-07-05T08:38:07.257541+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.20798","citing_title":"Phenomenology of heavy-flavour jet angularities at hadron colliders","ref_index":73,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/JYYA5RSI6HNTUC7FT77ARMZ2RA","json":"https://pith.science/pith/JYYA5RSI6HNTUC7FT77ARMZ2RA.json","graph_json":"https://pith.science/api/pith-number/JYYA5RSI6HNTUC7FT77ARMZ2RA/graph.json","events_json":"https://pith.science/api/pith-number/JYYA5RSI6HNTUC7FT77ARMZ2RA/events.json","paper":"https://pith.science/paper/JYYA5RSI"},"agent_actions":{"view_html":"https://pith.science/pith/JYYA5RSI6HNTUC7FT77ARMZ2RA","download_json":"https://pith.science/pith/JYYA5RSI6HNTUC7FT77ARMZ2RA.json","view_paper":"https://pith.science/paper/JYYA5RSI","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2403.06929&json=true","fetch_graph":"https://pith.science/api/pith-number/JYYA5RSI6HNTUC7FT77ARMZ2RA/graph.json","fetch_events":"https://pith.science/api/pith-number/JYYA5RSI6HNTUC7FT77ARMZ2RA/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/JYYA5RSI6HNTUC7FT77ARMZ2RA/action/timestamp_anchor","attest_storage":"https://pith.science/pith/JYYA5RSI6HNTUC7FT77ARMZ2RA/action/storage_attestation","attest_author":"https://pith.science/pith/JYYA5RSI6HNTUC7FT77ARMZ2RA/action/author_attestation","sign_citation":"https://pith.science/pith/JYYA5RSI6HNTUC7FT77ARMZ2RA/action/citation_signature","submit_replication":"https://pith.science/pith/JYYA5RSI6HNTUC7FT77ARMZ2RA/action/replication_record"}},"created_at":"2026-07-05T08:38:07.257541+00:00","updated_at":"2026-07-05T08:38:07.257541+00:00"}