{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2019:TYRYUBIFHKGPGQUXGIDNOFVGIG","short_pith_number":"pith:TYRYUBIF","schema_version":"1.0","canonical_sha256":"9e238a05053a8cf342973206d716a641a899dcdb5c45f13d0c2715b6b493ce0d","source":{"kind":"arxiv","id":"1905.03771","version":2},"attestation_state":"computed","paper":{"title":"Resummed prediction for Higgs boson production through $b\\bar{b}$ annihilation at N$^3$LL","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Ajjath A H, Amlan Chakraborty, Goutam Das, Pooja Mukherjee, V. Ravindran","submitted_at":"2019-05-09T17:54:35Z","abstract_excerpt":"We present an accurate theoretical prediction for the production of Higgs boson through bottom quark annihilation at the LHC up to next-to-next-to-next-to leading order (N$^3$LO) plus next-to-next-to-next-to-leading logarithmic (N$^3$LL) accuracy. We determine the third order perturbative Quantum Chromodynamics (QCD) correction to the process dependent constant in the resummed expression using the three loop bottom quark form factor and third order quark soft distribution function. Thanks to the recent computation of N$^3$LO corrections to this production cross-section from all the partonic ch"},"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":"1905.03771","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2019-05-09T17:54:35Z","cross_cats_sorted":[],"title_canon_sha256":"db79ff421ad868bdb8a861e9edee4005f1b3a6051b7d919f2c76cf14e3728716","abstract_canon_sha256":"f688fe905e2e6c792e1a5211a9503bccee7f67221c82830df2ce635be59a6062"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T00:28:22.868528Z","signature_b64":"gYMz8p+pQGjLeVgGyEr/33bBGtPnYVAogSIYCtR5r3pD/o+PpdxcYy16nVv32tXik8JgmGBC+fHg623xrvfbDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9e238a05053a8cf342973206d716a641a899dcdb5c45f13d0c2715b6b493ce0d","last_reissued_at":"2026-07-05T00:28:22.868126Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T00:28:22.868126Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Resummed prediction for Higgs boson production through $b\\bar{b}$ annihilation at N$^3$LL","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Ajjath A H, Amlan Chakraborty, Goutam Das, Pooja Mukherjee, V. Ravindran","submitted_at":"2019-05-09T17:54:35Z","abstract_excerpt":"We present an accurate theoretical prediction for the production of Higgs boson through bottom quark annihilation at the LHC up to next-to-next-to-next-to leading order (N$^3$LO) plus next-to-next-to-next-to-leading logarithmic (N$^3$LL) accuracy. We determine the third order perturbative Quantum Chromodynamics (QCD) correction to the process dependent constant in the resummed expression using the three loop bottom quark form factor and third order quark soft distribution function. Thanks to the recent computation of N$^3$LO corrections to this production cross-section from all the partonic ch"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1905.03771","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/1905.03771/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":"1905.03771","created_at":"2026-07-05T00:28:22.868186+00:00"},{"alias_kind":"arxiv_version","alias_value":"1905.03771v2","created_at":"2026-07-05T00:28:22.868186+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1905.03771","created_at":"2026-07-05T00:28:22.868186+00:00"},{"alias_kind":"pith_short_12","alias_value":"TYRYUBIFHKGP","created_at":"2026-07-05T00:28:22.868186+00:00"},{"alias_kind":"pith_short_16","alias_value":"TYRYUBIFHKGPGQUX","created_at":"2026-07-05T00:28:22.868186+00:00"},{"alias_kind":"pith_short_8","alias_value":"TYRYUBIF","created_at":"2026-07-05T00:28:22.868186+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2605.24131","citing_title":"Associated $ZH$ production in gluon fusion process at NLO+NLL","ref_index":38,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/TYRYUBIFHKGPGQUXGIDNOFVGIG","json":"https://pith.science/pith/TYRYUBIFHKGPGQUXGIDNOFVGIG.json","graph_json":"https://pith.science/api/pith-number/TYRYUBIFHKGPGQUXGIDNOFVGIG/graph.json","events_json":"https://pith.science/api/pith-number/TYRYUBIFHKGPGQUXGIDNOFVGIG/events.json","paper":"https://pith.science/paper/TYRYUBIF"},"agent_actions":{"view_html":"https://pith.science/pith/TYRYUBIFHKGPGQUXGIDNOFVGIG","download_json":"https://pith.science/pith/TYRYUBIFHKGPGQUXGIDNOFVGIG.json","view_paper":"https://pith.science/paper/TYRYUBIF","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1905.03771&json=true","fetch_graph":"https://pith.science/api/pith-number/TYRYUBIFHKGPGQUXGIDNOFVGIG/graph.json","fetch_events":"https://pith.science/api/pith-number/TYRYUBIFHKGPGQUXGIDNOFVGIG/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/TYRYUBIFHKGPGQUXGIDNOFVGIG/action/timestamp_anchor","attest_storage":"https://pith.science/pith/TYRYUBIFHKGPGQUXGIDNOFVGIG/action/storage_attestation","attest_author":"https://pith.science/pith/TYRYUBIFHKGPGQUXGIDNOFVGIG/action/author_attestation","sign_citation":"https://pith.science/pith/TYRYUBIFHKGPGQUXGIDNOFVGIG/action/citation_signature","submit_replication":"https://pith.science/pith/TYRYUBIFHKGPGQUXGIDNOFVGIG/action/replication_record"}},"created_at":"2026-07-05T00:28:22.868186+00:00","updated_at":"2026-07-05T00:28:22.868186+00:00"}