{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2017:KUUGL2FZP35FIYKMPKPC2AQNBU","short_pith_number":"pith:KUUGL2FZ","schema_version":"1.0","canonical_sha256":"552865e8b97efa54614c7a9e2d020d0d03e6f94021824737e0277141df9190db","source":{"kind":"arxiv","id":"1709.07799","version":2},"attestation_state":"computed","paper":{"title":"Reconstruction of top-quark mass effects in Higgs pair production and other gluon-fusion processes","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Andreas Maier, Ramona Gr\\\"ober, Thomas Rauh","submitted_at":"2017-09-22T15:00:19Z","abstract_excerpt":"We propose a novel method for the treatment of top-quark mass effects in the production of $H^{(*)}$, $HH$, $HZ$ and $ZZ$ final states in gluon fusion. We show that it is possible to reconstruct the full top-quark mass dependence of the virtual amplitudes from the corresponding large-$m_t$ expansion and the non-analytic part of the amplitude near the top-quark threshold $\\hat{s}=4m_t^2$ with a Pad\\'e ansatz. The reliability of our method is clearly demonstrated by a comparison with the recent NLO result for Higgs pair production with full top-quark mass dependence."},"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":"1709.07799","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2017-09-22T15:00:19Z","cross_cats_sorted":[],"title_canon_sha256":"f5ff9491d5c6870d5b4bfc2ddb2e1bc6cacd1934b5e3800c3a411142d281fbae","abstract_canon_sha256":"9f416388cec487ee1e56dd99f498a113ee733fd0f14e44f7b18304dd72aed54b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:21:56.868190Z","signature_b64":"Fq9TZD+KQY0IUDSqhJbgqHDd3nCYzuAVfSfYLshUbb7xia2w1PliAN2ApjBb1jXFrbWIRQ7GHxpi9cJew1aQBg==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"552865e8b97efa54614c7a9e2d020d0d03e6f94021824737e0277141df9190db","last_reissued_at":"2026-05-18T00:21:56.867403Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:21:56.867403Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Reconstruction of top-quark mass effects in Higgs pair production and other gluon-fusion processes","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Andreas Maier, Ramona Gr\\\"ober, Thomas Rauh","submitted_at":"2017-09-22T15:00:19Z","abstract_excerpt":"We propose a novel method for the treatment of top-quark mass effects in the production of $H^{(*)}$, $HH$, $HZ$ and $ZZ$ final states in gluon fusion. We show that it is possible to reconstruct the full top-quark mass dependence of the virtual amplitudes from the corresponding large-$m_t$ expansion and the non-analytic part of the amplitude near the top-quark threshold $\\hat{s}=4m_t^2$ with a Pad\\'e ansatz. The reliability of our method is clearly demonstrated by a comparison with the recent NLO result for Higgs pair production with full top-quark mass dependence."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1709.07799","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":"1709.07799","created_at":"2026-05-18T00:21:56.867521+00:00"},{"alias_kind":"arxiv_version","alias_value":"1709.07799v2","created_at":"2026-05-18T00:21:56.867521+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1709.07799","created_at":"2026-05-18T00:21:56.867521+00:00"},{"alias_kind":"pith_short_12","alias_value":"KUUGL2FZP35F","created_at":"2026-05-18T12:31:28.150371+00:00"},{"alias_kind":"pith_short_16","alias_value":"KUUGL2FZP35FIYKM","created_at":"2026-05-18T12:31:28.150371+00:00"},{"alias_kind":"pith_short_8","alias_value":"KUUGL2FZ","created_at":"2026-05-18T12:31:28.150371+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/KUUGL2FZP35FIYKMPKPC2AQNBU","json":"https://pith.science/pith/KUUGL2FZP35FIYKMPKPC2AQNBU.json","graph_json":"https://pith.science/api/pith-number/KUUGL2FZP35FIYKMPKPC2AQNBU/graph.json","events_json":"https://pith.science/api/pith-number/KUUGL2FZP35FIYKMPKPC2AQNBU/events.json","paper":"https://pith.science/paper/KUUGL2FZ"},"agent_actions":{"view_html":"https://pith.science/pith/KUUGL2FZP35FIYKMPKPC2AQNBU","download_json":"https://pith.science/pith/KUUGL2FZP35FIYKMPKPC2AQNBU.json","view_paper":"https://pith.science/paper/KUUGL2FZ","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1709.07799&json=true","fetch_graph":"https://pith.science/api/pith-number/KUUGL2FZP35FIYKMPKPC2AQNBU/graph.json","fetch_events":"https://pith.science/api/pith-number/KUUGL2FZP35FIYKMPKPC2AQNBU/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/KUUGL2FZP35FIYKMPKPC2AQNBU/action/timestamp_anchor","attest_storage":"https://pith.science/pith/KUUGL2FZP35FIYKMPKPC2AQNBU/action/storage_attestation","attest_author":"https://pith.science/pith/KUUGL2FZP35FIYKMPKPC2AQNBU/action/author_attestation","sign_citation":"https://pith.science/pith/KUUGL2FZP35FIYKMPKPC2AQNBU/action/citation_signature","submit_replication":"https://pith.science/pith/KUUGL2FZP35FIYKMPKPC2AQNBU/action/replication_record"}},"created_at":"2026-05-18T00:21:56.867521+00:00","updated_at":"2026-05-18T00:21:56.867521+00:00"}