{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2010:JNR5CTJ2HAJSSLGFH4FXCLA2IT","short_pith_number":"pith:JNR5CTJ2","schema_version":"1.0","canonical_sha256":"4b63d14d3a3813292cc53f0b712c1a44d8890bcc8beb565c81d07584fa7b2b0a","source":{"kind":"arxiv","id":"1009.4670","version":2},"attestation_state":"computed","paper":{"title":"Higgs boson pair production in new physics models at hadron, lepton, and photon colliders","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Daisuke Harada, Eri Asakawa, Koji Tsumura, Shinya Kanemura, Yasuhiro Okada","submitted_at":"2010-09-23T18:07:27Z","abstract_excerpt":"We study Higgs boson pair production processes at future hadron and lepton colliders including the photon collision option in several new physics models; i.e., the two-Higgs-doublet model, the scalar leptoquark model, the sequential fourth generation fermion model and the vector-like quark model. Cross sections for these processes can deviate significantly from the standard model predictions due to the one-loop correction to the triple Higgs boson coupling constant. For the one-loop induced processes such as $gg \\to hh$ and $\\gamma\\gamma\\to hh$, where $h$ is the (lightest) Higgs boson and $g$ "},"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":"1009.4670","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2010-09-23T18:07:27Z","cross_cats_sorted":[],"title_canon_sha256":"f19b3cc866b31e449d6ff324c79965cadfb3704d872d95e335e6d97f0aa327af","abstract_canon_sha256":"43938aca06d37c6aa06a094232551393d83982553ba34b41fd58106d5b48fcf9"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:32:36.005521Z","signature_b64":"UQfbH+MGAuSVAOtq1ep2FEv47jSMRNdFDZzmPGlMJ5piBW97FZ4iX5k3E53jBLLva4ntlBDkLoMIf9tDVzQuCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4b63d14d3a3813292cc53f0b712c1a44d8890bcc8beb565c81d07584fa7b2b0a","last_reissued_at":"2026-05-18T04:32:36.004981Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:32:36.004981Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Higgs boson pair production in new physics models at hadron, lepton, and photon colliders","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Daisuke Harada, Eri Asakawa, Koji Tsumura, Shinya Kanemura, Yasuhiro Okada","submitted_at":"2010-09-23T18:07:27Z","abstract_excerpt":"We study Higgs boson pair production processes at future hadron and lepton colliders including the photon collision option in several new physics models; i.e., the two-Higgs-doublet model, the scalar leptoquark model, the sequential fourth generation fermion model and the vector-like quark model. Cross sections for these processes can deviate significantly from the standard model predictions due to the one-loop correction to the triple Higgs boson coupling constant. For the one-loop induced processes such as $gg \\to hh$ and $\\gamma\\gamma\\to hh$, where $h$ is the (lightest) Higgs boson and $g$ "},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1009.4670","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":"1009.4670","created_at":"2026-05-18T04:32:36.005061+00:00"},{"alias_kind":"arxiv_version","alias_value":"1009.4670v2","created_at":"2026-05-18T04:32:36.005061+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1009.4670","created_at":"2026-05-18T04:32:36.005061+00:00"},{"alias_kind":"pith_short_12","alias_value":"JNR5CTJ2HAJS","created_at":"2026-05-18T12:26:09.077623+00:00"},{"alias_kind":"pith_short_16","alias_value":"JNR5CTJ2HAJSSLGF","created_at":"2026-05-18T12:26:09.077623+00:00"},{"alias_kind":"pith_short_8","alias_value":"JNR5CTJ2","created_at":"2026-05-18T12:26:09.077623+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2604.24421","citing_title":"Double SM-like Higgs Production at future $ e^+ e^- $ colliders in the 3-Higgs Doublet Model under the $ S_{3} $ symmetry","ref_index":21,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/JNR5CTJ2HAJSSLGFH4FXCLA2IT","json":"https://pith.science/pith/JNR5CTJ2HAJSSLGFH4FXCLA2IT.json","graph_json":"https://pith.science/api/pith-number/JNR5CTJ2HAJSSLGFH4FXCLA2IT/graph.json","events_json":"https://pith.science/api/pith-number/JNR5CTJ2HAJSSLGFH4FXCLA2IT/events.json","paper":"https://pith.science/paper/JNR5CTJ2"},"agent_actions":{"view_html":"https://pith.science/pith/JNR5CTJ2HAJSSLGFH4FXCLA2IT","download_json":"https://pith.science/pith/JNR5CTJ2HAJSSLGFH4FXCLA2IT.json","view_paper":"https://pith.science/paper/JNR5CTJ2","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1009.4670&json=true","fetch_graph":"https://pith.science/api/pith-number/JNR5CTJ2HAJSSLGFH4FXCLA2IT/graph.json","fetch_events":"https://pith.science/api/pith-number/JNR5CTJ2HAJSSLGFH4FXCLA2IT/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/JNR5CTJ2HAJSSLGFH4FXCLA2IT/action/timestamp_anchor","attest_storage":"https://pith.science/pith/JNR5CTJ2HAJSSLGFH4FXCLA2IT/action/storage_attestation","attest_author":"https://pith.science/pith/JNR5CTJ2HAJSSLGFH4FXCLA2IT/action/author_attestation","sign_citation":"https://pith.science/pith/JNR5CTJ2HAJSSLGFH4FXCLA2IT/action/citation_signature","submit_replication":"https://pith.science/pith/JNR5CTJ2HAJSSLGFH4FXCLA2IT/action/replication_record"}},"created_at":"2026-05-18T04:32:36.005061+00:00","updated_at":"2026-05-18T04:32:36.005061+00:00"}