{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2010:NK6ZTU2KDLZCECOJBFQOGIDIFZ","short_pith_number":"pith:NK6ZTU2K","schema_version":"1.0","canonical_sha256":"6abd99d34a1af22209c90960e320682e5497853871ce88e3db117efe1d14b369","source":{"kind":"arxiv","id":"1004.0535","version":1},"attestation_state":"computed","paper":{"title":"Prospects for Observing the Standard Model Higgs Boson Decaying into b\\bar{b} Final States Produced in Weak Boson Fusion with an Associated Photon at the LHC","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"C. Santamarina, D. M. Asner, K. Randrianarivony, M. Cunningham, M. Schram, S. Dejong","submitted_at":"2010-04-04T21:31:30Z","abstract_excerpt":"One of the primary goals of the Large Hadron Collider is to understand the electroweak symmetry breaking mechanism. In the Standard Model, electroweak symmetry breaking is described by the Higgs mechanism which includes a scalar Higgs boson. Electroweak measurements constrain the Standard Model Higgs boson mass to be in the 114.4 to 157 GeV/c^2 range. Within this mass window, the Higgs predominantly decays into two b-quarks. As such, we investigate the prospect of observing the Standard Model Higgs decaying to b\\bar{b} produced in weak-boson-fusion with an associated central photon. An isolate"},"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":"1004.0535","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2010-04-04T21:31:30Z","cross_cats_sorted":[],"title_canon_sha256":"2996d561b266671016692c8b7b3968116a3becd41ede5bcb159e94922c78d5b9","abstract_canon_sha256":"97dd86e9148e25b9465b191a1bfd7254664d98b844c65b5cc2a31da83607b61c"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T04:36:33.817608Z","signature_b64":"VVUyTym2X2yUfey/oaDVodIfRysbZwujc8F3sKMvIEZymFmJ3YJjZdyyzSnS+fS9FKN8QbdDQF08yIeyJayrCQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"6abd99d34a1af22209c90960e320682e5497853871ce88e3db117efe1d14b369","last_reissued_at":"2026-05-18T04:36:33.817108Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T04:36:33.817108Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Prospects for Observing the Standard Model Higgs Boson Decaying into b\\bar{b} Final States Produced in Weak Boson Fusion with an Associated Photon at the LHC","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"C. Santamarina, D. M. Asner, K. Randrianarivony, M. Cunningham, M. Schram, S. Dejong","submitted_at":"2010-04-04T21:31:30Z","abstract_excerpt":"One of the primary goals of the Large Hadron Collider is to understand the electroweak symmetry breaking mechanism. In the Standard Model, electroweak symmetry breaking is described by the Higgs mechanism which includes a scalar Higgs boson. Electroweak measurements constrain the Standard Model Higgs boson mass to be in the 114.4 to 157 GeV/c^2 range. Within this mass window, the Higgs predominantly decays into two b-quarks. As such, we investigate the prospect of observing the Standard Model Higgs decaying to b\\bar{b} produced in weak-boson-fusion with an associated central photon. An isolate"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1004.0535","kind":"arxiv","version":1},"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":"1004.0535","created_at":"2026-05-18T04:36:33.817180+00:00"},{"alias_kind":"arxiv_version","alias_value":"1004.0535v1","created_at":"2026-05-18T04:36:33.817180+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1004.0535","created_at":"2026-05-18T04:36:33.817180+00:00"},{"alias_kind":"pith_short_12","alias_value":"NK6ZTU2KDLZC","created_at":"2026-05-18T12:26:10.704358+00:00"},{"alias_kind":"pith_short_16","alias_value":"NK6ZTU2KDLZCECOJ","created_at":"2026-05-18T12:26:10.704358+00:00"},{"alias_kind":"pith_short_8","alias_value":"NK6ZTU2K","created_at":"2026-05-18T12:26:10.704358+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/NK6ZTU2KDLZCECOJBFQOGIDIFZ","json":"https://pith.science/pith/NK6ZTU2KDLZCECOJBFQOGIDIFZ.json","graph_json":"https://pith.science/api/pith-number/NK6ZTU2KDLZCECOJBFQOGIDIFZ/graph.json","events_json":"https://pith.science/api/pith-number/NK6ZTU2KDLZCECOJBFQOGIDIFZ/events.json","paper":"https://pith.science/paper/NK6ZTU2K"},"agent_actions":{"view_html":"https://pith.science/pith/NK6ZTU2KDLZCECOJBFQOGIDIFZ","download_json":"https://pith.science/pith/NK6ZTU2KDLZCECOJBFQOGIDIFZ.json","view_paper":"https://pith.science/paper/NK6ZTU2K","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1004.0535&json=true","fetch_graph":"https://pith.science/api/pith-number/NK6ZTU2KDLZCECOJBFQOGIDIFZ/graph.json","fetch_events":"https://pith.science/api/pith-number/NK6ZTU2KDLZCECOJBFQOGIDIFZ/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/NK6ZTU2KDLZCECOJBFQOGIDIFZ/action/timestamp_anchor","attest_storage":"https://pith.science/pith/NK6ZTU2KDLZCECOJBFQOGIDIFZ/action/storage_attestation","attest_author":"https://pith.science/pith/NK6ZTU2KDLZCECOJBFQOGIDIFZ/action/author_attestation","sign_citation":"https://pith.science/pith/NK6ZTU2KDLZCECOJBFQOGIDIFZ/action/citation_signature","submit_replication":"https://pith.science/pith/NK6ZTU2KDLZCECOJBFQOGIDIFZ/action/replication_record"}},"created_at":"2026-05-18T04:36:33.817180+00:00","updated_at":"2026-05-18T04:36:33.817180+00:00"}