{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2022:2IFCVG6TC47MRKXO77XJMNMZHP","short_pith_number":"pith:2IFCVG6T","schema_version":"1.0","canonical_sha256":"d20a2a9bd3173ec8aaeeffee9635993bef9460f3336fe43b21d6bc918e4d500a","source":{"kind":"arxiv","id":"2202.07288","version":2},"attestation_state":"computed","paper":{"title":"Search for resonant pair production of Higgs bosons in the $b\\bar{b}b\\bar{b}$ final state using $pp$ collisions at $\\sqrt{s}$ = 13 TeV with the ATLAS detector","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"ATLAS Collaboration","submitted_at":"2022-02-15T10:09:13Z","abstract_excerpt":"A search for resonant Higgs boson pair production in the $b\\bar{b}b\\bar{b}$ final state is presented. The analysis uses 126-139 fb$^{-1}$ of $pp$ collision data at $\\sqrt{s}$ = 13 TeV collected with the ATLAS detector at the Large Hadron Collider. The analysis is divided into two channels, targeting Higgs boson decays which are reconstructed as pairs of small-radius jets or as individual large-radius jets. Spin-0 and spin-2 benchmark signal models are considered, both of which correspond to resonant $HH$ production via gluon$-$gluon fusion. The data are consistent with Standard Model predictio"},"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":"2202.07288","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ex","submitted_at":"2022-02-15T10:09:13Z","cross_cats_sorted":[],"title_canon_sha256":"a02f930f4f013dcbd0903b0d5d3a45440becf4b9640b50931ec14eb7d9807bca","abstract_canon_sha256":"56528e79d46cec3c46e92a16e611e5a000046154f224b7cd9e21ecda3d1776c4"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T04:33:30.636173Z","signature_b64":"JAqFRAgtiqkYxNH/pF0w5awn4aPmIFzoqfyujFeL48GAykEDT7WTimZfABJG0/+gNV2aRzZBbKmOvTLMZquOAQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"d20a2a9bd3173ec8aaeeffee9635993bef9460f3336fe43b21d6bc918e4d500a","last_reissued_at":"2026-07-05T04:33:30.635638Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T04:33:30.635638Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Search for resonant pair production of Higgs bosons in the $b\\bar{b}b\\bar{b}$ final state using $pp$ collisions at $\\sqrt{s}$ = 13 TeV with the ATLAS detector","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"ATLAS Collaboration","submitted_at":"2022-02-15T10:09:13Z","abstract_excerpt":"A search for resonant Higgs boson pair production in the $b\\bar{b}b\\bar{b}$ final state is presented. The analysis uses 126-139 fb$^{-1}$ of $pp$ collision data at $\\sqrt{s}$ = 13 TeV collected with the ATLAS detector at the Large Hadron Collider. The analysis is divided into two channels, targeting Higgs boson decays which are reconstructed as pairs of small-radius jets or as individual large-radius jets. Spin-0 and spin-2 benchmark signal models are considered, both of which correspond to resonant $HH$ production via gluon$-$gluon fusion. The data are consistent with Standard Model predictio"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2202.07288","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/2202.07288/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":"2202.07288","created_at":"2026-07-05T04:33:30.635712+00:00"},{"alias_kind":"arxiv_version","alias_value":"2202.07288v2","created_at":"2026-07-05T04:33:30.635712+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2202.07288","created_at":"2026-07-05T04:33:30.635712+00:00"},{"alias_kind":"pith_short_12","alias_value":"2IFCVG6TC47M","created_at":"2026-07-05T04:33:30.635712+00:00"},{"alias_kind":"pith_short_16","alias_value":"2IFCVG6TC47MRKXO","created_at":"2026-07-05T04:33:30.635712+00:00"},{"alias_kind":"pith_short_8","alias_value":"2IFCVG6T","created_at":"2026-07-05T04:33:30.635712+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2605.29345","citing_title":"Alignment and Enhanced Multi-Higgs Production","ref_index":27,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/2IFCVG6TC47MRKXO77XJMNMZHP","json":"https://pith.science/pith/2IFCVG6TC47MRKXO77XJMNMZHP.json","graph_json":"https://pith.science/api/pith-number/2IFCVG6TC47MRKXO77XJMNMZHP/graph.json","events_json":"https://pith.science/api/pith-number/2IFCVG6TC47MRKXO77XJMNMZHP/events.json","paper":"https://pith.science/paper/2IFCVG6T"},"agent_actions":{"view_html":"https://pith.science/pith/2IFCVG6TC47MRKXO77XJMNMZHP","download_json":"https://pith.science/pith/2IFCVG6TC47MRKXO77XJMNMZHP.json","view_paper":"https://pith.science/paper/2IFCVG6T","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2202.07288&json=true","fetch_graph":"https://pith.science/api/pith-number/2IFCVG6TC47MRKXO77XJMNMZHP/graph.json","fetch_events":"https://pith.science/api/pith-number/2IFCVG6TC47MRKXO77XJMNMZHP/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/2IFCVG6TC47MRKXO77XJMNMZHP/action/timestamp_anchor","attest_storage":"https://pith.science/pith/2IFCVG6TC47MRKXO77XJMNMZHP/action/storage_attestation","attest_author":"https://pith.science/pith/2IFCVG6TC47MRKXO77XJMNMZHP/action/author_attestation","sign_citation":"https://pith.science/pith/2IFCVG6TC47MRKXO77XJMNMZHP/action/citation_signature","submit_replication":"https://pith.science/pith/2IFCVG6TC47MRKXO77XJMNMZHP/action/replication_record"}},"created_at":"2026-07-05T04:33:30.635712+00:00","updated_at":"2026-07-05T04:33:30.635712+00:00"}