{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2026:RFW6AEEOIAC7ACDIUEU6GS6U6I","short_pith_number":"pith:RFW6AEEO","schema_version":"1.0","canonical_sha256":"896de0108e4005f00868a129e34bd4f212bb12dac5cdd7c380357796f14c4d0f","source":{"kind":"arxiv","id":"2602.20477","version":2},"attestation_state":"computed","paper":{"title":"Search for pair production of heavy resonances in final states with a photon and large-radius jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"CMS Collaboration","submitted_at":"2026-02-24T02:10:37Z","abstract_excerpt":"A search for the pair production of heavy spin-1/2 or spin-3/2 resonances (t$^*$) in proton-proton collisions at $\\sqrt{s}$ = 13 TeV is presented. Data collected with the CMS detector at the CERN LHC from 2016 to 2018 corresponding to an integrated luminosity of 138 fb$^{-1}$ are used. The analysis targets benchmark signal scenarios where one t$^*$ decays into a top quark (t) and a photon ($\\gamma$), and the other into a t quark and a gluon (g), i.e., pp $\\to$ t$^*\\bar{\\mathrm{t}}^*$ $\\to$ tt$\\gamma$g. All-hadronic final states from the t pair decay chain are selected using jet substructure te"},"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":"2602.20477","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ex","submitted_at":"2026-02-24T02:10:37Z","cross_cats_sorted":[],"title_canon_sha256":"e895363cba9f8c0c45f45e4567db2fc708fa44733a9c4376e0046af7b3999957","abstract_canon_sha256":"a77e767531473ae165bbcdcc4c84e39053d3ee3ed714f5ffefce4960e13adc43"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-06-19T16:11:21.114610Z","signature_b64":"skZ+alIXuvnYmQ0IFnwl8SXIc+aOUGL5vyQ44QZc4fGwN0ltU8fl+UYnM+Gv0GDQGiZZj6YdiTEK6HHygUKyBQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"896de0108e4005f00868a129e34bd4f212bb12dac5cdd7c380357796f14c4d0f","last_reissued_at":"2026-06-19T16:11:21.114136Z","signature_status":"signed_v1","first_computed_at":"2026-06-19T16:11:21.114136Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Search for pair production of heavy resonances in final states with a photon and large-radius jets in proton-proton collisions at $\\sqrt{s}$ = 13 TeV","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":[],"primary_cat":"hep-ex","authors_text":"CMS Collaboration","submitted_at":"2026-02-24T02:10:37Z","abstract_excerpt":"A search for the pair production of heavy spin-1/2 or spin-3/2 resonances (t$^*$) in proton-proton collisions at $\\sqrt{s}$ = 13 TeV is presented. Data collected with the CMS detector at the CERN LHC from 2016 to 2018 corresponding to an integrated luminosity of 138 fb$^{-1}$ are used. The analysis targets benchmark signal scenarios where one t$^*$ decays into a top quark (t) and a photon ($\\gamma$), and the other into a t quark and a gluon (g), i.e., pp $\\to$ t$^*\\bar{\\mathrm{t}}^*$ $\\to$ tt$\\gamma$g. All-hadronic final states from the t pair decay chain are selected using jet substructure te"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2602.20477","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/2602.20477/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":"2602.20477","created_at":"2026-06-19T16:11:21.114192+00:00"},{"alias_kind":"arxiv_version","alias_value":"2602.20477v2","created_at":"2026-06-19T16:11:21.114192+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2602.20477","created_at":"2026-06-19T16:11:21.114192+00:00"},{"alias_kind":"pith_short_12","alias_value":"RFW6AEEOIAC7","created_at":"2026-06-19T16:11:21.114192+00:00"},{"alias_kind":"pith_short_16","alias_value":"RFW6AEEOIAC7ACDI","created_at":"2026-06-19T16:11:21.114192+00:00"},{"alias_kind":"pith_short_8","alias_value":"RFW6AEEO","created_at":"2026-06-19T16:11:21.114192+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/RFW6AEEOIAC7ACDIUEU6GS6U6I","json":"https://pith.science/pith/RFW6AEEOIAC7ACDIUEU6GS6U6I.json","graph_json":"https://pith.science/api/pith-number/RFW6AEEOIAC7ACDIUEU6GS6U6I/graph.json","events_json":"https://pith.science/api/pith-number/RFW6AEEOIAC7ACDIUEU6GS6U6I/events.json","paper":"https://pith.science/paper/RFW6AEEO"},"agent_actions":{"view_html":"https://pith.science/pith/RFW6AEEOIAC7ACDIUEU6GS6U6I","download_json":"https://pith.science/pith/RFW6AEEOIAC7ACDIUEU6GS6U6I.json","view_paper":"https://pith.science/paper/RFW6AEEO","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2602.20477&json=true","fetch_graph":"https://pith.science/api/pith-number/RFW6AEEOIAC7ACDIUEU6GS6U6I/graph.json","fetch_events":"https://pith.science/api/pith-number/RFW6AEEOIAC7ACDIUEU6GS6U6I/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/RFW6AEEOIAC7ACDIUEU6GS6U6I/action/timestamp_anchor","attest_storage":"https://pith.science/pith/RFW6AEEOIAC7ACDIUEU6GS6U6I/action/storage_attestation","attest_author":"https://pith.science/pith/RFW6AEEOIAC7ACDIUEU6GS6U6I/action/author_attestation","sign_citation":"https://pith.science/pith/RFW6AEEOIAC7ACDIUEU6GS6U6I/action/citation_signature","submit_replication":"https://pith.science/pith/RFW6AEEOIAC7ACDIUEU6GS6U6I/action/replication_record"}},"created_at":"2026-06-19T16:11:21.114192+00:00","updated_at":"2026-06-19T16:11:21.114192+00:00"}