{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2022:JZ6VBFOCPUJD3CGLYYJMT7H54B","short_pith_number":"pith:JZ6VBFOC","schema_version":"1.0","canonical_sha256":"4e7d5095c27d123d88cbc612c9fcfde0785c6216e9fcd383f508023ffdba744e","source":{"kind":"arxiv","id":"2210.15813","version":1},"attestation_state":"computed","paper":{"title":"Probing a $\\mathrm{Z}^{\\prime}$ with non-universal fermion couplings through top quark fusion, decays to bottom quarks, and machine learning techniques","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Alfredo Gurrola, Andr\\'es Fl\\'orez, Diego Barbosa, Elijah Sheridan, Felipe D\\'iaz, Francesco Romeo, Liliana Quintero, Manuel Sanchez","submitted_at":"2022-10-28T00:32:51Z","abstract_excerpt":"The production of heavy mass resonances has been widely studied theoretically and experimentally. Several extensions of the standard model (SM) of particle physics, naturally give rise to a new resonance, with neutral electric charge, commonly referred to as the $\\textrm{Z}^{\\prime}$ boson. The nature, mass, couplings, and associated quantum numbers of this hypothetical particle are yet to be determined. We present a feasibility study on the production of a vector like $\\textrm{Z}^{\\prime}$ boson at the LHC, with preferential couplings to third generation fermions, considering proton-proton co"},"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":"2210.15813","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2022-10-28T00:32:51Z","cross_cats_sorted":[],"title_canon_sha256":"f647f58a4c9a507050e9473f72827034f001dcd201b6d90f68b9d8ee42694764","abstract_canon_sha256":"ccacf0088a672e016c14f554b00b8ea7bcbaaadbaf516fd165a94a173c3f5b71"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T06:15:17.318123Z","signature_b64":"u53K4hAbJqFg8I2SPTtWY7ntDGAzinkS4f3eA5OGSicobGyMDn1UpLwKzDuf1n098QZm3TEDzHH1M/9Se9C/CQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"4e7d5095c27d123d88cbc612c9fcfde0785c6216e9fcd383f508023ffdba744e","last_reissued_at":"2026-07-05T06:15:17.317658Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T06:15:17.317658Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Probing a $\\mathrm{Z}^{\\prime}$ with non-universal fermion couplings through top quark fusion, decays to bottom quarks, and machine learning techniques","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Alfredo Gurrola, Andr\\'es Fl\\'orez, Diego Barbosa, Elijah Sheridan, Felipe D\\'iaz, Francesco Romeo, Liliana Quintero, Manuel Sanchez","submitted_at":"2022-10-28T00:32:51Z","abstract_excerpt":"The production of heavy mass resonances has been widely studied theoretically and experimentally. Several extensions of the standard model (SM) of particle physics, naturally give rise to a new resonance, with neutral electric charge, commonly referred to as the $\\textrm{Z}^{\\prime}$ boson. The nature, mass, couplings, and associated quantum numbers of this hypothetical particle are yet to be determined. We present a feasibility study on the production of a vector like $\\textrm{Z}^{\\prime}$ boson at the LHC, with preferential couplings to third generation fermions, considering proton-proton co"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2210.15813","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":""},"integrity":{"clean":true,"summary":{"advisory":0,"critical":0,"by_detector":{},"informational":0},"endpoint":"/pith/2210.15813/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":"2210.15813","created_at":"2026-07-05T06:15:17.317731+00:00"},{"alias_kind":"arxiv_version","alias_value":"2210.15813v1","created_at":"2026-07-05T06:15:17.317731+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2210.15813","created_at":"2026-07-05T06:15:17.317731+00:00"},{"alias_kind":"pith_short_12","alias_value":"JZ6VBFOCPUJD","created_at":"2026-07-05T06:15:17.317731+00:00"},{"alias_kind":"pith_short_16","alias_value":"JZ6VBFOCPUJD3CGL","created_at":"2026-07-05T06:15:17.317731+00:00"},{"alias_kind":"pith_short_8","alias_value":"JZ6VBFOC","created_at":"2026-07-05T06:15:17.317731+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":0,"sample":[{"citing_arxiv_id":"2606.27441","citing_title":"Collider Probes of Dark Energy Microphysics","ref_index":64,"is_internal_anchor":false}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/JZ6VBFOCPUJD3CGLYYJMT7H54B","json":"https://pith.science/pith/JZ6VBFOCPUJD3CGLYYJMT7H54B.json","graph_json":"https://pith.science/api/pith-number/JZ6VBFOCPUJD3CGLYYJMT7H54B/graph.json","events_json":"https://pith.science/api/pith-number/JZ6VBFOCPUJD3CGLYYJMT7H54B/events.json","paper":"https://pith.science/paper/JZ6VBFOC"},"agent_actions":{"view_html":"https://pith.science/pith/JZ6VBFOCPUJD3CGLYYJMT7H54B","download_json":"https://pith.science/pith/JZ6VBFOCPUJD3CGLYYJMT7H54B.json","view_paper":"https://pith.science/paper/JZ6VBFOC","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2210.15813&json=true","fetch_graph":"https://pith.science/api/pith-number/JZ6VBFOCPUJD3CGLYYJMT7H54B/graph.json","fetch_events":"https://pith.science/api/pith-number/JZ6VBFOCPUJD3CGLYYJMT7H54B/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/JZ6VBFOCPUJD3CGLYYJMT7H54B/action/timestamp_anchor","attest_storage":"https://pith.science/pith/JZ6VBFOCPUJD3CGLYYJMT7H54B/action/storage_attestation","attest_author":"https://pith.science/pith/JZ6VBFOCPUJD3CGLYYJMT7H54B/action/author_attestation","sign_citation":"https://pith.science/pith/JZ6VBFOCPUJD3CGLYYJMT7H54B/action/citation_signature","submit_replication":"https://pith.science/pith/JZ6VBFOCPUJD3CGLYYJMT7H54B/action/replication_record"}},"created_at":"2026-07-05T06:15:17.317731+00:00","updated_at":"2026-07-05T06:15:17.317731+00:00"}