{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2022:64OEKGMPVCWYEHAXB6C7OD22KW","short_pith_number":"pith:64OEKGMP","schema_version":"1.0","canonical_sha256":"f71c45198fa8ad821c170f85f70f5a55bd3ef948b090293b3e6171229c960c16","source":{"kind":"arxiv","id":"2202.01789","version":2},"attestation_state":"computed","paper":{"title":"Unravelling the left-right mixing using $0\\nu \\beta\\beta$ decay and collider probes","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Gang Li, Juan Carlos Vasquez, Michael J. Ramsey-Musolf","submitted_at":"2022-02-03T19:00:01Z","abstract_excerpt":"In the context of the minimal left-right symmetric model, we study the interplay between current and future neutrinoless double beta ($0\\nu\\beta\\beta$) decay experiments, long-lived particle searches at the LHC main detectors ATLAS/CMS, and the proposed far detector MATHUSLA. The heavy Majorana neutrino can be produced in association with an electron from the decay of $W$ boson for a non-zero left-right mixing and subsequently decays into another electron with the same charge and jets. Owing to the suppression of large right-handed charged gauge boson $W_R$ mass, the heavy neutrinos could be l"},"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":"2202.01789","kind":"arxiv","version":2},"metadata":{"license":"http://creativecommons.org/licenses/by/4.0/","primary_cat":"hep-ph","submitted_at":"2022-02-03T19:00:01Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"7fefd7c53264c08661fe137f2ef5fab6cb8613daa4dfa186e45fa13db21fc0c3","abstract_canon_sha256":"cc6cab648f97029f708a74c980c313bd2757c06896a4725ded8f300f7f75a824"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T04:35:43.234428Z","signature_b64":"bIxSomqYP0rLS0GtMRzvBJOE6HniImaoY4CYe3+4oalt08IW1tWG7aPjfBIXQE+rIlxwh8CTJE0fBaY4H3E8Aw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"f71c45198fa8ad821c170f85f70f5a55bd3ef948b090293b3e6171229c960c16","last_reissued_at":"2026-07-05T04:35:43.233888Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T04:35:43.233888Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Unravelling the left-right mixing using $0\\nu \\beta\\beta$ decay and collider probes","license":"http://creativecommons.org/licenses/by/4.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Gang Li, Juan Carlos Vasquez, Michael J. Ramsey-Musolf","submitted_at":"2022-02-03T19:00:01Z","abstract_excerpt":"In the context of the minimal left-right symmetric model, we study the interplay between current and future neutrinoless double beta ($0\\nu\\beta\\beta$) decay experiments, long-lived particle searches at the LHC main detectors ATLAS/CMS, and the proposed far detector MATHUSLA. The heavy Majorana neutrino can be produced in association with an electron from the decay of $W$ boson for a non-zero left-right mixing and subsequently decays into another electron with the same charge and jets. Owing to the suppression of large right-handed charged gauge boson $W_R$ mass, the heavy neutrinos could be l"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2202.01789","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/2202.01789/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":"2202.01789","created_at":"2026-07-05T04:35:43.233945+00:00"},{"alias_kind":"arxiv_version","alias_value":"2202.01789v2","created_at":"2026-07-05T04:35:43.233945+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2202.01789","created_at":"2026-07-05T04:35:43.233945+00:00"},{"alias_kind":"pith_short_12","alias_value":"64OEKGMPVCWY","created_at":"2026-07-05T04:35:43.233945+00:00"},{"alias_kind":"pith_short_16","alias_value":"64OEKGMPVCWYEHAX","created_at":"2026-07-05T04:35:43.233945+00:00"},{"alias_kind":"pith_short_8","alias_value":"64OEKGMP","created_at":"2026-07-05T04:35:43.233945+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2504.12141","citing_title":"Heavy neutrino mixing prospects at hadron colliders: a machine learning study","ref_index":79,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/64OEKGMPVCWYEHAXB6C7OD22KW","json":"https://pith.science/pith/64OEKGMPVCWYEHAXB6C7OD22KW.json","graph_json":"https://pith.science/api/pith-number/64OEKGMPVCWYEHAXB6C7OD22KW/graph.json","events_json":"https://pith.science/api/pith-number/64OEKGMPVCWYEHAXB6C7OD22KW/events.json","paper":"https://pith.science/paper/64OEKGMP"},"agent_actions":{"view_html":"https://pith.science/pith/64OEKGMPVCWYEHAXB6C7OD22KW","download_json":"https://pith.science/pith/64OEKGMPVCWYEHAXB6C7OD22KW.json","view_paper":"https://pith.science/paper/64OEKGMP","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2202.01789&json=true","fetch_graph":"https://pith.science/api/pith-number/64OEKGMPVCWYEHAXB6C7OD22KW/graph.json","fetch_events":"https://pith.science/api/pith-number/64OEKGMPVCWYEHAXB6C7OD22KW/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/64OEKGMPVCWYEHAXB6C7OD22KW/action/timestamp_anchor","attest_storage":"https://pith.science/pith/64OEKGMPVCWYEHAXB6C7OD22KW/action/storage_attestation","attest_author":"https://pith.science/pith/64OEKGMPVCWYEHAXB6C7OD22KW/action/author_attestation","sign_citation":"https://pith.science/pith/64OEKGMPVCWYEHAXB6C7OD22KW/action/citation_signature","submit_replication":"https://pith.science/pith/64OEKGMPVCWYEHAXB6C7OD22KW/action/replication_record"}},"created_at":"2026-07-05T04:35:43.233945+00:00","updated_at":"2026-07-05T04:35:43.233945+00:00"}