{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2021:5SC7OIG5SHFEOWJT5LUA4QB2TF","short_pith_number":"pith:5SC7OIG5","schema_version":"1.0","canonical_sha256":"ec85f720dd91ca475933eae80e403a997f441520f5dbe6508c504f6de26af65d","source":{"kind":"arxiv","id":"2109.09585","version":2},"attestation_state":"computed","paper":{"title":"Testing left-right symmetry with an inverse seesaw mechanism at the LHC","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Adithya Sampath, Ananya Mukherjee, Lakshmi Priya, Mathew Thomas Arun, Subhadip Mitra, Tanumoy Mandal","submitted_at":"2021-09-20T14:41:04Z","abstract_excerpt":"In the left-right symmetric models, a heavy charged gauge boson $W'$ can decay to a lepton and a right-handed neutrino (RHN). If the neutrino masses are generated through the standard type-I seesaw mechanism, the Yukawa couplings controlling two-body decays of the RHN become very small. As a result, the RHN decays to another lepton and a pair of jets via an off-shell $W'$. This is the basis of the Keung-Senjanovi\\'{c} (KS) process, which was originally proposed as a probe of lepton number violation at the LHC. However, if a different mechanism like the inverse seesaw generates the neutrino mas"},"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":"2109.09585","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2021-09-20T14:41:04Z","cross_cats_sorted":["hep-ex"],"title_canon_sha256":"63ab168a1fcccd5c5e663590599ddb493131f890d4d2c5d77a1939a598483eb8","abstract_canon_sha256":"d299904c5e6de9063fa1d1e3aac4b9722bc1f85169f9eb1b80fda098ec39d656"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-05T04:42:14.485306Z","signature_b64":"RORl4U7mgFZ7vLBvWOlh5E/3d2hRQELjV+0P6pyP831wF/q7r1Ftlf7EO0OvWhiYsn5qjD/+tskBGU9HGsyWDA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"ec85f720dd91ca475933eae80e403a997f441520f5dbe6508c504f6de26af65d","last_reissued_at":"2026-07-05T04:42:14.484934Z","signature_status":"signed_v1","first_computed_at":"2026-07-05T04:42:14.484934Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Testing left-right symmetry with an inverse seesaw mechanism at the LHC","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["hep-ex"],"primary_cat":"hep-ph","authors_text":"Adithya Sampath, Ananya Mukherjee, Lakshmi Priya, Mathew Thomas Arun, Subhadip Mitra, Tanumoy Mandal","submitted_at":"2021-09-20T14:41:04Z","abstract_excerpt":"In the left-right symmetric models, a heavy charged gauge boson $W'$ can decay to a lepton and a right-handed neutrino (RHN). If the neutrino masses are generated through the standard type-I seesaw mechanism, the Yukawa couplings controlling two-body decays of the RHN become very small. As a result, the RHN decays to another lepton and a pair of jets via an off-shell $W'$. This is the basis of the Keung-Senjanovi\\'{c} (KS) process, which was originally proposed as a probe of lepton number violation at the LHC. However, if a different mechanism like the inverse seesaw generates the neutrino mas"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"2109.09585","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/2109.09585/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":"2109.09585","created_at":"2026-07-05T04:42:14.484990+00:00"},{"alias_kind":"arxiv_version","alias_value":"2109.09585v2","created_at":"2026-07-05T04:42:14.484990+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.2109.09585","created_at":"2026-07-05T04:42:14.484990+00:00"},{"alias_kind":"pith_short_12","alias_value":"5SC7OIG5SHFE","created_at":"2026-07-05T04:42:14.484990+00:00"},{"alias_kind":"pith_short_16","alias_value":"5SC7OIG5SHFEOWJT","created_at":"2026-07-05T04:42:14.484990+00:00"},{"alias_kind":"pith_short_8","alias_value":"5SC7OIG5","created_at":"2026-07-05T04:42:14.484990+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2412.19751","citing_title":"Right-handed neutrino production through first-generation leptoquarks","ref_index":9,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/5SC7OIG5SHFEOWJT5LUA4QB2TF","json":"https://pith.science/pith/5SC7OIG5SHFEOWJT5LUA4QB2TF.json","graph_json":"https://pith.science/api/pith-number/5SC7OIG5SHFEOWJT5LUA4QB2TF/graph.json","events_json":"https://pith.science/api/pith-number/5SC7OIG5SHFEOWJT5LUA4QB2TF/events.json","paper":"https://pith.science/paper/5SC7OIG5"},"agent_actions":{"view_html":"https://pith.science/pith/5SC7OIG5SHFEOWJT5LUA4QB2TF","download_json":"https://pith.science/pith/5SC7OIG5SHFEOWJT5LUA4QB2TF.json","view_paper":"https://pith.science/paper/5SC7OIG5","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=2109.09585&json=true","fetch_graph":"https://pith.science/api/pith-number/5SC7OIG5SHFEOWJT5LUA4QB2TF/graph.json","fetch_events":"https://pith.science/api/pith-number/5SC7OIG5SHFEOWJT5LUA4QB2TF/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/5SC7OIG5SHFEOWJT5LUA4QB2TF/action/timestamp_anchor","attest_storage":"https://pith.science/pith/5SC7OIG5SHFEOWJT5LUA4QB2TF/action/storage_attestation","attest_author":"https://pith.science/pith/5SC7OIG5SHFEOWJT5LUA4QB2TF/action/author_attestation","sign_citation":"https://pith.science/pith/5SC7OIG5SHFEOWJT5LUA4QB2TF/action/citation_signature","submit_replication":"https://pith.science/pith/5SC7OIG5SHFEOWJT5LUA4QB2TF/action/replication_record"}},"created_at":"2026-07-05T04:42:14.484990+00:00","updated_at":"2026-07-05T04:42:14.484990+00:00"}