{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2014:WMWZ5BUEYW3DZQUXKFVLJUYMAB","short_pith_number":"pith:WMWZ5BUE","schema_version":"1.0","canonical_sha256":"b32d9e8684c5b63cc297516ab4d30c004d43b8c679fb80060e2d4aaabb81a9c9","source":{"kind":"arxiv","id":"1408.0774","version":3},"attestation_state":"computed","paper":{"title":"The lowest limits on the doubly charged Higgs boson masses in the minimal left-right symmetric model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"G. Bambhaniya, J. Chakrabortty, J. Gluza, M. Kordiaczynska, T. Jelinski","submitted_at":"2014-08-04T19:13:05Z","abstract_excerpt":"The doubly charged Higgs bosons $H_{1,2}^{\\pm\\pm}$ would undoubtedly be clear messengers of the new physics. We discuss their mass spectrum and show how experimental data and relations between scalar masses put limits on it. In particular, both the masses of the particles $H_1^0$, $A_1^0$ that play a crucial role in FCNC effects and the masses of the additional gauge bosons $W_2$, $Z_2$ are notably important. For instance, if $M_{H_1^0,A_1^0}\\simeq 15$ TeV and $M_{W_2}\\simeq 3.76$ TeV then the lowest mass of $H_1^{\\pm\\pm}$ is 465 GeV. In contrast, due to the freedom in the parameter space of t"},"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":"1408.0774","kind":"arxiv","version":3},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2014-08-04T19:13:05Z","cross_cats_sorted":[],"title_canon_sha256":"879efad606599e646f0e06a784830682b160d1c74fd3b7260cbad3c38690ec97","abstract_canon_sha256":"1413eeacdcde9597aab2b830baa22a7888451b69216adb9a918c6535026c1c86"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:27:57.037832Z","signature_b64":"nUua3MpqmPuStOEKqVq2QX7uLi374x1l6pp+QYPSaJ02ZoMzwTDJlqxEmuLCcmsVN5XSkh4NYQfxWPWQ5p3yBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"b32d9e8684c5b63cc297516ab4d30c004d43b8c679fb80060e2d4aaabb81a9c9","last_reissued_at":"2026-05-18T02:27:57.037380Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:27:57.037380Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"The lowest limits on the doubly charged Higgs boson masses in the minimal left-right symmetric model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"G. Bambhaniya, J. Chakrabortty, J. Gluza, M. Kordiaczynska, T. Jelinski","submitted_at":"2014-08-04T19:13:05Z","abstract_excerpt":"The doubly charged Higgs bosons $H_{1,2}^{\\pm\\pm}$ would undoubtedly be clear messengers of the new physics. We discuss their mass spectrum and show how experimental data and relations between scalar masses put limits on it. In particular, both the masses of the particles $H_1^0$, $A_1^0$ that play a crucial role in FCNC effects and the masses of the additional gauge bosons $W_2$, $Z_2$ are notably important. For instance, if $M_{H_1^0,A_1^0}\\simeq 15$ TeV and $M_{W_2}\\simeq 3.76$ TeV then the lowest mass of $H_1^{\\pm\\pm}$ is 465 GeV. In contrast, due to the freedom in the parameter space of t"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1408.0774","kind":"arxiv","version":3},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"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":"1408.0774","created_at":"2026-05-18T02:27:57.037449+00:00"},{"alias_kind":"arxiv_version","alias_value":"1408.0774v3","created_at":"2026-05-18T02:27:57.037449+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1408.0774","created_at":"2026-05-18T02:27:57.037449+00:00"},{"alias_kind":"pith_short_12","alias_value":"WMWZ5BUEYW3D","created_at":"2026-05-18T12:28:54.890064+00:00"},{"alias_kind":"pith_short_16","alias_value":"WMWZ5BUEYW3DZQUX","created_at":"2026-05-18T12:28:54.890064+00:00"},{"alias_kind":"pith_short_8","alias_value":"WMWZ5BUE","created_at":"2026-05-18T12:28:54.890064+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/WMWZ5BUEYW3DZQUXKFVLJUYMAB","json":"https://pith.science/pith/WMWZ5BUEYW3DZQUXKFVLJUYMAB.json","graph_json":"https://pith.science/api/pith-number/WMWZ5BUEYW3DZQUXKFVLJUYMAB/graph.json","events_json":"https://pith.science/api/pith-number/WMWZ5BUEYW3DZQUXKFVLJUYMAB/events.json","paper":"https://pith.science/paper/WMWZ5BUE"},"agent_actions":{"view_html":"https://pith.science/pith/WMWZ5BUEYW3DZQUXKFVLJUYMAB","download_json":"https://pith.science/pith/WMWZ5BUEYW3DZQUXKFVLJUYMAB.json","view_paper":"https://pith.science/paper/WMWZ5BUE","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1408.0774&json=true","fetch_graph":"https://pith.science/api/pith-number/WMWZ5BUEYW3DZQUXKFVLJUYMAB/graph.json","fetch_events":"https://pith.science/api/pith-number/WMWZ5BUEYW3DZQUXKFVLJUYMAB/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/WMWZ5BUEYW3DZQUXKFVLJUYMAB/action/timestamp_anchor","attest_storage":"https://pith.science/pith/WMWZ5BUEYW3DZQUXKFVLJUYMAB/action/storage_attestation","attest_author":"https://pith.science/pith/WMWZ5BUEYW3DZQUXKFVLJUYMAB/action/author_attestation","sign_citation":"https://pith.science/pith/WMWZ5BUEYW3DZQUXKFVLJUYMAB/action/citation_signature","submit_replication":"https://pith.science/pith/WMWZ5BUEYW3DZQUXKFVLJUYMAB/action/replication_record"}},"created_at":"2026-05-18T02:27:57.037449+00:00","updated_at":"2026-05-18T02:27:57.037449+00:00"}