{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2015:VICWCZXVOVY3B2UKRCVIUDEV5T","short_pith_number":"pith:VICWCZXV","schema_version":"1.0","canonical_sha256":"aa056166f57571b0ea8a88aa8a0c95ece5bacfa750633695726467feb42184da","source":{"kind":"arxiv","id":"1502.00919","version":2},"attestation_state":"computed","paper":{"title":"Low-energy phenomenology of trinification: an effective left-right-symmetric model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Berthold Stech, Jamil Hetzel","submitted_at":"2015-02-03T16:38:36Z","abstract_excerpt":"The trinification model is an interesting extension of the Standard Model (SM) based on the gauge group $SU(3)_C\\times SU(3)_L\\times SU(3)_R$. We study its low-energy phenomenology by constructing a low-energy effective field theory, thereby reducing the number of particles and free parameters that need to be studied. The resulting model predicts that several new scalar particles have masses in the $\\mathcal{O}\\left(100\\text{ GeV}\\right)$ range. We study a few of the interesting phenomenological scenarios, such as the presence of a light fermiophobic scalar in addition to a SM-like Higgs, or a"},"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":"1502.00919","kind":"arxiv","version":2},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2015-02-03T16:38:36Z","cross_cats_sorted":[],"title_canon_sha256":"7e3013c44ccaab9539fb6c753c4117f3d5db809536375582fd497f860eab1b0f","abstract_canon_sha256":"52b688e12b01f2637547624994876a4731820b2ea8234ecb1b33d5cde1ffb45b"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T02:17:51.281021Z","signature_b64":"zqrHuE6e7A7IjfvG96E+esNeeSgGVXbth/Lp9gFnXPsT9GVH8lD4+62pWLqmJ6t4TqOM33wIzKW3dWLON5yBBA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"aa056166f57571b0ea8a88aa8a0c95ece5bacfa750633695726467feb42184da","last_reissued_at":"2026-05-18T02:17:51.280425Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T02:17:51.280425Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Low-energy phenomenology of trinification: an effective left-right-symmetric model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Berthold Stech, Jamil Hetzel","submitted_at":"2015-02-03T16:38:36Z","abstract_excerpt":"The trinification model is an interesting extension of the Standard Model (SM) based on the gauge group $SU(3)_C\\times SU(3)_L\\times SU(3)_R$. We study its low-energy phenomenology by constructing a low-energy effective field theory, thereby reducing the number of particles and free parameters that need to be studied. The resulting model predicts that several new scalar particles have masses in the $\\mathcal{O}\\left(100\\text{ GeV}\\right)$ range. We study a few of the interesting phenomenological scenarios, such as the presence of a light fermiophobic scalar in addition to a SM-like Higgs, or a"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1502.00919","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":""},"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":"1502.00919","created_at":"2026-05-18T02:17:51.280505+00:00"},{"alias_kind":"arxiv_version","alias_value":"1502.00919v2","created_at":"2026-05-18T02:17:51.280505+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1502.00919","created_at":"2026-05-18T02:17:51.280505+00:00"},{"alias_kind":"pith_short_12","alias_value":"VICWCZXVOVY3","created_at":"2026-05-18T12:29:44.643036+00:00"},{"alias_kind":"pith_short_16","alias_value":"VICWCZXVOVY3B2UK","created_at":"2026-05-18T12:29:44.643036+00:00"},{"alias_kind":"pith_short_8","alias_value":"VICWCZXV","created_at":"2026-05-18T12:29:44.643036+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2507.01777","citing_title":"Charge quantisation, monopoles and emergent symmetry in the Standard Model and its embeddings","ref_index":35,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/VICWCZXVOVY3B2UKRCVIUDEV5T","json":"https://pith.science/pith/VICWCZXVOVY3B2UKRCVIUDEV5T.json","graph_json":"https://pith.science/api/pith-number/VICWCZXVOVY3B2UKRCVIUDEV5T/graph.json","events_json":"https://pith.science/api/pith-number/VICWCZXVOVY3B2UKRCVIUDEV5T/events.json","paper":"https://pith.science/paper/VICWCZXV"},"agent_actions":{"view_html":"https://pith.science/pith/VICWCZXVOVY3B2UKRCVIUDEV5T","download_json":"https://pith.science/pith/VICWCZXVOVY3B2UKRCVIUDEV5T.json","view_paper":"https://pith.science/paper/VICWCZXV","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1502.00919&json=true","fetch_graph":"https://pith.science/api/pith-number/VICWCZXVOVY3B2UKRCVIUDEV5T/graph.json","fetch_events":"https://pith.science/api/pith-number/VICWCZXVOVY3B2UKRCVIUDEV5T/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/VICWCZXVOVY3B2UKRCVIUDEV5T/action/timestamp_anchor","attest_storage":"https://pith.science/pith/VICWCZXVOVY3B2UKRCVIUDEV5T/action/storage_attestation","attest_author":"https://pith.science/pith/VICWCZXVOVY3B2UKRCVIUDEV5T/action/author_attestation","sign_citation":"https://pith.science/pith/VICWCZXVOVY3B2UKRCVIUDEV5T/action/citation_signature","submit_replication":"https://pith.science/pith/VICWCZXVOVY3B2UKRCVIUDEV5T/action/replication_record"}},"created_at":"2026-05-18T02:17:51.280505+00:00","updated_at":"2026-05-18T02:17:51.280505+00:00"}