{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:1997:3LV2O46SDCJNEA4Z44WXTGG2TY","short_pith_number":"pith:3LV2O46S","schema_version":"1.0","canonical_sha256":"daeba773d21892d20399e72d7998da9e3522e714248a1ca959aceec0757689c9","source":{"kind":"arxiv","id":"hep-ph/9710552","version":1},"attestation_state":"computed","paper":{"title":"Hybrid $SU(2)\\times U(1)$ models, electric charge nonconservation and the photon mass","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"A.Yu.Ignatiev, G.C.Joshi","submitted_at":"1997-10-31T02:47:26Z","abstract_excerpt":"Hybrid $SU(2) \\times U(1)$ models are the models in which $SU(2) \\times U(1)$ symmetry is broken down not only spontaneously (as in the Standard Model), but also explicitely by adding a hard mass term for the U(1) field in the lagrangian. We study the issue of electric charge nonconservation and dequantization in these models. For this purpose we construct and analyze a series of hybrid models with different scalar contents. We show that some of these models posess an interesting property: the photon can remain massless (at least, at the tree level) even though the electric charge is not conse"},"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":"hep-ph/9710552","kind":"arxiv","version":1},"metadata":{"license":"","primary_cat":"hep-ph","submitted_at":"1997-10-31T02:47:26Z","cross_cats_sorted":[],"title_canon_sha256":"842171886706b947d7cd1a62f0e91b6d6c95066ad54b2eb9a83ad9f05828e577","abstract_canon_sha256":"f5f5962cc3d2702c607f7e07b0deaff1808dc93be522676b6dad9028d6303c8d"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-07-04T14:48:56.891661Z","signature_b64":"4kv6J+nSK5SjhjgCeXVC9vDvgLjf8/yKaa6A1l3BlOMp2O9bkKwScVIgmN7rzj2cllUrGGBlEMJB2B2UtARmDQ==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"daeba773d21892d20399e72d7998da9e3522e714248a1ca959aceec0757689c9","last_reissued_at":"2026-07-04T14:48:56.891244Z","signature_status":"signed_v1","first_computed_at":"2026-07-04T14:48:56.891244Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Hybrid $SU(2)\\times U(1)$ models, electric charge nonconservation and the photon mass","license":"","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"A.Yu.Ignatiev, G.C.Joshi","submitted_at":"1997-10-31T02:47:26Z","abstract_excerpt":"Hybrid $SU(2) \\times U(1)$ models are the models in which $SU(2) \\times U(1)$ symmetry is broken down not only spontaneously (as in the Standard Model), but also explicitely by adding a hard mass term for the U(1) field in the lagrangian. We study the issue of electric charge nonconservation and dequantization in these models. For this purpose we construct and analyze a series of hybrid models with different scalar contents. We show that some of these models posess an interesting property: the photon can remain massless (at least, at the tree level) even though the electric charge is not conse"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"hep-ph/9710552","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/hep-ph/9710552/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":"hep-ph/9710552","created_at":"2026-07-04T14:48:56.891322+00:00"},{"alias_kind":"arxiv_version","alias_value":"hep-ph/9710552v1","created_at":"2026-07-04T14:48:56.891322+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.hep-ph/9710552","created_at":"2026-07-04T14:48:56.891322+00:00"},{"alias_kind":"pith_short_12","alias_value":"3LV2O46SDCJN","created_at":"2026-07-04T14:48:56.891322+00:00"},{"alias_kind":"pith_short_16","alias_value":"3LV2O46SDCJNEA4Z","created_at":"2026-07-04T14:48:56.891322+00:00"},{"alias_kind":"pith_short_8","alias_value":"3LV2O46S","created_at":"2026-07-04T14:48:56.891322+00:00"}],"events":[],"event_summary":{},"paper_claims":[],"inbound_citations":{"count":1,"internal_anchor_count":1,"sample":[{"citing_arxiv_id":"2504.20044","citing_title":"How Charged Can Neutrinos Be?","ref_index":87,"is_internal_anchor":true}]},"formal_canon":{"evidence_count":0,"sample":[],"anchors":[]},"links":{"html":"https://pith.science/pith/3LV2O46SDCJNEA4Z44WXTGG2TY","json":"https://pith.science/pith/3LV2O46SDCJNEA4Z44WXTGG2TY.json","graph_json":"https://pith.science/api/pith-number/3LV2O46SDCJNEA4Z44WXTGG2TY/graph.json","events_json":"https://pith.science/api/pith-number/3LV2O46SDCJNEA4Z44WXTGG2TY/events.json","paper":"https://pith.science/paper/3LV2O46S"},"agent_actions":{"view_html":"https://pith.science/pith/3LV2O46SDCJNEA4Z44WXTGG2TY","download_json":"https://pith.science/pith/3LV2O46SDCJNEA4Z44WXTGG2TY.json","view_paper":"https://pith.science/paper/3LV2O46S","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=hep-ph/9710552&json=true","fetch_graph":"https://pith.science/api/pith-number/3LV2O46SDCJNEA4Z44WXTGG2TY/graph.json","fetch_events":"https://pith.science/api/pith-number/3LV2O46SDCJNEA4Z44WXTGG2TY/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/3LV2O46SDCJNEA4Z44WXTGG2TY/action/timestamp_anchor","attest_storage":"https://pith.science/pith/3LV2O46SDCJNEA4Z44WXTGG2TY/action/storage_attestation","attest_author":"https://pith.science/pith/3LV2O46SDCJNEA4Z44WXTGG2TY/action/author_attestation","sign_citation":"https://pith.science/pith/3LV2O46SDCJNEA4Z44WXTGG2TY/action/citation_signature","submit_replication":"https://pith.science/pith/3LV2O46SDCJNEA4Z44WXTGG2TY/action/replication_record"}},"created_at":"2026-07-04T14:48:56.891322+00:00","updated_at":"2026-07-04T14:48:56.891322+00:00"}