{"record_type":"pith_number_record","schema_url":"https://pith.science/schemas/pith-number/v1.json","pith_number":"pith:2019:BJOENFKKJHMEHR4TKO3FTK64BV","short_pith_number":"pith:BJOENFKK","schema_version":"1.0","canonical_sha256":"0a5c46954a49d843c79353b659abdc0d6c9a36009507f4104ae62db13a52a643","source":{"kind":"arxiv","id":"1905.05600","version":1},"attestation_state":"computed","paper":{"title":"Electro-weak Phase Transition With Three Phases in The $SU(2)_1 \\otimes SU(2)_2 \\otimes U(1)_Y$ Model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Nguyen Minh Anh, Vo Quoc Phong","submitted_at":"2019-05-14T13:40:28Z","abstract_excerpt":"Our analysis shows that SM-like electroweak phase transition (EWPT) in the $SU(2)_1 \\otimes SU(2)_2 \\otimes U(1)_Y$ (2-2-1) model is a first-order phase transition at the $200$ GeV scale (the SM scale). Its strength ($S$) is about $1 - 2.7$ and the masses of new gauge bosons are larger than $1.7$ TeV when the second VEV is larger than $535$ GeV in a three-stage EWPT scenario and the coupling constant of $SU(2)_2$ group must be larger than 2. Therefore, this first order EWPT can be used to fix VEVs and the coupling constant of the gauge group in electro-weak models."},"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":"1905.05600","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"hep-ph","submitted_at":"2019-05-14T13:40:28Z","cross_cats_sorted":[],"title_canon_sha256":"1228ed8a93d985877caa8adcb82ff456a0e3e64aedfd8d091de8ae6deb3474fb","abstract_canon_sha256":"9da47de50d542409d241c85f91800c5d95de34e72f4f3e78eb002db07cf120a1"},"schema_version":"1.0"},"receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-17T23:46:14.114038Z","signature_b64":"yeFw46IY0gjJN9bf14Ed7FW7teqo8gcEGceYCkAH9IAcHtDUQwnJlRPA3NyICQIhMMqE3/0DfRQupzrkC3s2AA==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"0a5c46954a49d843c79353b659abdc0d6c9a36009507f4104ae62db13a52a643","last_reissued_at":"2026-05-17T23:46:14.113393Z","signature_status":"signed_v1","first_computed_at":"2026-05-17T23:46:14.113393Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"graph_snapshot":{"paper":{"title":"Electro-weak Phase Transition With Three Phases in The $SU(2)_1 \\otimes SU(2)_2 \\otimes U(1)_Y$ Model","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":[],"primary_cat":"hep-ph","authors_text":"Nguyen Minh Anh, Vo Quoc Phong","submitted_at":"2019-05-14T13:40:28Z","abstract_excerpt":"Our analysis shows that SM-like electroweak phase transition (EWPT) in the $SU(2)_1 \\otimes SU(2)_2 \\otimes U(1)_Y$ (2-2-1) model is a first-order phase transition at the $200$ GeV scale (the SM scale). Its strength ($S$) is about $1 - 2.7$ and the masses of new gauge bosons are larger than $1.7$ TeV when the second VEV is larger than $535$ GeV in a three-stage EWPT scenario and the coupling constant of $SU(2)_2$ group must be larger than 2. Therefore, this first order EWPT can be used to fix VEVs and the coupling constant of the gauge group in electro-weak models."},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1905.05600","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":""},"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":"1905.05600","created_at":"2026-05-17T23:46:14.113495+00:00"},{"alias_kind":"arxiv_version","alias_value":"1905.05600v1","created_at":"2026-05-17T23:46:14.113495+00:00"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1905.05600","created_at":"2026-05-17T23:46:14.113495+00:00"},{"alias_kind":"pith_short_12","alias_value":"BJOENFKKJHME","created_at":"2026-05-18T12:33:12.712433+00:00"},{"alias_kind":"pith_short_16","alias_value":"BJOENFKKJHMEHR4T","created_at":"2026-05-18T12:33:12.712433+00:00"},{"alias_kind":"pith_short_8","alias_value":"BJOENFKK","created_at":"2026-05-18T12:33:12.712433+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/BJOENFKKJHMEHR4TKO3FTK64BV","json":"https://pith.science/pith/BJOENFKKJHMEHR4TKO3FTK64BV.json","graph_json":"https://pith.science/api/pith-number/BJOENFKKJHMEHR4TKO3FTK64BV/graph.json","events_json":"https://pith.science/api/pith-number/BJOENFKKJHMEHR4TKO3FTK64BV/events.json","paper":"https://pith.science/paper/BJOENFKK"},"agent_actions":{"view_html":"https://pith.science/pith/BJOENFKKJHMEHR4TKO3FTK64BV","download_json":"https://pith.science/pith/BJOENFKKJHMEHR4TKO3FTK64BV.json","view_paper":"https://pith.science/paper/BJOENFKK","resolve_alias":"https://pith.science/api/pith-number/resolve?arxiv=1905.05600&json=true","fetch_graph":"https://pith.science/api/pith-number/BJOENFKKJHMEHR4TKO3FTK64BV/graph.json","fetch_events":"https://pith.science/api/pith-number/BJOENFKKJHMEHR4TKO3FTK64BV/events.json","actions":{"anchor_timestamp":"https://pith.science/pith/BJOENFKKJHMEHR4TKO3FTK64BV/action/timestamp_anchor","attest_storage":"https://pith.science/pith/BJOENFKKJHMEHR4TKO3FTK64BV/action/storage_attestation","attest_author":"https://pith.science/pith/BJOENFKKJHMEHR4TKO3FTK64BV/action/author_attestation","sign_citation":"https://pith.science/pith/BJOENFKKJHMEHR4TKO3FTK64BV/action/citation_signature","submit_replication":"https://pith.science/pith/BJOENFKKJHMEHR4TKO3FTK64BV/action/replication_record"}},"created_at":"2026-05-17T23:46:14.113495+00:00","updated_at":"2026-05-17T23:46:14.113495+00:00"}