{"doi":"10.1103/vx7q-ns9p","title":"Radiative corrections to the \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:mi>S</mml:mi></mml:mrow></mml:math>\n, \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:mi>T</mml:mi></mml:mrow></mml:math>\n, \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:mi>U</mml:mi></mml:mrow></mml:math>\n parameters and their impact on the \n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mi>W</mml:mi></mml:math>\n boson mass in the 331 model","abstract":"<jats:p>We investigate radiative corrections to electroweak precision observables, specifically the Peskin-Takeuchi parameters <a:math xmlns:a=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><a:mrow><a:mi>S</a:mi></a:mrow></a:math>, <c:math xmlns:c=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><c:mrow><c:mi>T</c:mi></c:mrow></c:math>, and <e:math xmlns:e=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><e:mi>U</e:mi></e:math>, in the <g:math xmlns:g=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><g:mi>S</g:mi><g:mi>U</g:mi><g:mo stretchy=\"false\">(</g:mo><g:mn>3</g:mn><g:msub><g:mo stretchy=\"false\">)</g:mo><g:mi>C</g:mi></g:msub><g:mo>×</g:mo><g:mi>S</g:mi><g:mi>U</g:mi><g:mo stretchy=\"false\">(</g:mo><g:mn>3</g:mn><g:msub><g:mo stretchy=\"false\">)</g:mo><g:mi>L</g:mi></g:msub><g:mo>×</g:mo><g:mi>U</g:mi><g:mo stretchy=\"false\">(</g:mo><g:mn>1</g:mn><g:msub><g:mo stretchy=\"false\">)</g:mo><g:mi>X</g:mi></g:msub></g:math> model (also known as the 331 model) with <o:math xmlns:o=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><o:mi>β</o:mi><o:mo>=</o:mo><o:mo>−</o:mo><o:msqrt><o:mn>3</o:mn></o:msqrt></o:math>. Using the  and heno packages, we compute the mass spectrum and low-energy observables. We show that these parameters place strong constraints on the model, requiring most of the scalar masses to lie in the TeV range or below, and impose indirect bounds on the newly predicted gauge bosons. Furthermore, we demonstrate that the model can accommodate the <q:math xmlns:q=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><q:mi>W</q:mi></q:math> boson mass anomaly reported by the CDF Collaboration, should future measurements confirm its persistence.</jats:p>","journal":"Physical Review D","year":2025,"id":11425,"datarank":0.0,"base_score":0.0,"endowment":0.0,"self_citation_contribution":0.0,"citation_network_contribution":0.0,"self_endowment_contribution":0.0,"citer_contribution":0.0,"corpus_percentile":null,"corpus_rank":null,"citation_count":0,"citer_count":0,"citers_with_citation_signal":0,"citers_with_endowment":0,"datacite_reuse_total":0,"is_dataset":false,"is_dataset_confidence":0.0666,"is_data_producer":false,"deposit_databanks":null,"is_oa":true,"file_count":0,"downloads":0,"has_version_chain":false,"published_date":"2025-09-19","fair_score":null,"fair_percentile":null,"algorithm_id":"datarank_citation_only_1hop_v6","ranking_scope":"data_only","authors":[{"id":91674,"name":"M. A. Iqbal","orcid":"0009-0002-3968-801X","position":1,"is_corresponding":false},{"id":91675,"name":"M. E. Gómez","orcid":"0000-0002-0137-0295","position":2,"is_corresponding":false},{"id":91676,"name":"O. Panella","orcid":"0000-0003-4262-894X","position":3,"is_corresponding":false},{"id":91673,"name":"M. Rehman","orcid":"0000-0002-1069-0637","position":0,"is_corresponding":true}],"reference_count":58,"raw_metadata":null,"created_at":"2026-03-01T18:20:47.508186Z","pmid":null,"pmcid":null,"fwci":null,"citation_percentile":null,"influential_citations":0,"oa_status":null,"license":null,"views":0,"total_file_size_bytes":0,"version_count":0,"fair_f":null,"fair_a":null,"fair_i":null,"fair_r":null,"fair_zscore":null,"fair_rationale":null,"fair_model":null,"fair_agent_version":null,"fair_fulltext_source":null,"fair_has_llm":null,"fair_computed_at":null,"clinical_trials":[],"software_tools":[],"db_accessions":[],"linked_datasets":[],"topics":[]}