Precision Higgs Constraints in U(1) Extensions of the Standard Model with a Light <i>Z</i>′-Boson

Anomaly-free <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mi>U</mi><mo>(</mo><mn>1</mn><mo>)</mo></mrow></semantics></math></inline-...

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Main Authors: Zoltán Péli, Zoltán Trócsányi
Format: Article
Language:English
Published: MDPI AG 2025-01-01
Series:Universe
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Online Access:https://www.mdpi.com/2218-1997/11/1/12
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author Zoltán Péli
Zoltán Trócsányi
author_facet Zoltán Péli
Zoltán Trócsányi
author_sort Zoltán Péli
collection DOAJ
description Anomaly-free <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mi>U</mi><mo>(</mo><mn>1</mn><mo>)</mo></mrow></semantics></math></inline-formula> extensions of the standard model (SM) predict a new neutral gauge boson <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msup><mi>Z</mi><mo>′</mo></msup></semantics></math></inline-formula>. When <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msup><mi>Z</mi><mo>′</mo></msup></semantics></math></inline-formula> obtains its mass from the spontaneous breaking of the new <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mi>U</mi><mo>(</mo><mn>1</mn><mo>)</mo></mrow></semantics></math></inline-formula> symmetry by a new complex scalar field, the model also predicts a second real scalar <i>s</i>, and the search for the new scalar and the search for the new gauge boson become intertwined. We present the computation of production cross sections and decay widths of such a scalar <i>s</i> in models with a light <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msup><mi>Z</mi><mo>′</mo></msup></semantics></math></inline-formula> boson when the decay <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mi>h</mi><mo>→</mo><msup><mi>Z</mi><mo>′</mo></msup><msup><mi>Z</mi><mo>′</mo></msup></mrow></semantics></math></inline-formula> may have a sizeable branching ratio. We show how the Higgs signal strength measurement in this channel can provide stricter exclusion bounds on the parameters of the model than those obtained from the total signal strength for Higgs boson production.
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spelling doaj-art-bb6c22a80951436f85d64f4ac079ff6d2025-01-24T13:51:28ZengMDPI AGUniverse2218-19972025-01-011111210.3390/universe11010012Precision Higgs Constraints in U(1) Extensions of the Standard Model with a Light <i>Z</i>′-BosonZoltán Péli0Zoltán Trócsányi1Institute for Theoretical Physics, ELTE Eötvös Loránd University, Pázmány Péter Sétány 1/A, 1117 Budapest, HungaryInstitute for Theoretical Physics, ELTE Eötvös Loránd University, Pázmány Péter Sétány 1/A, 1117 Budapest, HungaryAnomaly-free <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mi>U</mi><mo>(</mo><mn>1</mn><mo>)</mo></mrow></semantics></math></inline-formula> extensions of the standard model (SM) predict a new neutral gauge boson <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msup><mi>Z</mi><mo>′</mo></msup></semantics></math></inline-formula>. When <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msup><mi>Z</mi><mo>′</mo></msup></semantics></math></inline-formula> obtains its mass from the spontaneous breaking of the new <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mi>U</mi><mo>(</mo><mn>1</mn><mo>)</mo></mrow></semantics></math></inline-formula> symmetry by a new complex scalar field, the model also predicts a second real scalar <i>s</i>, and the search for the new scalar and the search for the new gauge boson become intertwined. We present the computation of production cross sections and decay widths of such a scalar <i>s</i> in models with a light <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><msup><mi>Z</mi><mo>′</mo></msup></semantics></math></inline-formula> boson when the decay <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mi>h</mi><mo>→</mo><msup><mi>Z</mi><mo>′</mo></msup><msup><mi>Z</mi><mo>′</mo></msup></mrow></semantics></math></inline-formula> may have a sizeable branching ratio. We show how the Higgs signal strength measurement in this channel can provide stricter exclusion bounds on the parameters of the model than those obtained from the total signal strength for Higgs boson production.https://www.mdpi.com/2218-1997/11/1/12beyond the standard modelsuperweak extensionnew neutral gauge bosonscalar searchexclusion limits
spellingShingle Zoltán Péli
Zoltán Trócsányi
Precision Higgs Constraints in U(1) Extensions of the Standard Model with a Light <i>Z</i>′-Boson
Universe
beyond the standard model
superweak extension
new neutral gauge boson
scalar search
exclusion limits
title Precision Higgs Constraints in U(1) Extensions of the Standard Model with a Light <i>Z</i>′-Boson
title_full Precision Higgs Constraints in U(1) Extensions of the Standard Model with a Light <i>Z</i>′-Boson
title_fullStr Precision Higgs Constraints in U(1) Extensions of the Standard Model with a Light <i>Z</i>′-Boson
title_full_unstemmed Precision Higgs Constraints in U(1) Extensions of the Standard Model with a Light <i>Z</i>′-Boson
title_short Precision Higgs Constraints in U(1) Extensions of the Standard Model with a Light <i>Z</i>′-Boson
title_sort precision higgs constraints in u 1 extensions of the standard model with a light i z i boson
topic beyond the standard model
superweak extension
new neutral gauge boson
scalar search
exclusion limits
url https://www.mdpi.com/2218-1997/11/1/12
work_keys_str_mv AT zoltanpeli precisionhiggsconstraintsinu1extensionsofthestandardmodelwithalightiziboson
AT zoltantrocsanyi precisionhiggsconstraintsinu1extensionsofthestandardmodelwithalightiziboson