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Interpreting electroweak precision data including the W-mass CDF anomaly
by
Strumia, Alessandro
in
Classical and Quantum Gravitation
/ Collaboration
/ Dark matter
/ Elementary Particles
/ Extra Dimensions
/ High energy physics
/ Kinematics
/ New Gauge Interactions
/ Other Weak Scale BSM Models
/ Particle decay
/ Physics
/ Physics and Astronomy
/ Quantum Field Theories
/ Quantum Field Theory
/ Quantum Physics
/ Quarks
/ Regular Article - Theoretical Physics
/ Relativity Theory
/ String Theory
2022
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Interpreting electroweak precision data including the W-mass CDF anomaly
by
Strumia, Alessandro
in
Classical and Quantum Gravitation
/ Collaboration
/ Dark matter
/ Elementary Particles
/ Extra Dimensions
/ High energy physics
/ Kinematics
/ New Gauge Interactions
/ Other Weak Scale BSM Models
/ Particle decay
/ Physics
/ Physics and Astronomy
/ Quantum Field Theories
/ Quantum Field Theory
/ Quantum Physics
/ Quarks
/ Regular Article - Theoretical Physics
/ Relativity Theory
/ String Theory
2022
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Interpreting electroweak precision data including the W-mass CDF anomaly
by
Strumia, Alessandro
in
Classical and Quantum Gravitation
/ Collaboration
/ Dark matter
/ Elementary Particles
/ Extra Dimensions
/ High energy physics
/ Kinematics
/ New Gauge Interactions
/ Other Weak Scale BSM Models
/ Particle decay
/ Physics
/ Physics and Astronomy
/ Quantum Field Theories
/ Quantum Field Theory
/ Quantum Physics
/ Quarks
/ Regular Article - Theoretical Physics
/ Relativity Theory
/ String Theory
2022
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Interpreting electroweak precision data including the W-mass CDF anomaly
Journal Article
Interpreting electroweak precision data including the W-mass CDF anomaly
2022
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Overview
A
bstract
We perform a global fit of electroweak data, finding that the anomaly in the
W
mass claimed by the CDF collaboration can be reproduced as a universal new-physics correction to the
T
parameter or |
H
†
D
μ
H
|
2
operator. Contributions at tree-level from multi-TeV new physics can fit the anomaly compatibly with collider bounds: we explore which scalar vacuum expectation values (such as a triplet with zero hypercharge),
Z
′ vectors (such as a
Z
′ coupled to the Higgs only), little-Higgs models or higher-dimensional geometries provide good global fits. On the other hand, new physics that contributes at loop-level must be around the weak scale to fit the anomaly. Thereby it generically conflicts with collider bounds, that can be bypassed assuming special kinematics like quasi-degenerate particles that decay into Dark Matter (such as an inert Higgs doublet or appropriate supersymmetric particles).
Publisher
Springer Berlin Heidelberg,Springer Nature B.V,SpringerOpen
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