用电弱有效理论约束共振

I. Rosell, A. Pich, J. J. Sanz-Cillero
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引用次数: 1

摘要

考虑到标准模型(SM)态与可能的新粒子之间的质量差距,有效场论是一种合适的方法。我们研究了电弱对称性破缺的非线性实现:电弱有效理论(EWET),也称为希格斯有效场理论(HEFT)或电弱手性拉格朗日理论(EWChL)。在更高的尺度上,我们考虑一个共振电弱拉格朗日,将SM场耦合到共振。将这些共振积分出来,并假设它们具有良好的高能行为,一些玻色子的低能常数是由共振质量决定或限制的。目前这些低能常数的实验边界允许我们将共振质量尺度推到TeV范围,$M_R \geq 2\,$ TeV,与先前的估计很好地一致。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Constraining resonances by using the electroweak effective theory
In the light of the mass gap between Standard Model (SM) states and possible new particles, effective field theories are a suitable approach. We take on the non-linear realization of the electroweak symmetry breaking: the electroweak effective theory (EWET), also known as Higgs effective field theory (HEFT) or electroweak chiral Lagrangian (EWChL). At higher scales we consider a resonance electroweak Lagrangian, coupling SM fields to resonances. Integrating out these resonances and assuming a well-behaved high-energy behavior, some of the bosonic low-energy constants are determined or constrained in terms of resonance masses. Present experimental bounds on these low-energy constants allow us to push the resonance mass scale to the TeV range, $M_R \geq 2\,$TeV, in good agreement with previous estimations.
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