Abstract
Leptoquark (LQ) models can be the solution to the $(g-2)_{\mu}$ anomaly because of the chiral enhancements. In this work, we consider the models extended by the LQ and vector-like quark (VLQ) simultaneously, which can be used to explain the anomaly because of the top quark and top partner (denoted as $T$) mixing. For the one LQ and one VLQ extended models, there are contributions from the top and $T$ quark. In the minimal LQ models, only the $R_2$ and $S_1$ representations can lead to the chiral enhancements. Here, we find one new $S_3$ solution to the anomaly in the presence of $(X,T,B)_{L,R}$ triplet. We also consider the one LQ and two VLQ extended models, which can solve the anomaly even in the absence of top interactions and mixings. Then, we propose new LQ search channels under the constraints of $(g-2)_{\mu}$. Besides the traditional $t\mu$ decay channel, the LQ can also decay into $T\mu$ final states, which will lead to the characteristic multi-top and multi-muon signals at hadron colliders.
Highlights
Lepton magnetic moments play an important role in the development of the standard model (SM) of elementary particle physics
SUMMARY AND CONCLUSIONS We consider the models containing the LQ and vectorlike quark (VLQ) simultaneously, which can be the solution to the ðg − 2Þμ anomaly because of the chiral enhancement
In addition to the traditional R2 and S1 choices, we find the new S3 solution to the anomaly in the presence of the ðX; T; BÞL;R triplet, which is dominated by the T-quark contributions
Summary
Lepton magnetic moments play an important role in the development of the standard model (SM) of elementary particle physics. The SM prediction is aSμM 1⁄4 116591810ð43Þ × 10−11 [5–25], which results in a 4.2σ discrepancy with Δaμ ≡ aEμxp − aSμM 1⁄4 ð251 Æ 59Þ × 10−11 This excess may be pinned down with more data at FNAL and J-PARC [26]. This anomaly could be caused by the experimental and theoretical uncertainties [27], we are more interested in the new physics interpretations. Leptoquarks (LQs) are well motivated in the grand unified theories [55–57], and they can be an alternative choice for the ðg − 2Þμ anomaly [58–64] because of the significant chiral enhancement mt=mμ They can be used to explain the anomalies in B physics [60,65–69], we will not discuss those here. We will consider the simultaneous scalar LQ and VLQ extended models
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