Changes between Version 6 and Version 7 of FourFermionbbll
- Timestamp:
- Mar 24, 2021, 3:22:27 PM (3 years ago)
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FourFermionbbll
v6 v7 16 16 #!latex 17 17 \begin{align*} 18 \mathcal{L}_{eff} = \frac{g^2}{\Lambda^2}\sum_{i,j=L,R} \eta_{ij}(\bar{b}_{i} \gamma_{\mu} b_{i}) (\bar{\ell}_{j} \gamma^{\mu} \ell_{j}) ,18 \mathcal{L}_{eff} = \frac{g^2}{\Lambda^2}\sum_{i,j=L,R} \eta_{ij}(\bar{b}_{i} \gamma_{\mu} b_{i}) (\bar{\ell}_{j} \gamma^{\mu} \ell_{j}) ~. 19 19 \end{align*} 20 20 }}} … … 31 31 32 32 where the first term is the pure SM term and the second term contains the NP contributions. The NP contributions have one interference and one pure NP term: 33 33 34 {{{ 34 35 #!latex 35 36 \begin{align*} 36 \sigma^{NP}(g,\Lambda,m_{\ell \ell})=\frac{g^2}{\Lambda^2} \cdot \sigma^{SM \times NP}(m_{\ell \ell}) + \frac{g^4}{\Lambda^4} \cdot \sigma^{NP \times NP}(m_{\ell \ell}) ~ ,37 \sigma^{NP}(g,\Lambda,m_{\ell \ell})=\frac{g^2}{\Lambda^2} \cdot \sigma^{SM \times NP}(m_{\ell \ell}) + \frac{g^4}{\Lambda^4} \cdot \sigma^{NP \times NP}(m_{\ell \ell}) ~. 37 38 \end{align*} 38 39 }}}
