Table 1 The field content of the TNMSSM.
Superfields | Bosons | Fermions |
|---|---|---|
\(\widehat{Q}\) | \(\widetilde{Q}^{T}=(\widetilde{u},\widetilde{d})_{L}\) | \(Q^{T}=(u,d)_{L}\) |
\(\widehat{L}\) | \(\widetilde{L}^{T}=(\widetilde{\nu _{l}},\widetilde{l})_{L}\) | \(L^{T}=(\nu _{l},l)_{L}\) |
\(\widehat{U}\) | \(\widetilde{U}=\widetilde{u}^{*}_{R}\) | \((u_{R})^{C}=(u^{C})_{L}\) |
\(\widehat{D}\) | \(\widetilde{D}=\widetilde{d}^{*}_{R}\) | \((d_{R})^{C}=(d^{C})_{L}\) |
\(\widehat{E}\) | \(\widetilde{E}=\widetilde{l}^{*}_{R}\) | \((l_{R})^{C}=(l^{C})_{L}\) |
\(\widehat{H_{u}}\) | \(H_{u}^{T}=(H_{u}^{+},H_{u}^{0})\) | \(\widetilde{H}_{u}^{T}=(\widetilde{H}_{u}^{+},\widetilde{H}_{u}^{0})\) |
\(\widehat{H_{d}}\) | \(H_{d}^{T}=(H_{d}^{0},H_{d}^{-})\) | \(\widetilde{H}_{d}^{T}=(\widetilde{H}_{d}^{0},\widetilde{H}_{u}^{-})\) |
\(\widehat{S}\) | S | \(\widetilde{S}\) |
\(\widehat{T}\) | \(\left( \begin{array}{ll} \widetilde{T}^{+}/\sqrt{2} &{} -\widetilde{T}^{++}\\ \widetilde{T}^0 &{} -\widetilde{T}^{+}/ \sqrt{2} \end{array}\right) \) | \(\left( \begin{array}{ll} T^{+}/\sqrt{2} &{}-T^{++}\\ T^0 &{} -T^{+}/ \sqrt{2} \end{array}\right) \) |
\(\widehat{\bar{T}}\) | \(\left( \begin{array}{ll} \widetilde{\bar{T}}^{-}/\sqrt{2} &{} -\widetilde{\bar{T}}^{0}\\ \widetilde{\bar{T}}^{{-}{-}} &{} -\widetilde{\bar{T}}^{-}/\sqrt{2} \end{array}\right) \) | \(\left( \begin{array}{ll} \bar{T}^{-}/\sqrt{2} &{} -\bar{T}^{0}\\ \bar{T}^{{-}{-}} &{} -\bar{T}^{-}/\sqrt{2} \end{array}\right) \) |
