  ![The left panels show contours of the stop soft mass needed in order to raise the Higgs mass to he observed value when $\mu_{\Sigma}=000{~\text{GeV}}$, $m_{\chi}=00{~\text{TeV}}$ and $\tan\beta=00$. In () both stops have the same mass while () only changes the right-handed soft mass and keeps the left-handed stop at $000{~\text{GeV}}$. The right panels show the corresponding contours of fine tuning. The dark red region marks where the vevs of the triplets cause too-large contributions to the $\mathcal{T}$ parameter. The orange region supposes an improvement in the measured $\mathcal{T}$ parameter by an order of magnitude.[]{data-label="fig:ftLambda"}](Stops_MuSig_000_mchi_00000_Both.pdf "fig:"){width="0.00\linewidth"} ![The left panels show contours of the stop soft mass needed in order to raise the Higgs mass to he observed value when $\mu_{\Sigma}=000{~\text{GeV}}$, $m_{\chi}=00{~\text{TeV}}$ and $\tan\beta=00$. In () both stops have the same mass while () only changes the right-handed soft mass and keeps the left-handed stop at $000{~\text{GeV}}$. The right panels show the corresponding contours of fine tuning. The dark red region marks where the vevs of the triplets cause too-large contributions to the $\mathcal{T}$ parameter. The orange region supposes an improvement in the measured $\mathcal{T}$ parameter by an order of magnitude.[]{data-label="fig:ftLambda"}](FT_MuSig_000_mchi_00000_Both.pdf "fig:"){width="0.00\linewidth"}  ![The left panels show contours of the stop soft mass needed in order to raise the Higgs mass to he observed value when $\mu_{\Sigma}=000{~\text{GeV}}$, $m_{\chi}=00{~\text{TeV}}$ and $\tan\beta=00$. In () both stops have the same mass while () only changes the right-handed soft mass and keeps the left-handed stop at $000{~\text{GeV}}$. The right panels show the corresponding contours of fine tuning. The dark red region marks where the vevs of the triplets cause too-large contributions to the $\mathcal{T}$ parameter. The orange region supposes an improvement in the measured $\mathcal{T}$ parameter by an order of magnitude.[]{data-label="fig:ftLambda"}](Stops_MuSig_000_mchi_00000.pdf "fig:"){width="0.00\linewidth"} ![The left panels show contours of the stop soft mass needed in order to raise the Higgs mass to he observed value when $\mu_{\Sigma}=000{~\text{GeV}}$, $m_{\chi}=00{~\text{TeV}}$ and $\tan\beta=00$. In () both stops have the same mass while () only changes the right-handed soft mass and keeps the left-handed stop at $000{~\text{GeV}}$. The right panels show the corresponding contours of fine tuning. The dark red region marks where the vevs of the triplets cause too-large contributions to the $\mathcal{T}$ parameter. The orange region supposes an improvement in the measured $\mathcal{T}$ parameter by an order of magnitude.[]{data-label="fig:ftLambda"}](FT_MuSig_000_mchi_00000.pdf "fig:"){width="0.00\linewidth"} 