the correct order of magnitude we now calculate the various soft terms bringing $M_p$ back in the expressions. Then the gravitino mass $m_{3/2}$ and scalar mass term $m_{\alpha}$ are given by

$$\begin{gathered}
\label{gravitino}
m_{3/2}^2=\frac{1}{M_p^4} e^{ h(\tilde t_0)} \frac{1}{16 \tilde s_0 \tilde t_0^3} \left[f(\tilde s_0)
+\frac{A a e^{-a \tilde t_0}}{-\frac{3}{2 \tilde t_0}+h'(\tilde t_0)}\right]^2\\ 
\label{softmass}
\begin{split}
m_{\alpha}^2 = ~   & m_{3/2}^2 \\
&+ \frac{1}{M_p^4}\frac {e^{h(\tilde t_0)}}{{16 \tilde s_0 \tilde t_0^3}}  \frac{1}{\left(\frac{3}{4 \tilde t_0^2}
+h''(\tilde t_0) \right)} \left[f^2 ( \tilde s_0) \left(\frac{3}{2 \tilde t_0}-h'(\tilde t_0) \right)^2 \right]\left[1-
\frac{1}{4 \tilde t^2_0} \frac{1}{\left(\frac{3}{4 \tilde t_0^2}+ h''(\tilde t_0)\right)}\right]
\end{split}\end{gathered}$$

Considering the VEV for all moduli fields $\sim M_p$ and $h''(\tilde t_0)$ as well as $a$ are very close to $O(1)$, the gravitino mass $m_{3/2}$ may become $\sim$ TeV. With $A \sim \Lambda_N^3 
\sim 10^{42} ~\rm GeV^3$ gravitino mass $\sim$ TeV can be generated. It is important to note that, the contribution arising from $F^T$ would involve only $f(\tilde s_0)$ at the minimum. Then, accepting the fact that $f(\tilde s_0)$ assumes a value which can produce a small vacuum energy, $F^T$ cannot provide any significant contributions towards the soft breaking parameters. Thus in Eq.(\[softmass\]), the scalar mass term $m^2_\alpha$ parameter includes the $m^2_{3/2}$ as the leading term. 