Let $f({\bf x})\equiv f(x_1,x_2,\ldots,x_n)$ is a function of $n$ real variables ${\bf x}=(x_1,x_2,\ldots,x_n)$. The Taylor expansion of $f({\bf x})$ is about the point ${\bf x}^0=(x_1^0,x_2^0,\ldots,x_n^0)$, reads, $$f({\bf x})=f({\bf x}^0)+\sum_i\left(\frac{\partial f}{\partial x_i}\right)_{{\bf x}={\bf x}^0}(x_i-x_i^0)+\frac{1}{2!}\sum_i\sum_j\left(\frac{\partial^2 f}{\partial x_i\partial x_j}\right)_{{\bf x}={\bf x}^0}(x_i-x_i^0)(x_j-x_j^0)+\ldots$$ If ${\bf x}^0$ is a local minimum, $$\partial f/\partial x_i=0, \forall i .$$ This is true.
However, is it also true that at ${\bf x}^0$, $$H_{ij}\equiv\left(\frac{\partial^2 f}{\partial x_i\partial x_j}\right)_{{\bf x}={\bf x}^0}\geq 0$$ as claimed here in this Quantum Field Theory Textbook by Lewis Ryder (Eq. 8.24)? See here. If so, can you offer proof of this?