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?
You can see the positivity from taking a limit. Note that for a function $g$ with second derivative at $0$ we have
$$g''(0) = \lim_{t\to 0} \frac{g(t) + g(-t) - 2 g(0)}{t^2}$$
and so, if moreover $0$ is a local minimum, we have $g''(0) \ge 0$.
Now take the case of your problem. Let $h\in \mathbb{R}^n$. The functions
$$t \mapsto g(t) \colon = f(x_0 + t h)$$
has a minimum at $t=0$, so $g''(0)\ge 0$. But we have
$$g''(0) = \sum_{i,j} \frac{\partial f}{\partial x_i \partial x_j}_{x=x_0} h_i h_j $$