Having read a lot of things by Arnold, I think his point of view was that "every student should know" the formula
$$\int\ldots\int_{\mathbb{R}^n}\exp\left\{-\frac12 x^TAx\right\}dx_1\ldots dx_n=\frac{(2\pi)^{n/2}}{\sqrt{\mathrm{det}\,A}},\tag{1}$$
where $x^T=(x_1,\ldots,x_n)$ and $A$ is a real symmetric positive definite $n\times n$ matrix. Actually, every physics student should know it indeed.
What remains is a simple linear algebra exercise.
Added: The gaussian integration formula (1) is obtained by noticing that the matrix $A$ can be brought to diagonal form by orthogonal transformation, characterized by unit jacobian. Then one is left with a product of gaussian integrals $\prod_{k=1}^n\int_{-\infty}^{\infty}\exp\{-\lambda_k x^2/2\}dx$, where $\lambda_{1\ldots n}$ denote the eigenvalues of $A$.