Quadratic forms and positive definiteness
Quadratic forms
$$ q(x) = x^TAx, \quad A \text{ symmetric (WLOG: the antisymmetric part of } A \text{ always contributes } 0). $$
Shapes
$$ q(x)=\underbrace{x^T}_{1\times n}\ \underbrace{A}_{n\times n}\ \underbrace{x}_{n\times1}=\underbrace{q(x)}_{1\times1} =\sum_{i,j}A_{ij}\,x_ix_j. $$
Squeezed between a row and a column, the $n\times n$ matrix collapses to a single number: $Ax$ is a vector ($n\times1$), and $x^T$ dots it with $x$ to give a scalar.
Intuition: $q$ traces a bowl, dome, or saddle; $A$'s eigenvalues are the curvature along each principal axis.
Example
Reusing $A = \begin{pmatrix}2&1\\1&2\end{pmatrix}$:
$$ q(x) = 2x_1^2 + 2x_1x_2 + 2x_2^2, \quad q(1,1) = 2+2+2 = 6. $$
Diagonalizing a quadratic form
Using the spectral theorem $A=Q\Lambda Q^T$, substitute $y = Q^Tx$ (coordinates in the eigenbasis):
$$ q(x) = x^TQ\Lambda Q^Tx = y^T\Lambda y = \sum_i \lambda_iy_i^2. $$
Shapes
$$ \underbrace{y}_{n\times1}=\underbrace{Q^T}_{n\times n}\underbrace{x}_{n\times1}, \qquad q=\underbrace{y^T}_{1\times n}\underbrace{\begin{pmatrix}\lambda_1&&\\&\ddots&\\&&\lambda_n\end{pmatrix}}_{\Lambda,\ n\times n}\underbrace{y}_{n\times1}. $$
Intuition: in the eigenbasis, a quadratic form is just a weighted sum of squares, no cross terms.
Example
For $x=(1,1)$: $y = Q^Tx = (\sqrt2, 0)$, so $q(x) = 3(\sqrt2)^2 + 1(0)^2 = 6$. ✓
Positive definiteness
$A$ is positive definite if $q(x)>0$ for every $x\neq0$. From the sum-of-squares form, that holds iff every $\lambda_i>0$ (semidefinite allows $\lambda_i\geq0$; indefinite means mixed signs, a saddle).
Quick test without eigenvalues, for $A=\begin{pmatrix}a&b\\b&d\end{pmatrix}$: positive definite iff $a>0$ and $ad-b^2>0$.
Intuition: positive definite means every direction curves upward, a genuine bowl with one bottom.
Example
Our $A$: $a=2>0$, $ad-b^2=4-1=3>0$, positive definite, matching eigenvalues $3,1>0$.
Contrast $B=\begin{pmatrix}0&1\\1&0\end{pmatrix}$: $a=0$ fails immediately; eigenvalues are $\pm1$, indefinite (a saddle). Note $B$ shares $A$’s eigenvectors, since $A=2I+B$.
The Hessian and convexity
Near a critical point $x_0$ (where $\nabla f(x_0)=0$), a smooth $f$ looks like its own quadratic form:
$$ f(x_0+\Delta x) \approx f(x_0) + \tfrac12 \Delta x^TH\Delta x, \quad H = \nabla^2f(x_0) \text{ (the Hessian)}. $$
Shapes
$$ \underbrace{\Delta x^T}_{1\times n}\ \underbrace{H}_{n\times n}\ \underbrace{\Delta x}_{n\times1} = \underbrace{\text{scalar}}_{1\times1}, \qquad H = H^T \ (n\times n\text{, symmetric}). $$
Intuition: the Hessian is just another $A$ in $x^TAx$, built from an $n\times n$ grid of second partial derivatives, one feature pair at a time.
$H$ positive definite: strict local minimum. $H$ negative definite: local maximum. $H$ indefinite: saddle point. $f$ is convex everywhere iff $H(x)$ is positive semidefinite everywhere.
Intuition: close to a critical point, the Hessian's definiteness is the only thing that decides what kind of point it is.
Example
$f(x_1,x_2) = x_1^2+x_1x_2+x_2^2$ has Hessian $H=\begin{pmatrix}2&1\\1&2\end{pmatrix}=A$, our running example, positive definite. So $x=0$ is a strict (global) minimum of $f$.