$\left( \frac{1}{2m}(\vec \sigma ( \vec p - q\vec A))^2 + q\phi \right) \Psi = i \hbar \partial_t \Psi $
The Pauli equation describes how the state of a quantum system with half-integer spin changes in time.
In contrast, the Schrödinger equation describes the time evolution of systems without spin.
The Pauli equation is the non-relativistic limit of the Dirac equation.
The Pauli equation is the correct non-relativistic equation to describe spin $1/2$ particles.
Take note that $\vec \sigma$, a "vector of matrices" is only used as a convenient short-hand notation for the sums that appear in the equation. For example, $\vec \sigma \vec p = \sigma_1 p_1 + \sigma_2 p_2 + \sigma_3 p_3. $