In this paper, we consider the Cauchy problem for the H^{s} -critical inhomogeneous nonlinear Schrödinger (INLS) equation iu_{t} +\Delta u=\lvert{x}\rvert^{-b}f(u),\quad u(0)=u_{0} \in H^{s} (\mathbb{R}^{n}), where n\in \mathbb{N} , 0\le s<\smash{\frac{n}{2}} , 0<b<\min\{2, n-s, 1+\smash{\frac{n-2s}{2}}\} and f(u) is a nonlinear function that behaves like \lambda \lvert{u}\rvert^{\sigma}u with \lambda \in \mathbb{C} and \sigma=\smash{\frac{4-2b}{n-2s}} . First, we establish the local well-posedness as well as the small data global well-posedness in H^{s}(\mathbb{R}^{n}) for the H^{s} -critical INLS equation by using the contraction mapping principle based on the Strichartz estimates in Sobolev–Lorentz spaces. Next, we obtain some standard continuous dependence results for the H^{s} -critical INLS equation. Our results about the well-posedness and standard continuous dependence for the H^{s} -critical INLS equation improve the ones of Aloui–Tayachi [Discrete Contin. Dyn. Syst. 41 (2021), 5409–5437] and An–Kim [Evol. Equ. Control Theory 12 (2023), 1039–1055] by extending the validity of s and b . Based on the local well-posedness in H^{1}(\mathbb{R}^{n}) , we finally establish the blow-up criteria for H^{1} -solutions to the focusing energy-critical INLS equation. In particular, we prove the finite time blow-up for finite-variance, radially symmetric or cylindrically symmetric initial data.