Kähler form on the Blow up of a Kähler manifold

Let $\widetilde X$ be the blowup of $X$, and let $\pi\colon \widetilde X\to X$ denote the blow-down map. If the local coordinates $(z_i)$ are chosen so that $z=0$ is the point being blown up, then $D = \pi^{-1}(0)\subseteq \widetilde X$ is a complex hypersurface called the exceptional divisor. Because $z_i\circ\pi\equiv 0$, it follows that $d(z_i\circ \pi)$ annihilates every vector tangent to $D$, and the same goes for $d(\bar z_i\circ\pi)$.

If $M$ and $N$ be complex manifolds of the same dimension and $π:M→N$ is a holomorphic mapping, then for a volume form (as measure )$Ψ$ on $N$ the pull-back $π^∗Ψ$ is positive outside aramification divisor of $M$ and may not be a positive on the whole of $M$. There is a classical paper of P. Griffiths http://publications.ias.edu/sites/default/files/nevanlinna.pdf

From Principles of Algebraic Geometry by Phillip Griffiths and Joseph Harris, we have:

Let $Y\subset X$. If $Y$ is compact then blow up is Kahler but to construct the metric on $Bl_YX $substantially you use $π^∗ω+εc_1(\mathcal O(−E))$ where $E$ is the exceptional divisor and $π:Bl_YX\to X$ is the canonical surjection

Definition of positivity of pull back of kahler form as current is different with what you wrote , see this paper. See also the definition of pull back of current https://arxiv.org/pdf/math/0606248.pdf

See Lemma 34. of this paper