One strategy is to show that $H$ admits a power series about any point in $\mathbb{C}\setminus\{(-\infty,0]\{0\}$ with the help of a little integration theory (dominated convergence).
Here is a sketch of a solution. I let the OP deal with the details should she/he is interested.
One can consider the map
$$F(z)=\int^{\infty}_0\frac{\phi(t)}{t^2-z}dt$$
to make things look more symmetric. The OP's map is $H(z)=F(-z)$.
The map $F$ is analytic (and hence holomorphic) on $D=\{z=x+iy: x>0\}$. To wit, choose $M>0$ so that $|\phi(t)|\leq M$ for all $t$.
Fix $a=\alpha+i\beta\in D$. Notice that $\rho=\inf\{|a-t^2|:t\in\mathbb{R}\}>0$.
Let $B(a;r)$ be an open ball with $r<\rho$. Notice that
$$\frac{\phi(t)}{t^2-z}=\frac{\phi(t)}{(t^2-a)-(z-a)}=\frac{\phi(t)}{t^2-a}\frac{1}{1-\tfrac{z-a}{t^2-a}}=\frac{\phi(t)}{t^2-a}\sum^\infty_{n=0}\Big(\frac{z-a}{t^2-a}\Big)^n\tag{0}\label{zero}$$
The series converges absolutely and uniformly on $B(a;r)$ since $\Big|\frac{z-a}{t^2-a}\Big|\leq \frac{r}{\rho}<1$; furthermore,
$$
\left|\frac{\phi(t)}{t^2-a}\sum^\infty_{n=0}\Big(\frac{z-a}{t^2-a}\Big)^n\right|\leq\frac{M}{\sqrt{(t^2-\alpha)^2+\beta^2}} \frac{\rho}{\rho-r}\in L_1(0,\infty)
$$
The conclusion follows by an application of dominated convergence. In addition, one can obtain the expression:
$$F(z)=\sum^\infty_{n=0}c_n(z-a)^n,\qquad z\in B(a;r)$$
where
$c_n=\int^\infty\frac{\phi(t)}{(t^2-a)^{n+1}}\,dt$.