It might be an easy question, possibly not worth posting here. In the proof of the Lagrangian neighborhood theorem, the authors have written the expression for the derivative of a symplectomorphism at a point of the zero section. I don't understand how one arrives at this expression.
Let $L$ be a Lagrangian submanifold of the symplectic manifold $(M,\omega)$. Choose an almost complex structure $J\colon TM\to TM$ compatible with $\omega$. Thus $g_J:=\omega(-,J\cdot)$ is a Riemannian metric on $M$.
Define $\phi\colon T^*L\to M$ as follows $\phi(q, v^*)=\exp_q\left(J_q \Phi_q(v^*)\right)$, where $g_J\left(\Phi_q(v^*),v\right)=v^*(v)$.
Question 1: I think $\phi$ can't be defined on whole $T^*L$, shouldn't the domain of definition of $\phi$ is an open subset of the zero section $L\subset T^*L$?
Question 2: Why $d\phi_{(q,0)}(v_0,v_1^*)=v_0+J_q\Phi_q(v_1^*)$, where $(v_0,v_1^*)\in T_qL\oplus T^*_qL=T_{(q,0)}T^*L$?
Note that $J(TL)$ is the normal bundle $NL$ of $L$ in $M$ w.r.t. $g_J$.
Reference: Introduction to Symplectic Topology by Dusa McDuff, Dietmar Salamon; see page 121.