I have been reading Chapter 0 of Griffiths' and Harris' Principles of Algebraic Geometry, in particular, the section on Vector Bundles, Connections, and Curvature. I have three questions:
A connection is defined on page 72 as follows: A connection $D$ on a complex vector bundle $E \to M$ is a map $$D : \Omega^0(E) \longrightarrow \Omega^1(E)$$ satisfying the Leibniz rule $$D(f \cdot \zeta) = df \otimes \zeta + f \cdot D(\zeta),$$ for all sections $\zeta \in \Omega^0(E)(U)$, $f \in \mathscr{C}^{\infty}(U)$.
Q1. Why does a connection take values in the space of smooth 1-forms on $E$? A connection yields a way of differentiating sections, generalising the directional derivative on functions. We remind ourselves that the directional derivative of a function $f \in \mathscr{C}^{\infty}(M)$ in the direction of $v \in T_p M$ is the smooth function $D_v f \in \mathscr{C}^{\infty}(M)$ given by $\nabla f \cdot v$.
Is $\nabla f \cdot v$ a 1-form? -- I am not seeing the compatibility here.
Q2. I have previously seen the covariant derivative be defined as a map $D : \Gamma(E) \longrightarrow \Gamma(E) \otimes \Gamma(T^{\ast} M)$ satisfying $D_{v+u}(\sigma) = D_v(\sigma) + D_u(\sigma)$, $D_{f v} (\sigma) = f D_v(\sigma)$, $\mathbb{R}$-linearity in $\sigma$, and the Leiniz rule. Do these definitions coincide, i.e., do we get tensoriality, $\mathbb{R}$-linearity, etc., from the Leibniz rule alone?
Q3. What is the distinction between a unitary frame and a holomorphic frame? Griffiths and Harris do not seem to define the distinction, but they are distinguished (see, e.g., page 73).
Please let me know if anything is not clear, or whether these questions have already been asked here. Thanks in advance.