Given the definition used and the other post fosho made here (If $f$ and $g$ are branches of $z^a$ and $z^b$ respectively show that $fg$ is a branch of $z^{a+b}$) I think the text in question is Conway's Functions of One Complex Variable I.
The definition of a branch of $z^b$ is given with respect to a branch of log. So if f is a branch of log, we can define a corresponding branch
of $z^b$ by the formula $exp(b f(z))$. In your original post, you list all of the branches of $z^b$ on the connected set $\mathbb{C} - \{z \in R : z \le 0\}$. These correspond to all of the branches of log on this set.
Reviewing Conway's definition, a branch of log on a connected open set G is a continuous function f that satisfies $z = exp(f(z))$ for all z in G. In Joe's answer, he notes that in addition to the choice of $2\pi i k$, there is also a set of branches of log associated with each argument function. It's worth noting that as he defines these argument functions, they are discontinuous along a ray of angle $\theta_0 + \pi$ going from 0 to infinity. Therefore, the branch of log associated with each one will only be defined on the complex plane excluding this ray. That said, when I usually see someone define a branch cut it does take this form, just removing some ray that emanates out from the branch point.
It's probably worth noting that using Conway's definition, there are a large number of other choices for a branch of log that you could make. To give the next simplest example that occurs to me, consider this diagram.

Our choice of the domain, G, is the entire plane except the arrowed curve that consists of a line segment from 0 to -1 and -1 to $-1+i\infty$. Let $f(z) = Log z$, the principal log value on the unshaded region, and $Log z - 2 \pi i$ on the shaded region, $\{Im z > 0, Re z < -1\}$. As you pass across the negative real axis for a real value below -1, this function is continuous. For z just below the negative real axis, $f(z)$ will have imaginary part slightly above $-\pi$. For $f(z)$ just above the negative real axis and with real part below $-1$, it will have imaginary part just below $(\pi - 2\pi) = -\pi$, so the imaginary part does not jump as you go across the negative real axis to the left of $-1$.
At this point in Conway, he hasn't yet defined the contour integral, but if you're familiar with it, one way to describe a large variety of the branches of log would be to say:
- Choose a domain, G, that contains no curves that wind completely around the branch point at 0, and where any two points are connected by a sufficiently regular contour that the contour integral along the curve can be defined.
- Choose a point $z_*$ in G.
- Choose a value for the branch at the point $z_*$ from the possible values, $log z_* + 2\pi i k$ for some integer k.
- The branch will then be well-defined if $f(z) = f(z_*) + \int_\gamma z^{-1} dz$, where $\gamma$ is any curve in G that goes from $z_*$ to z. That this definition
does not depend on the choice of $\gamma$ is due to $z^{-1}$ being analytic away from 0 and $\gamma$ not being able to wind around 0, but this shouldn't be clear yet at this point in the book.
At this point in the book, the best thing you can really say is what Conway says, that any two branches defined on the same connected domain G will differ by a constant factor of $2\pi i k$ for some integer $k$. Therefore any two branches of $z^b$ will differ by a multiplicative factor of the form $exp(i 2 \pi k b)$. When b is a rational number p/q and p and q share no common factors, there will be q different branches with multiplicative factors distributed evenly around the unit circle. When b is irrational, the multiplicative factors will correspond to a countable dense subset of the unit circle. When b is imaginary the branches are real scalar multiples of each other.