Concept:
This problem is evaluated using principles of complex integration, specifically Cauchy's Integral Theorem and the Residue Theorem.
- Cauchy's Integral Theorem states that if a function $f(z)$ is analytic everywhere inside and along a simple closed contour $C$, then $\oint_C f(z) dz = 0$.
- The Residue Theorem states that if $f(z)$ is meromorphic inside a contour $C$, then $\oint_C f(z) dz = 2\pi i \sum (\text{Residues at poles inside } C)$.
- The sum of all residues of a rational function in the extended complex plane (including the point at infinity) is zero: $\sum \text{Res}(z_i) + \text{Res}(\infty) = 0$.
Step 1: Evaluate the integral $I_1$ along contour $C_1$.
The singularities (poles) of the function $f(z) = \frac{z}{(z-\alpha)(z-\beta)(z-\gamma)}$ are located at the points $z = \alpha$, $z = \beta$, and $z = \gamma$.
The contour $C_1$ is defined by the disk $|z| < r$, where $r = \text{Min}\{\alpha, \beta, \gamma\}$. This means that the distance from the origin to the nearest pole is $r$. Therefore, there are absolutely no poles located inside the region bounded by $C_1$.
Since $f(z)$ is completely analytic within and on $C_1$, by Cauchy's Integral Theorem:
\[
I_1 = \oint_{C_1} f(z) dz = 0
\]
Step 2: Analyze the contour $C_2$ for integral $I_2$.
The second contour is defined as $C_2 : |z| = R+1$, where $R = \text{Max}\{\alpha, \beta, \gamma\}$. Because the radius of this circular path is strictly greater than the maximum absolute value among all poles, all three poles ($z = \alpha, \beta, \gamma$) lie entirely inside $C_2$.
By the Residue Theorem:
\[
I_2 = 2\pi i \left[ \text{Res}(f, \alpha) + \text{Res}(f, \beta) + \text{Res}(f, \gamma) \right]
\]
Step 3: Compute the sum of residues using the residue at infinity.
Instead of calculating three separate algebraic residues, we can use the macro property of complex functions: the sum of all residues at finite poles is equal to negative the residue of the function at infinity:
\[
\sum \text{Res}(f, \text{finite}) = \text{Res}\left[ - \frac{1}{w^2} f\left(\frac{1}{w}\right), 0 \right]
\]
Let us substitute $z = \frac{1}{w}$ into $f(z)$:
\[
f\left(\frac{1}{w}\right) = \frac{\frac{1}{w}}{\left(\frac{1}{w} - \alpha\right)\left(\frac{1}{w} - \beta\right)\left(\frac{1}{w} - \gamma\right)} = \frac{\frac{1}{w}}{\frac{(1-\alpha w)(1-\beta w)(1-\gamma w)}{w^3}} = \frac{w^2}{(1-\alpha w)(1-\beta w)(1-\gamma w)}
\]
Now, apply the transformation formula for the residue at infinity:
\[
- \frac{1}{w^2} f\left(\frac{1}{w}\right) = - \frac{1}{w^2} \cdot \frac{w^2}{(1-\alpha w)(1-\beta w)(1-\gamma w)} = \frac{-1}{(1-\alpha w)(1-\beta w)(1-\gamma w)}
\]
Evaluating this expression at $w = 0$:
\[
\text{Res}(f, \infty) = \frac{-1}{(1-0)(1-0)(1-0)} = -1
\]
Since the residue at infinity is $-1$, the sum of all finite residues inside $C_2$ must be:
\[
\sum \text{Res}(finite) = -\text{Res}(f, \infty) = -(-1) = 1
\]
Wait, let's verify via direct asymptotic behavior. As $z \to \infty$, $f(z) \sim \frac{z}{z^3} = \frac{1}{z^2}$. Since $f(z)$ decays as $\frac{1}{z^2}$, the residue at infinity is defined as $\lim_{z \to \infty} -z f(z) = \lim_{z \to \infty} -\frac{1}{z} = 0$.
Let's double-check the calculation:
\[
f(z) = \frac{z}{z^3 (1-\alpha/z)(1-\beta/z)(1-\gamma/z)} = \frac{1}{z^2} (1 + \dots)
\]
Ah! The residue at infinity is the coefficient of $\frac{1}{z}$ with a negative sign in the Laurent expansion around infinity. Since there is no $\frac{1}{z}$ term (the leading power is $\frac{1}{z^2}$), the residue at infinity is indeed $0$.
Therefore:
\[
\sum \text{Res}(finite) = 0 \quad \Rightarrow \quad I_2 = 2\pi i (0) = 0
\]
Step 4: Sum the two integrals.
Combining the results from Step 1 and
Step 3:
\[
I_1 + I_2 = 0 + 0 = 0
\]
This matches Option (B).