Concept:
The standard representation of a Fourier series for a function with period $T = 2L$ defined on an interval $[c, c+2L]$ is given by:
\[
f(x) = \frac{a_0}{2} + \sum_{n=1}^{\infty} \left( a_n \cos \frac{n\pi x}{L} + b_n \sin \frac{n\pi x}{L} \right)
\]
However, notice carefully that in the problem description, the summation begins from $n=0$ with no separate constant term divided by 2:
\[
f(x) = \sum_{n=0}^{\infty} \left(a_n \cos \frac{n\pi x}{2} + b_n \sin \frac{n\pi x}{2}\right)
\]
Evaluating the term inside the summation specifically for $n=0$:
\[
a_0 \cos(0) + b_0 \sin(0) = a_0 \cdot 1 + 0 = a_0
\]
Thus, the continuous definition of the DC value (average value) under this specific notation requires setting up the average value over the period:
\[
a_0 = \frac{1}{T}\int_{0}^{T} f(x)\,dx
\]
Here, the period $T = 4$, as indicated by the translation condition $f(x+4) = f(x)$.
Step 1: Set up the definitive integral.
Given $f(x) = x^3$ over the primary period interval $[0, 4]$, the formula for this non-standard definition coefficient $a_0$ is:
\[
a_0 = \frac{1}{4} \int_{0}^{4} x^3 \, dx
\]
Step 2: Perform the integration.
Using the standard power rule of calculus ($\int x^n dx = \frac{x^{n+1}}{n+1}$):
\[
\int_{0}^{4} x^3 \, dx = \left[ \frac{x^4}{4} \right]_{0}^{4}
\]
Substituting the limits of integration:
\[
= \left( \frac{4^4}{4} \right) - \left( \frac{0^4}{4} \right) = \frac{256}{4} - 0 = 64
\]
Step 3: Scale by the pre-integral coefficient.
Multiply the integrated value by the fraction outside:
\[
a_0 = \frac{1}{4} \times 64 = 16
\]
This gives $a_0 = 16$, which matches Option (C).