(a) $x_{CM} = \frac{\int_{}^{}{xdm}}{\int_{}^{}{dm}}$
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If $n = 0$
Then $x_{CM} = \frac{L}{2}$
As $n$ increases, the centre of mass shift away from $x = \frac{L}{2}$ which only option (a) is satisfying.
Alternately, you can use basic concept.
$x_{CM} = \frac{\int_{0}^{L}{k\left( \frac{x}{L} \right)^{n}} \times xdx}{\int_{0}^{L}{k\left( \frac{x}{L} \right)^{n}dx}}$
$= L\left\lbrack \frac{n + 1}{n + 2} \right\rbrack$