For the Bessel function \( J_0(x) \), the Laplace transform \( Y(s) \) satisfies the differential equation:
\[
\frac{dY}{ds} + \frac{sY}{s^2 + 1} = 0, \quad s > 0.
\]
This is a standard result for the Laplace transform of \( J_0(x) \).
Now, let’s examine the options:
Option A: \( \frac{dY}{ds} + \frac{2sY}{s^2 + 1} = 0 \)
This is incorrect because the coefficient \( 2s \) is not correct.
Option B: \( \frac{dY}{ds} + \frac{2sY}{s^2 + 1} = 0 \)
This is also incorrect for the same reason as option A.
Option C: \( \frac{dY}{ds} - \frac{sY}{s^2 + 1} = 0 \)
This is incorrect because the sign before the second term is wrong.
Option D: \( \frac{dY}{ds} + \frac{sY}{s^2 + 1} = 0 \)
This is the correct equation, matching the known differential equation for the Laplace transform of \( J_0(x) \).
Thus, Option D is the correct answer.
\[
\boxed{D} \quad \frac{dY}{ds} + \frac{sY}{s^2 + 1} = 0, \, s > 0
\]