Step 1: Properties of Fourier transform.
Fourier transform symmetry properties relate the nature of $x(t)$ to $X(\omega)$. Step 2: Given condition.
The signal $x(t)$ is real and odd. Step 3: Apply known Fourier properties.
For a real and odd time-domain signal, the Fourier transform is purely imaginary and odd. Step 4: Verification of options.
Only option (B) satisfies both conditions: imaginary and odd. Step 5: Final conclusion.
Thus, $X(\omega)$ is an imaginary and odd function of $\omega$.