Step 1: Consider a real-valued signal.
Let $x(t)$ be a real-valued time-domain signal with Fourier transform $X(\omega)$. Step 2: Apply Fourier symmetry property.
For real signals, the Fourier transform satisfies the conjugate symmetry condition:
\[
X(-\omega) = X^*(\omega)
\] Step 3: Interpretation of symmetry.
This property is known as conjugate symmetry and is characteristic of real-valued signals. Step 4: Eliminate incorrect options.
Odd or even symmetry alone is insufficient to describe $X(\omega)$. Step 5: Final conclusion.
Therefore, the Fourier transform of a real-valued signal has conjugate symmetry.