  We study the connection between STFT multipliers $A^{g_1,g_2}_{1\otimes m}$
having windows $g_1,g_2$, symbols $a(x,\omega)=(1\otimes
m)(x,\omega)=m(\omega)$, $(x,\omega)\in\mathbb{R}^{2d}$, and the Fourier
multipliers $T_{m_2}$ with symbol $m_2$ on $\mathbb{R}^d$. We find sufficient
and necessary conditions on symbols $m,m_2$ and windows $g_1,g_2$ for the
equality $T_{m_2}= A^{g_1,g_2}_{1\otimes m}$. For $m=m_2$ the former equality
holds only for particular choices of window functions in modulation spaces,
whereas it never occurs in the realm of Lebesgue spaces. In general, the STFT
multiplier $A^{g_1,g_2}_{1\otimes m}$, also called localization operator,
presents a smoothing effect due to the so-called two-window short-time Fourier
transform which enters in the definition of $A^{g_1,g_2}_{1\otimes m}$. As a
by-product we prove necessary conditions for the continuity of anti-Wick
operators $A^{g,g}_{1\otimes m}: L^p\to L^q$ having multiplier $m$ in weak
$L^r$ spaces. Finally, we exhibit the related results for their discrete
counterpart: in this setting STFT multipliers are called Gabor multipliers
whereas Fourier multiplier are better known as linear time invariant (LTI)
filters.
