  Polarized synchrotron emission from multiple Faraday depths can be separated
by calculating the complex Fourier transform of the Stokes' parameters as a
function of the wavelength squared, known as Faraday Synthesis. As commonly
implemented, the transform introduces an additional term $\lambda_0^2$, which
broadens the real and imaginary spectra, but not the amplitude spectrum. We use
idealized tests to investigate whether additional information can be recovered
with a clean process restoring beam set to the narrower width of the peak in
the real ``full" resolution spectrum with $\lambda_0^2=0$. We find that the
$\lambda_0^2$ choice makes no difference, except for the use of a smaller
restoring beam. With this smaller beam, the accuracy and phase stability are
unchanged for single Faraday components. However, using the smaller restoring
beam for multiple Faraday components we find a) better discrimination of the
components, b) significant reductions in blending of structures in tomography
images, and c) reduction of spurious features in the Faraday spectra and
tomography maps. We also discuss the limited accuracy of information on scales
comparable to the width of the amplitude spectrum peak, and note a clean-bias,
reducing the recovered amplitudes. We present examples using MeerKAT L-band
data. We also revisit the maximum width in Faraday depth to which surveys are
sensitive, and introduce the variable $W_{max}$, the width for which the power
drops by a factor of 2. We find that most surveys cannot resolve continuous
Faraday distributions unless the narrower full restoring beam is used.
