Two limiting-case algorithms have previously been proposed for hologra
phically imaging atoms near surfaces using photoelectron diffraction d
ata and other diffraction data associated with electron emission:(i) a
phased sum of Fourier transforms of scanned-angle data taken at sever
al energies from Barton, (ii) and a phased sum of Fourier transforms o
f scanned-energy data taken along several directions due to Tong et al
. We first point out that both methods are equivalent three-dimensiona
l transforms in the wave Vector k of the emitted electron, differing o
nly in the way they sample k-space. A continuum of different sampling
densities in the direction and magnitude of k exists in such holograph
y, spanning the two limits previously discussed. An additional variant
on these methods involves using only a small cone of data in k-space
for each transform. Using model diffraction calculations for localized
electron emission (e.g., core photoelectron emission) from Cu(001) cl
usters, we have explored the full range of k-space sampling possible,
and find that optimum image quality is expected for choices intermedia
te between the extreme limits of scanned-angle or scanned-energy. Gene
ral rules for optimizing image quality for a given data-set range are
also discussed, and used to evaluate the sampling choices made in some
prior experimental studies.