When the focal depth is required to be much larger than the wavelength
, lambda, the effective NA of the beam with optimal resolution is much
less than unity. An aperture that is much larger than this beam's foo
tprint is then of no consequence. Such beams that maximize the mean en
circled energy fraction within a cylindrical focal region are shown to
depend on only a single parameter, omega, that is proportional to the
ratio of the square of the cylinder's radius to the product of its le
ngth and lambda. A linear combination of Hermite- or Laguerre-Gaussian
modes is used to represent these fields in two and three dimensions,
respectively. For small omega, the results are compared both to asympt
otic expansions and to optimal Gaussian and Bessel-Gauss beams. (C) 19
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