1995
DOI: 10.1117/12.210938
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<title>Experimental realization of the laser telescope with overall compensation for distortions via phase conjugation</title>

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Cited by 5 publications
(2 citation statements)
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“…The basic scheme for the holographic correction of an aberrated reflecting primary is shown in Figure 1, with various alternative configurations discussed in previous work [2][3][4][5][6][7][8][9] . A distant source of laser illumination is incident on an aberrated primary mirror, with the focused light gathered by a secondary element, which forms a demagnified image of the mirror surface onto the plane of the hologram [ Fig.…”
Section: Introductionmentioning
confidence: 99%
“…The basic scheme for the holographic correction of an aberrated reflecting primary is shown in Figure 1, with various alternative configurations discussed in previous work [2][3][4][5][6][7][8][9] . A distant source of laser illumination is incident on an aberrated primary mirror, with the focused light gathered by a secondary element, which forms a demagnified image of the mirror surface onto the plane of the hologram [ Fig.…”
Section: Introductionmentioning
confidence: 99%
“…Phase holograms were recorded using a continuous-wave, frequency-doubled Nd:YAG laser (λ = 532nm) on bleached Agfa 8E56 plate film. Typically phase holograms produced in such a medium can be expected to be 70-90% efficient [8][9][10][11][12] , but due to the effect of low-frequency vibrations and air turbulence on the membrane, the actual efficiency was an order of magnitude lower than this.…”
Section: Holographic Correctionmentioning
confidence: 99%