Point spread function characteristics analysis of the wavefront coding system
Most of the previous imaging characteristics analysis of the wavefront coding system has been carried out within the frequency domain. In this paper, the stationary phase method is employed to perform the analysis within the spatial domain. The approximate expression of point spread function (PSF) i...
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Published in | Optics express Vol. 15; no. 4; pp. 1543 - 1552 |
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Main Authors | , , , , |
Format | Journal Article |
Language | English |
Published |
United States
19.02.2007
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Abstract | Most of the previous imaging characteristics analysis of the wavefront coding system has been carried out within the frequency domain. In this paper, the stationary phase method is employed to perform the analysis within the spatial domain. The approximate expression of point spread function (PSF) in the presence of defocus aberration is derived for the system with a cubic phase mask, which shows a good agreement with the Fast Fourier Transform (FFT) approach. Based on this, the PSF characteristics are analyzed in terms of the boundaries, oscillations and sensitivities to defocus, astigmatism and coma. |
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AbstractList | Most of the previous imaging characteristics analysis of the wavefront coding system has been carried out within the frequency domain. In this paper, the stationary phase method is employed to perform the analysis within the spatial domain. The approximate expression of point spread function (PSF) in the presence of defocus aberration is derived for the system with a cubic phase mask, which shows a good agreement with the Fast Fourier Transform (FFT) approach. Based on this, the PSF characteristics are analyzed in terms of the boundaries, oscillations and sensitivities to defocus, astigmatism and coma. |
Author | Zhao, Tingyu Yu, Feihong Ye, Zi Chen, Yanping Zhang, Wenzi |
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BackLink | https://www.ncbi.nlm.nih.gov/pubmed/19532386$$D View this record in MEDLINE/PubMed |
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CitedBy_id | crossref_primary_10_1364_OE_21_029523 crossref_primary_10_1016_j_optcom_2008_05_046 crossref_primary_10_1145_2503144 crossref_primary_10_1364_AO_49_006893 crossref_primary_10_4028_www_scientific_net_AMM_333_335_1591 crossref_primary_10_1364_OL_32_001220 crossref_primary_10_1016_j_optcom_2019_125121 crossref_primary_10_1111_j_1365_2966_2011_18385_x crossref_primary_10_7498_aps_61_074207 crossref_primary_10_1016_j_optcom_2013_02_033 crossref_primary_10_1088_1674_1056_ac560c crossref_primary_10_1016_j_ins_2011_09_026 crossref_primary_10_1364_OL_36_004647 crossref_primary_10_1364_OE_22_018668 crossref_primary_10_1364_OL_470949 crossref_primary_10_1016_j_optlaseng_2010_03_008 crossref_primary_10_1364_AO_55_007009 crossref_primary_10_1364_OE_17_006245 crossref_primary_10_1080_09500341003615683 crossref_primary_10_1117_1_3050348 crossref_primary_10_1364_AO_47_005893 crossref_primary_10_1364_OE_20_002408 crossref_primary_10_1016_j_optlastec_2012_08_022 crossref_primary_10_1364_AO_50_003337 |
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