{"title":"Measurement of a Non-Kolmogorov Structure Function","authors":"T. Nicholls, N. Wooder, C. Dainty","doi":"10.1364/adop.1996.awd.15","DOIUrl":null,"url":null,"abstract":"The structure function of atmospheric phase fluctuations is defined as follows: A generalised model for the structure function of phase is: ℛ\n 0\n is related to the size of the long-exposure image formed by a large-aperture telescope, while γ\n ß\n is a parameter which depends on ß and on the precise definition of ℛ\n 0\n The widely-used Kolmogorov model of refractive index fluctuations [1] predicts a value of 11/3 for ß; in this case, with the appropriate definition, ℛ0 is equivalent to r0, the Fried parameter [2], Under the Kolmogorov assumption, the parameter r0 entirely describes the time-averaged statistics of the phase fluctuations. A knowledge of r0 can be used, for example, to predict how the energy in the phase fluctuations is distributed between the Zernike modes.","PeriodicalId":256393,"journal":{"name":"Adaptive Optics","volume":"35 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1900-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Adaptive Optics","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1364/adop.1996.awd.15","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
Abstract
The structure function of atmospheric phase fluctuations is defined as follows: A generalised model for the structure function of phase is: ℛ
0
is related to the size of the long-exposure image formed by a large-aperture telescope, while γ
ß
is a parameter which depends on ß and on the precise definition of ℛ
0
The widely-used Kolmogorov model of refractive index fluctuations [1] predicts a value of 11/3 for ß; in this case, with the appropriate definition, ℛ0 is equivalent to r0, the Fried parameter [2], Under the Kolmogorov assumption, the parameter r0 entirely describes the time-averaged statistics of the phase fluctuations. A knowledge of r0 can be used, for example, to predict how the energy in the phase fluctuations is distributed between the Zernike modes.