The Infrared &Amp; Electro-Optical Systems Handbook, Vol. 2: Atmospheric Propagation of Radiation 1993
DOI: 10.1117/3.2543821.ch2
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Propagation through Atmospheric Optical Turbulence

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Cited by 50 publications
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“…the signal from monostatic LGS can be used to correct for the "global" tilt of the wavefront in telescopes. Moreover, as estimates show, the magnitude of the measured value of such residual jitter will at least be comparable in magnitude to the LGS signal when using a polychromatic reference star 6 .…”
Section: Analytical and Numerical Calculationsmentioning
confidence: 88%
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“…the signal from monostatic LGS can be used to correct for the "global" tilt of the wavefront in telescopes. Moreover, as estimates show, the magnitude of the measured value of such residual jitter will at least be comparable in magnitude to the LGS signal when using a polychromatic reference star 6 .…”
Section: Analytical and Numerical Calculationsmentioning
confidence: 88%
“…We perform numerical calculations. The model of the turbulence profile of the structural constant of the refractive index of the atmosphere HV 5/7 was used in the calculations 6 . Table 2 shows the results of numerical calculation the magnitude of the signal jitter of the LGS image when working according to the monostatic scheme for different heights of LGS.…”
Section: Analytical and Numerical Calculationsmentioning
confidence: 99%
“…Then, the temperature structure parameter 𝐴𝐴 𝐴𝐴 2 𝑇𝑇 is extracted, similarly to Equation 7. Using the pressure and temperature from the radiosonde observations, the temperature structure parameter is finally converted to the refractive index structure parameter 𝐴𝐴 𝐴𝐴 2 𝑛𝑛 thanks to Beland (1993):…”
Section: Application To T-rex Thermosonde Measurements At Three River...mentioning
confidence: 99%
“…Then, the temperature structure parameter CT2 ${C}_{T}^{2}$ is extracted, similarly to Equation . Using the pressure and temperature from the radiosonde observations, the temperature structure parameter is finally converted to the refractive index structure parameter Cn2 ${C}_{n}^{2}$ thanks to Beland (1993): Cn20.22em=0.22emnT20.22emCT20.22em=0.22em79×106pT220.22emCT2, ${C}_{n}^{2}\,=\,{\left(\frac{\partial n}{\partial T}\right)}^{2}\,{C}_{T}^{2}\,=\,{\left(79\times 1{0}^{-6}\frac{p}{{T}^{2}}\right)}^{2}\,{C}_{T}^{2},$ with p in hectopascal, T in kelvin and the refractive index expression coming from Equation .…”
Section: Validation Of the Cn2 ${C}_{n}^{2}$ Models Through Data Anal...mentioning
confidence: 99%
“…For a slant path, where C n 2 is a function of height, the path-integrated transverse coherence length ρ 0 along the path length L, where L = H⋅sec β with zenith angle β, is given for a spherical wave by 5 : for downward looking case (sensor at height H, source at the ground)…”
Section: Turbulence Modulation Transfer Function Mtf and Point Spread...mentioning
confidence: 99%