Turbulence-induced fading probability in coherent optical communication through the atmosphere.

To assess the coherent detection of an optical signal perturbed by atmospheric turbulence, the loss in the mean signal-to-noise ratio (SNR) is usually invoked although it constitutes a limited description of the signal fluctuations. To produce statistical distributions of the SNR, we generate random optical fields. A 5/3-power law for the phase structure function is considered. The benefit of a wavefront tilt correction is assessed. Based on the 1%-probability fade, an optimum receiver size is found. For phase fluctuations only, a similarity between the signal distribution and the beta distribution is observed. Phase and amplitude are assumed independent, and the influence of amplitude perturbations is assessed with a scintillation index of 2. Turbulence impairments are compared for a coherent receiver and a direct-detection receiver.

[1]  Isaac Freund,et al.  Speckle spots ride phase saddles sidesaddle , 1995 .

[2]  Benjamin L. McGlamery,et al.  Computer Simulation Studies Of Compensation Of Turbulence Degraded Images , 1976, Other Conferences.

[3]  J. Conan,et al.  Wave-front temporal spectra in high-resolution imaging through turbulence , 1995 .

[4]  J. Strohbehn Line-of-sight wave propagation through the turbulent atmosphere , 1968 .

[5]  James H. Churnside,et al.  Experimental evaluation of log-normally modulated Rician and IK models of optical scintillation in the atmosphere , 1989 .

[6]  L C Andrews,et al.  Experimental verification and theory for an eight-element multiple-aperture equal-gain coherent laser receiver for laser communications. , 1998, Applied optics.

[7]  A. Glindemann RELEVANT PARAMETERS FOR TIP-TILT SYSTEMS OF LARGE TELESCOPES , 1997 .

[8]  Jennifer C. Ricklin,et al.  Performance loss factors for optical communication through clear air turbulence , 2004, SPIE Optics + Photonics.

[9]  D. Kouznetsov,et al.  Simulations of turbulence-induced phase and log-amplitude distortions. , 1997, Applied optics.

[10]  R. Lane,et al.  Fast simulation of a kolmogorov phase screen. , 1999, Applied optics.

[11]  David L Fried,et al.  Evaluation of the performance of Hartmann sensors in strong scintillation. , 2002, Applied optics.

[12]  Dirk Giggenbach,et al.  142 km, 5.625 Gbps free-space optical link based on homodyne BPSK modulation , 2006, SPIE LASE.

[13]  J. Churnside,et al.  Signal current probability distribution for optical heterodyne receivers in the turbulent atmosphere. 1: theory. , 1978, Applied Optics.

[14]  D. L. Fried,et al.  Optical heterodyne detection of an atmospherically distorted signal wave front , 1967 .

[15]  Hennes Henniger,et al.  Measurements of the beam-wave fluctuations over a 142 km atmospheric path , 2006, SPIE Optics + Photonics.

[16]  Larry C. Andrews,et al.  Special Functions Of Mathematics For Engineers , 2022 .

[17]  L. Andrews,et al.  Strehl ratio and scintillation theory for uplink Gaussian-beam waves: beam wander effects , 2006 .

[18]  John E. Kaufmann Performance limits of high-rate space-to-ground optical communications through the turbulent atmospheric channel , 1995, Photonics West.

[19]  V. I. Tatarskii The effects of the turbulent atmosphere on wave propagation , 1971 .

[20]  L. Andrews,et al.  Laser Beam Propagation Through Random Media , 1998 .

[21]  Robert Lange,et al.  Homodyne BPSK-based optical inter-satellite communication links , 2007, SPIE LASE.

[22]  I. Miller Probability, Random Variables, and Stochastic Processes , 1966 .

[23]  K A Winick,et al.  Atmospheric turbulence-induced signal fades on optical heterodyne communication links. , 1986, Applied optics.

[24]  D. Fried,et al.  Branch cuts in the phase function. , 1992, Applied optics.

[25]  Guang-ming Dai Modal compensation of atmospheric turbulence with the use of Zernike polynomials and Karhunen–Loève functions , 1995 .