A generalized Rice channel for modeling mobile satellite link

Jaafar, I.; Youssef, Néji; Boujemâa, Hatem

doi:10.1109/isccsp.2004.1296342

Cited by 3 publications

(3 citation statements)

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“…The probability density function (pdf) of the Rice-Hoyt envelope X = A + m 1 2 +m 2 2 and phase Θ = arctan ((μ 2 (t))/(A| + |μ 1 (t))) are given by [8] …”

Section: First-order Statisticsmentioning

confidence: 99%

“…Further, as found from the V2V measurements (antennas inside car) results in 5 GHz frequency band [31,32], the m value of each tap of the channel model described is found to be less than unity (0.75-0.89), which from [12] corresponds to the value of q (0.5-0.707). and phase Θ = arctan ((μ 2 (t))/(A| + |μ 1 (t))) are given by [8]…”

Section: Channel Modelmentioning

confidence: 99%

“…Several composite fading models combining the short-and long-term models including Nakagami-lognormal [3], Suzuki [6] and Rice-lognormal [7] have been proposed. Furthermore during the past decade, the statistical properties of the generalised Rice [8], Extended generalised Rice [9], generalised Rice-Hoyt [10], Nakagami-m fading [11] have been described. The second-order statistics of Nakagami-Hoyt channel has been derived in [12].…”

Section: Introductionmentioning

confidence: 99%

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Modelling and simulation of a generalised vehicle‐to‐vehicle fading channel

Akram

Sheikh

2013

IET Communications

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This study presents statistical properties of the vehicle-to-vehicle Nakagami-Hoyt channel model with diffused line of sight (LOS) under isotropic condition. The envelope and phase probability density functions, spatial-time autocorrelation function, the power spectral density, level crossing rate, the average duration of fade, squared time autocorrelation function and mean-square error of time autocorrelation function of the Nakagami-Hoyt channel have been derived under the assumption that both the transmitter and receiver are mobile having omnidirectional antennas and a diffused LOS component is present. The model has been validated using the inverse fast Fourier transform-based simulator. The simulator and analytical results corroborate.

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“…The probability density function (pdf) of the Rice-Hoyt envelope X = A + m 1 2 +m 2 2 and phase Θ = arctan ((μ 2 (t))/(A| + |μ 1 (t))) are given by [8] …”

Section: First-order Statisticsmentioning

confidence: 99%