2018
DOI: 10.1002/dac.3720
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Error performance of Uncoded Space Time Labelling Diversity in spatially correlated Nakagami‐q channels

Abstract: Summary Greater spectral efficiency has recently been achieved for Uncoded Space Time Labelling Diversity (USTLD) systems by increasing the number of antennas in the transmit antenna array. However, due to constrained physical space in hardware, the use of more antennas can lead to degradation in error performance due to correlation. Thus, this paper studies the effects of spatial correlation on the error performance of USTLD systems. The union bound approach, along with the Kronecker correlation model, is use… Show more

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Cited by 10 publications
(30 citation statements)
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“…The N R × 1 vector h t , i , t , i ∈ [1:2], represents the multipath fading experienced by the symbol transmitted from antenna i during time slot t . The fading is assumed to follow a uniform phase distribution and a Nakagami‐ q amplitude distribution, the probability density function for which is given by fxfalse(xfalse)=x()1+q2qexp()x2()1+q224q2I0()x2false(1q4false)4q2, where x is the fading amplitude, I 0 (·) is the modified zeroth‐order Bessel function of the first kind, and the fading parameter, q , is the energy ratio of the quadrature component of the fading to its in‐phase component and should be in the range 0 ≤ q ≤ 1. The Nakagami‐ q fading model provides a good fit for modelling signal propagation in satellite transmissions subjected to strong ionospheric scintillation .…”
Section: System Modelmentioning
confidence: 99%
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“…The N R × 1 vector h t , i , t , i ∈ [1:2], represents the multipath fading experienced by the symbol transmitted from antenna i during time slot t . The fading is assumed to follow a uniform phase distribution and a Nakagami‐ q amplitude distribution, the probability density function for which is given by fxfalse(xfalse)=x()1+q2qexp()x2()1+q224q2I0()x2false(1q4false)4q2, where x is the fading amplitude, I 0 (·) is the modified zeroth‐order Bessel function of the first kind, and the fading parameter, q , is the energy ratio of the quadrature component of the fading to its in‐phase component and should be in the range 0 ≤ q ≤ 1. The Nakagami‐ q fading model provides a good fit for modelling signal propagation in satellite transmissions subjected to strong ionospheric scintillation .…”
Section: System Modelmentioning
confidence: 99%
“…The Nakagami‐ q fading model provides a good fit for modelling signal propagation in satellite transmissions subjected to strong ionospheric scintillation . Furthermore, Nakagami‐ q allows more insight into the worst‐case error performance of the system and is thus used ahead of the more common Rayleigh fading model . The fading channels are assumed to be frequency flat and may be either fast fading or quasi‐static over the duration of the two time slots.…”
Section: System Modelmentioning
confidence: 99%
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