2013
DOI: 10.1049/el.2013.2768
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Exact and asymptotic PEP derivations for various quasi‐orthogonal space–time block codes

Abstract: Insightful closed-form formulas for the exact pairwise error probability (PEP) of quasi-orthogonal space-time block codes in Rayleigh fading channels are presented. In addition, simple asymptotic expressions are proposed, from which the achievable asymptotic diversity orders are easily determined in the high signal-to-noise ratio regime. Finally, comparing analytical and simulation results, the accuracy of the derived analytical formulas is validated.

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Cited by 4 publications
(5 citation statements)
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“…The result for correlated PEP (23) is of a similar form to that of the uncorrelated PEP (16). The difference between these 2 expressions is that the second argument of MGF M k is the squared Euclidean distance d k ðL;LÞ 2 for the uncorrelated PEP, whereas it is the eigenvalue product ν j η k for the correlated PEP.…”
Section: Correlated Nakagami-q Error Performancementioning
confidence: 82%
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“…The result for correlated PEP (23) is of a similar form to that of the uncorrelated PEP (16). The difference between these 2 expressions is that the second argument of MGF M k is the squared Euclidean distance d k ðL;LÞ 2 for the uncorrelated PEP, whereas it is the eigenvalue product ν j η k for the correlated PEP.…”
Section: Correlated Nakagami-q Error Performancementioning
confidence: 82%
“…The 2 × N r USTLD model was recently extended to consider any arbitrary N t transmit antennas by Patel et al 14 It is noted that N t × N r USTLD systems are comparable to existing quasi-orthogonal STBC (Q-STBC) systems with more than 2 transmit antennas. [15][16][17] The use of N t > 2 transmit antennas allows Q-STBC systems to achieve more transmit antenna diversity, improving error performance. However, Q-STBC systems use more than 2 time slots to transmit the same binary information.…”
Section: Introductionmentioning
confidence: 99%
“…and by adopting the derivation procedure in [5], the following closedform formula can be derived as [7, (3.211)]: As a special case with u = v ≠ 0 (compare p = q), (9) can be further simplified as [5] is achieved by the PS-QSTBC in Rayleigh fading channels, as can be seen from the power exponent, which is due to the fact that the asymptotic diversity order, d ∞ , can be expressed as…”
Section: Qstbc With Power Scalingmentioning
confidence: 99%
“…Hence, we have Pfalse(Sfalse→bold-italicSfalse^false)=1π0π/21+γsu4sin2θ1+γsv4sin2θ2Nrnormaldθand by adopting the derivation procedure in [5], the following closed‐form formula can be derived as [7, (3.211)]: right leftthickmathspace.5emscriptP(bold-italicSS^)=B(4Nr+12,12)2π1+p2Nr1+q2Nr×F112;thinmathspace2Nnormalr,thinmathspace2Nnormalr;thinmathspace4Nnormalr+1;thinmathspace11+p,11+qwhere B ( · , · ) is the beta function [7, (8.380)], F 1 ( · ; · , · ; · ; · , · ) is the Appell hypergeometric function [8, (07.36.02.0001.01)], γ s u /4 = p and γ s v /4 = q . As a special case with u = v ≠ 0...…”
Section: Exact Pep Derivation Of Ps‐qstbcmentioning
confidence: 99%
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