2016
DOI: 10.1109/twc.2016.2522419
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Performance Analysis of Large Multiuser MIMO Systems With Space-Constrained 2-D Antenna Arrays

Abstract: Massive Multiple-Input-Multiple-Output (MIMO) systems deploying a large number of antennas at the base station (BS) have been shown to produce high spectral and energy efficiency (EE) under the assumptions of increasing BS physical space and critical antenna spacing. We examine the deployment of massive MIMO systems and resulting EE with a more realistic scenario considering a 2D rectangular array with increasing antenna elements within a fixed physical space. Mutual coupling and correlation among the BS anten… Show more

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Cited by 66 publications
(67 citation statements)
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“…A proof-of-concept array was constructed and tests were performed that validate the reported design principles and simulation results. M. (5G) communication systems [1,2]. It has several unique advantages that arise from its ability to facilitate the presence of additional signal channels instead of requiring the use of extra frequency spectrum or power.…”
mentioning
confidence: 99%
See 1 more Smart Citation
“…A proof-of-concept array was constructed and tests were performed that validate the reported design principles and simulation results. M. (5G) communication systems [1,2]. It has several unique advantages that arise from its ability to facilitate the presence of additional signal channels instead of requiring the use of extra frequency spectrum or power.…”
mentioning
confidence: 99%
“…(5G) communication systems [1,2]. It has several unique advantages that arise from its ability to facilitate the presence of additional signal channels instead of requiring the use of extra frequency spectrum or power.…”
mentioning
confidence: 99%
“…For any two antenna elements n and n , where θ ∈ [0, π) is an arbitrary elevation angle and p Θ (θ) is constant over [0, π), we have θ exp (j2πdz n,n cos (θ)) J 0 (2πdxy n,n sin (θ)) p Θ (θ) × sin (θ) dθ = A π 0 exp (j2πdz n,n cos (θ)) × J 0 (2πdxy n,n sin (θ)) p Θ (θ) sin (θ) dθ, (32) where A is the scaling constant to make sure the elevation PDF integrates to 1. To calculate A, we have 1 = exp (−j2πdz n,n u) I 0 j2πdxy n,n 1 − u 2 du (34) = sinh (j2πdz n,n ) 2 + (j2πdxy n,n ) 2 (j2πdz n,n ) 2 + (j2πdxy n,n )…”
Section: Appendix B Proof Of Theoremmentioning
confidence: 99%
“…This effect can be critical in physically constrained scenarios, where a large number of antennas are packed in fixed physical structures such that inter-antenna spacings are shorter than half a wavelength, as studied in [17], [32]. Specifically, [32] shows a considerable decrease in the achievable rates of microwave systems due to MC. Overall, the influence of both MC and array topology in the mmWave band still remains an open problem [13].…”
Section: Introductionmentioning
confidence: 99%
“…In [1] it was stated that very large antenna arrays may not be useful when the antennas are deployed within a fixed physical space. However, the smaller wavelengths of mmWave bands will make it possible to rig a large number of antennas in constrained physical spaces.…”
Section: Introductionmentioning
confidence: 99%