2013
DOI: 10.1109/twc.2013.050613.120325
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Analytical Modeling of Uplink Cellular Networks

Abstract: Abstract-Cellular uplink analysis has typically been undertaken by either a simple approach that lumps all interference into a single deterministic or random parameter in a Wynertype model, or via complex system level simulations that often do not provide insight into why various trends are observed. This paper proposes a novel middle way using point processes that is both accurate and also results in easy-to-evaluate integral expressions based on the Laplace transform of the interference. We assume mobiles an… Show more

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Cited by 439 publications
(493 citation statements)
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“…It should be noted that the random variables {R z } z∈Z are identically distributed but not independent in general. This dependence is induced by the restriction of having one user served per-BS-per channel, i.e., the coupling of the BS and served user per channel point processes [13,16,23]. Here, we demonstrate that this dependence is weak which motivates our independence assumption for {R z } z∈Z .…”
Section: Distribution Of R Zmentioning
confidence: 61%
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“…It should be noted that the random variables {R z } z∈Z are identically distributed but not independent in general. This dependence is induced by the restriction of having one user served per-BS-per channel, i.e., the coupling of the BS and served user per channel point processes [13,16,23]. Here, we demonstrate that this dependence is weak which motivates our independence assumption for {R z } z∈Z .…”
Section: Distribution Of R Zmentioning
confidence: 61%
“…We consider that LOS probability function p(R) = e −βR , where 1/β = 141.4 m. The antenna gain pattern of a BS is assumed to be characterized with M r = 10 dB, m r = −10 dB, and θ r = 30 • , while that of a user is assumed to be characterized with M t = 10 dB, m t = −10 dB, and θ t = 90 • . For comparison purpose, we have also included the conventional stochastic geometry analysis of the uplink channel in [13] that does not differentiate between LOS and NLOS transmission and assumes smallscale Rayleigh fading between the users and BSs (i.e., N L = N N = 1). Note that only one pathloss exponent is defined in [13] and is denoted here as α = α N .…”
Section: Numerical Results and Discussionmentioning
confidence: 99%
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