Skip to main content
Top
Published in: EURASIP Journal on Wireless Communications and Networking 1/2009

Open Access 01-12-2009 | Research Article

A Multiuser MIMO Transmit Beamformer Based on the Statistics of the Signal-to-Leakage Ratio

Authors: Batu K. Chalise, Luc Vandendorpe

Published in: EURASIP Journal on Wireless Communications and Networking | Issue 1/2009

Activate our intelligent search to find suitable subject content or patents.

search-config
loading …

Abstract

A multiuser multiple-input multiple-output (MIMO) downlink communication system is analyzed in a Rayleigh fading environment. The approximate closed-form expressions for the probability density function (PDF) of the signal-to-leakage ratio (SLR), its average, and the outage probability have been derived in terms of the transmit beamformer weight vector. With the help of some conservative derivations, it has been shown that the transmit beamformer which maximizes the average SLR also minimizes the outage probability of the SLR. Computer simulations are carried out to compare the theoretical and simulation results for the channels whose spatial correlations are modeled with different methods.

1. Introduction

The capacity of a wireless cellular system is limited by the mutual interference among simultaneous users. Using multiple antenna systems, and in particular, the adaptive beamforming, this problem can be minimized, and the system capacity can be improved. In recent years, the optimum downlink beamforming problem (including power control) has been extensively studied in [13] where the signal-to-interference-plus-noise ratio (SINR) is used as a quality of service (QoS) criterion. After it has been found that the multiple-input multiple-output (MIMO) techniques significantly enhance the performance of wireless communication systems [4, 5], the joint optimization of the transmit and receive beamformers [6] has also been investigated for MIMO systems. Motivated by the fact that the optimum transmit beamformers [13] and the joint optimum transmit-receive beamformers [6] can be obtained only iteratively due to the coupled nature of the corresponding optimization problems, recently, the concept of leakage and subsequently the signal-to-leakage-plus-noise ratio (SLNR) as a figure of merit have been introduced in [7, 8]. (Note that SLNR as a performance criterion has been considered in [911] for multiple-input-single-output (MISO) systems.) Although the latter approach only gives suboptimum solutions, it leads to a decoupled optimization problem and admits closed-form solutions for downlink beamforming in multiuser MIMO systems.
While investigating multiuser systems from a system level perspective, in many cases, the outage probability has also been widely used as a QoS parameter. The closed-form expressions of the outage probability with equal gain and optimum combining have been derived in [12, 13], respectively, in a flat-fading Rayleigh environment with cochannel interference. The latter work has been extended in [14] to a Rician-Rayleigh environment where the desired signal and interferers are subject to Rician and Rayleigh fading, respectively. However, in all of the above-mentioned papers, investigations have been limited to the derivations of the outage probability expressions for specific types of receivers. The outage probability of the signal-to-interference ratio is used to formulate the optimum power control problem for interference limited wireless systems in [15, 16] where the total transmit power is minimized subject to outage probability constraints. However, both of the these works [15, 16] are limited to systems with single antenna at transmitters and receivers.
In this paper, we consider the downlink of a multiuser MIMO wireless communication system in a Rayleigh fading environment. The base station (BS) communicates with several cochannel users in the same time and frequency slots. In our method, we use the average signal-to-leakage ratio (SLR) and the outage probability of SLR as performance metrics which are based on the concept of leakage power [7, 8]. In particular, the novelty of our work lies on the facts that we first derive an approximation of the statistical distribution of SLR [7] for each cochannel user of the MIMO system in terms of transmit beamforming weight vector. Second, the approximate closed-form expression for the outage probability of SLR is derived. Then, we obtain the solution for the transmit beamformer that minimizes the aforementioned outage probability. According to our best source of knowledge, this approach has not been previously considered for the multiuser MIMO downlink beamforming. With some conservative derivations, we also demonstrate that the beamformer which minimizes the outage probability is same as the one which maximizes the average SLR. Note that similar conclusion has been made in [17] where the downlink beamforming for multiuser MISO systems is analyzed using the SINR and its outage probability as the performance criteria. In contrast to [7], we consider that the BS has only the knowledge of the second-order statistics such as the covariance matrix of the downlink user-channels. The motivation behind this assumption is that the knowledge of instantaneous channel information can be available at the BS only through the feedback from users. The drawbacks of the feedback approach are the reduction of the system capacity because of the frequent channel usage required for the transmission of the feedback information from users to the BS, and inherent time delays, errors, and extra costs associated with such a feedback. Furthermore, if the channel varies rapidly, it is not reasonable to acquire the instantaneous feedback at the transmitter, because the optimal transmitter designed on the basis of previously acquired information becomes outdated quickly (see [18] and the references therein). Thus, we consider that no full-rate feedback information is available at the BS.
The remainder of this paper is organized as follows. The system model is presented in Section 2. The probability density function (PDF) of SLR, its mean, and the outage probability of SLR are derived in terms of the beamformer weight vector in Section 3. In Section 4, the transmit beamformer which maximizes the average SLR and minimizes the outage probability is obtained. In Section 5, analytical and numerical results are compared. Finally, conclusions are drawn in Section 6.
Notational conventions
Upper (lower) bold face letters will be used for matrices (vectors); https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq1_HTML.gif , https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq2_HTML.gif , https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq3_HTML.gif , https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq4_HTML.gif , https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq5_HTML.gif and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq6_HTML.gif denote the Hermitian transpose, mathematical expectation, https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq7_HTML.gif identity matrix, Euclidean norm, trace operator, and the space of https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq8_HTML.gif matrices with complex entries, respectively.

2. System Model

Consider a downlink multiuser scenario with a multi-antenna BS of https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq9_HTML.gif sensors communicating with https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq10_HTML.gif multi-antenna users. (If there are multiple BSs and they have also the channel information of users assigned to other BSs, the SLR-based method needs to be modified in such a way that each BS takes into account the power leaked by it to the users of other BSs. The necessary modifications, in our case, can be done with some straightforward steps.) The block diagram is shown in Figure 1. The signal transmitted by the BS is given by
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_Equ1_HTML.gif
(1)
where https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq11_HTML.gif and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq12_HTML.gif are, respectively, the signal stream and the transmit beamformer weight vector for https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq13_HTML.gif th user. It is assumed that https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq14_HTML.gif and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq15_HTML.gif for https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq16_HTML.gif (We consider equal power allocations to all users. Note that power control can be included in the design of beamformers by using a two-step approach, that is, by optimizing the beamformers first and then the powers or vice-versa [1, 2].) Moreover, following the spirit of [7], we consider that the beamformer weights are normalized, that is, https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq17_HTML.gif . Let https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq18_HTML.gif denote the number of receive antennas at https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq19_HTML.gif th user. The signal vector received by https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq20_HTML.gif th user is
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_Equ2_HTML.gif
(2)
where https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq21_HTML.gif is a constant that includes the effect of distance-dependent path loss factor and the distance-independent mean-channel power gain, https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq22_HTML.gif is the spatially correlated MIMO channel matrix, and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq23_HTML.gif denotes the additive noise. It is assumed that each user is surrounded by a large number of scatterers whereas the BS, which is generally located at larger heights from the ground level, does not observe rich scattering. In this scenario, the MIMO channel as seen from the user/BS is spatially uncorrelated/correlated. Thus, the https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq24_HTML.gif th MIMO channel can be given by replacing the receive correlation matrix with an identity matrix in the famous Kronecker-model [19] which turns into the following form: https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq25_HTML.gif , where the entries of https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq26_HTML.gif are assumed to be zero-mean circularly symmetric complex Gaussian (ZMCSCG) random variables with unit variance such that https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq27_HTML.gif , and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq28_HTML.gif represents the spatial correlation matrix at the BS corresponding to the https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq29_HTML.gif th user channel. It is important to emphasize here that the derivations for the SLR mean and SLR ouatge probability can be easily extended to double-sided correlated MIMO channels (including the user side correlation), and thus, our main results are also valid for such MIMO channels. Note that https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq30_HTML.gif are symmetric positive semidefinite matrices and are a function of the antenna spacing, average direction of arrival of the scattered signal from https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq31_HTML.gif th user, and the corresponding angular spread [20]. We invite our readers to have a look at [20] and the references therein for determining https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq32_HTML.gif . Furthermore, without loss of generality, the elements of https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq33_HTML.gif in (2) are considered to be ZMCSCG with the variance https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq34_HTML.gif , that is, https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq35_HTML.gif , where https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq36_HTML.gif denotes https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq37_HTML.gif identity matrix. Inserting (1) into (2) and applying the statistical expectation over signal and noise realizations, the SLNR for https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq38_HTML.gif th user can be expressed as [7]
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_Equ3_HTML.gif
(3)
Note that, here, https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq39_HTML.gif is the power of the desired signal for user https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq40_HTML.gif whereas https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq41_HTML.gif is the power of interference that is caused by user https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq42_HTML.gif on the signal received by some other user https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq43_HTML.gif . The leakage for user https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq44_HTML.gif is thus the total power leaked from this user to all other users which is https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq45_HTML.gif . The objective of beamformer is to make https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq46_HTML.gif as large as possible when compared to the leakage power https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq47_HTML.gif . (The performance of the beamformer can be boosted by taking into account the noise term https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq48_HTML.gif which acts as a diagonal loading factor [21].) The main motivation behind this approach is that it results into a decoupled optimization problem and provides analytical closed-form solutions (see [7, Sections I-III] for more information), though they are not optimal relative to the SINR criterion [13]. Moreover, the SLNR as a performance criterion also allows the BS to work more independently from the receivers since the BS does not need the knowledge of receive beamformer or in general receiver's operator. Similarly, each user performs beamforming or any other linear operations to recover its signal without depending on transmit beamforming vectors of other users. Let https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq49_HTML.gif th user uses a matched filter to recover its signal. The detected signal of this user can be given by https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq50_HTML.gif where https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq51_HTML.gif is the matched filter response. Then, using (1) and (2), https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq52_HTML.gif can be written as
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_Equ4_HTML.gif
(4)
Applying mathematical expectation with respect to independent realizations of signals and noise, the SINR for https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq53_HTML.gif th user is
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_Equ5_HTML.gif
(5)
It is considered that the transmitter (also the BS) does not know user's receiver, and thus, the SINR (5) is not available at the transmitter. In this case, the transmitter optimizes its beamforming vector to maximize the SLNR (3) thereby assisting the user's receiver in its task of improving the SINR (5). The latter fact can be verified numerically. Note that the beamformer based on maximization of (3) can also be designed for the cases where only the knowledge of second-order statistics of downlink channels is available at the BS. In such cases, the advantages are twofold; the BS and receivers can work in a distributed manner (since the criterion is SLNR), and the BS needs only a limited feedback information from the receivers. To facilitate the aforementioned scheme, we first analyze the statistics of SLNR (3) in the following section.

3. Average SLR and the Outage Probability

Using the notations https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq54_HTML.gif for all https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq55_HTML.gif , and assuming that the leakage power (The derivation of outage probability expression and its minimization become too involved if the noise power is not negligible. However, noting that the cellular systems such as UMTS with beamforming techniques can support a significant number of cochannel users per cell [21] (this number can be further increased if more scrambling codes can be allocated for each cell [22]), the assumption that the multiuser leakage power dominates the thermal noise power at each user is not a stringent one.) is large compared to the noise power, we get the SLR from (3) as
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_Equ6_HTML.gif
(6)
We first note that the rows of https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq56_HTML.gif are statistically independent, and each row has an https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq57_HTML.gif -variate complex Gaussian distribution with the mean vector https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq58_HTML.gif and the covariance matrix https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq59_HTML.gif . According to [23], in this case, https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq60_HTML.gif are complex Wishart distributed with the scaling matrix https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq61_HTML.gif and the degrees of freedom parameter https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq62_HTML.gif . For conciseness and simplified mathematical presentation, in the rest of this paper, we assume that https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq63_HTML.gif . Here, we also stress that our results can be easily extended to the general case where https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq64_HTML.gif are different. Mathematically, we can thus write https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq65_HTML.gif , where https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq66_HTML.gif represents the complex Wishart matrix of size https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq67_HTML.gif . Let us use the notations https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq68_HTML.gif and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq69_HTML.gif . According to the results of [14] and since https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq70_HTML.gif , we get https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq71_HTML.gif . We note that for any https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq72_HTML.gif , https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq73_HTML.gif , because https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq74_HTML.gif is a positive semidefinite matrix. Since https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq75_HTML.gif is a Chi-square distribution, the random variable https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq76_HTML.gif has the following PDF:
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_Equ7_HTML.gif
(7)
where https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq77_HTML.gif , https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq78_HTML.gif and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq79_HTML.gif is the Gamma function. Comparing the PDF of (7) to the standard form of Chi-square PDF [23], https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq80_HTML.gif can be alternatively expressed as
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_Equ8_HTML.gif
(8)
where https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq81_HTML.gif is the Chi-square distribution with degrees of freedom https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq82_HTML.gif . Using (8), https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq83_HTML.gif can be written as
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_Equ9_HTML.gif
(9)
It can be observed from (9) that https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq84_HTML.gif is a weighted sum of statistically independent Chi-square random variables, where the weights https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq85_HTML.gif since https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq86_HTML.gif are positive semidefinite. The exact and closed-form solution for the PDF of https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq87_HTML.gif is not known. However, according to [24] and the references therein, the PDF of https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq88_HTML.gif can be found by approximating https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq89_HTML.gif as a random variable with the Chi-square distribution having degrees of freedom https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq90_HTML.gif and the scaling factor https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq91_HTML.gif as
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_Equ10_HTML.gif
(10)
where https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq92_HTML.gif and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq93_HTML.gif can be determined by equating the first- and second-order moments of the left-and right-hand sides of relation (10). (This approximation is very accurate and widely adopted in statistics and engineering. The accuracy of the approximation will be confirmed later through numerical simulation results.) Evaluation of the first-order moment (mean) of the both sides of (10) gives
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_Equ11_HTML.gif
(11)
Similarly by equating the second-order moment (variance) of the both sides of (10), we get
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_Equ12_HTML.gif
(12)
Solving (11) and (12), https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq94_HTML.gif and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq95_HTML.gif can be expressed as
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_Equ13_HTML.gif
(13)
Like the PDF of https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq96_HTML.gif given in (7), the PDF of https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq97_HTML.gif is well known to be [23]
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_Equ14_HTML.gif
(14)
where again https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq98_HTML.gif . For the sake of better exposition, let https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq99_HTML.gif , where https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq100_HTML.gif is the ratio of two statistically independent random variables. The PDF of https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq101_HTML.gif can be thus written as
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_Equ15_HTML.gif
(15)
Applying (7) and (14) into (15) and after some steps, we get
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_Equ16_HTML.gif
(16)
With the help of [25, equation 3.38.4], (16) can be written in the closed-form as
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_Equ17_HTML.gif
(17)
The average of the SLR is thus given by
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_Equ18_HTML.gif
(18)
After substituting https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq102_HTML.gif from (17), applying [25, equation 3.194.3], and after some steps of straightforward derivations, we get
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_Equ19_HTML.gif
(19)
where https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq103_HTML.gif is the Beta function. Noting that https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq104_HTML.gif and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq105_HTML.gif , (19) can be further simplified as
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_Equ20_HTML.gif
(20)
The outage probability of SLR is a parameter that shows how often the transmit beamformer is not capable of maintaining the ratio of the signal power to the leakage power above a certain threshold value. The outage probability for the https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq106_HTML.gif th user is defined as
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_Equ21_HTML.gif
(21)
where https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq107_HTML.gif is the system specific threshold value. Note that (21) represents the probability of the transmit beamformer failing to perform its beamforming task properly. Hence, the concept of the SLR outage is analogous to the probability of receiver failing to work properly but is only applicable from a transmitter's point of view. Since the PDF of SLR is already known, the outage probability of (21) can be expressed as
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_Equ22_HTML.gif
(22)
Using (17) and applying [25, equation 3.194.1], it can be shown that the outage probability (22) can be expressed as
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_Equ23_HTML.gif
(23)
where https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq108_HTML.gif and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq109_HTML.gif is the Gauss hypergeometric function (see [25, equation 9.100]). Noting the transformation rule https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq110_HTML.gif (see [25, equation 9.131.1]) and the fact that https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq111_HTML.gif = https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq112_HTML.gif , and after some simple manipulations, (23) can also be expressed in the following alternative form:
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_Equ24_HTML.gif
(24)
Here, it is worthwhile to mention that for https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq113_HTML.gif , https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq114_HTML.gif (7) becomes exponentially distributed whereas https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq115_HTML.gif (9) becomes a weighted sum of independent exponentially distributed random variables. In this case, the outage probability expression of [15] can be easily derived. However, it cannot be analytically obtained by substituting https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq116_HTML.gif in (23) due to the approximation (10). Also, note that the proposed outage probability analysis can be applied to frequency-selective fading channels where we can consider that the orthogonal frequency division multiplexing (OFDM) is used as a modulation technique. In this context, the MIMO channel for each subcarrier can be considered to be a flat-fading channel. Considering that all users can access a given subcarrier and that the lengths of channel impulse responses for all receive-transmit antenna combinations of all users are shorter than the cyclic prefix [26], the SLR for the https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq117_HTML.gif th user and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq118_HTML.gif th subcarrier can be expressed as
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_Equ25_HTML.gif
(25)
where https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq119_HTML.gif is the MIMO channel in frequency domain for the https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq120_HTML.gif th user and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq121_HTML.gif th subcarrier, and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq122_HTML.gif is the corresponding gain. Let https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq123_HTML.gif be the https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq124_HTML.gif th row and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq125_HTML.gif th column entry of https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq126_HTML.gif , and be given by
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_Equ26_HTML.gif
(26)
where https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq127_HTML.gif is the total number of subcarriers, https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq128_HTML.gif is the number of independently fading channel-taps, and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq129_HTML.gif is the impulse response for https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq130_HTML.gif th tap of the channel between https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq131_HTML.gif th receive and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq132_HTML.gif th transmit antenna. If https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq133_HTML.gif are ZMCSCG, it is very easy to note that https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq134_HTML.gif is a ZMCSCG. Furthermore, if the average sum of the tap-powers for the channel between the https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq135_HTML.gif th receive and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq136_HTML.gif th transmit antennas is same, that is, if https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq137_HTML.gif for all https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq138_HTML.gif , after some straightforward steps, we can easily verify that the distribution of https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq139_HTML.gif remains complex Wishart with the same scaling matrix https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq140_HTML.gif and the degrees of freedom parameter https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq141_HTML.gif . This shows that the statistics of the signal and leakage powers for a given subcarrier and user remain unchanged.

4. Maximize the Average SLR and Minimize the Outage Probability

In this section, our objective is to find the optimum https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq142_HTML.gif which maximizes the average SLR and minimizes the outage probability of the SLR observed by https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq143_HTML.gif th user. Note that due to the fact that we use the average SLR and SLR outage as the criteria, the beamformer design is a decoupled problem and can be carried out separately for each user.

4.1. Maximize the Average SLR

The beamformer which maximizes the average SLR is obtained by solving the problem https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq144_HTML.gif which is a difficult optimization problem as https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq145_HTML.gif and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq146_HTML.gif are complicated functions of https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq147_HTML.gif , although https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq148_HTML.gif is a quadratic function of https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq149_HTML.gif . In order to make this optimization problem tractable, we make certain assumptions which will be clear in the sequel. We can write (20) as
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_Equ27_HTML.gif
(27)
Let us define https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq150_HTML.gif for all https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq151_HTML.gif , where https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq152_HTML.gif . Then, with the help of a well-known power-mean inequality, we can write
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_Equ28_HTML.gif
(28)
where the equality holds only if https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq153_HTML.gif are all equal. Applying the above inequality to the expression of https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq154_HTML.gif in (13), we can get an upper bound for https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq155_HTML.gif and more specifically we can write https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq156_HTML.gif . With this observation, the average SLR (27) can be lowerbounded as
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_Equ29_HTML.gif
(29)
Here, an interesting observation is that though https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq157_HTML.gif and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq158_HTML.gif are separately nonquadratic functions of https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq159_HTML.gif , their products https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq160_HTML.gif is quadratic in https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq161_HTML.gif . The latter fact can be observed from (13), and thus the product https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq162_HTML.gif can be expressed as
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_Equ30_HTML.gif
(30)
Using (30) and resubstituting https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq163_HTML.gif in terms of https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq164_HTML.gif , (29) can be expressed as
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_Equ31_HTML.gif
(31)
Since the exact average SLR (27) is difficult to maximize, we maximize its lower bound (31) which has a Rayleigh quotient form. The latter can be maximized by maximizing the numerator https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq165_HTML.gif (the useful power directed to the https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq166_HTML.gif th user) while keeping the denominator https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq167_HTML.gif (the leakage power) constant. This gives the well-known solution
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_Equ32_HTML.gif
(32)
Thus, the optimum weight vector https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq168_HTML.gif is the eigenvector associated with the largest eigenvalue (generalized eigenvalue problem) of the characteristic equation given by (32). Later, our numerical results confirm the tightness of the lower bound (31) of average SLR for the weight obtained from (32).

4.2. Minimize the SLR Outage

Mathematically, this problem has the following unconstrained minimization form: https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq169_HTML.gif . We note that https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq170_HTML.gif is a complicated function of https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq171_HTML.gif and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq172_HTML.gif which in turn depend on https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq173_HTML.gif . Therefore, the standard way of finding the first-order derivative of the outage probability with respect to https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq174_HTML.gif and equating the corresponding result to zero does not enable us to solve the problem in closed-form. Here, our approach is to first intituitively find the limiting values of https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq175_HTML.gif and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq176_HTML.gif for which the outage in (24) approaches to zero. The second step is to find https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq177_HTML.gif in order to achieve those limiting values of https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq178_HTML.gif and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq179_HTML.gif . After simple manipulation, the outage probability (24) can also be written as
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_Equ33_HTML.gif
(33)
Note that the Gauss hypergeometric function https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq180_HTML.gif converges for arbitrary https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq181_HTML.gif , https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq182_HTML.gif and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq183_HTML.gif if https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq184_HTML.gif (see [25, Section https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq185_HTML.gif ]). This is the case in (33) since https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq186_HTML.gif for any https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq187_HTML.gif . It is also not difficult to see from the series form of https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq188_HTML.gif (see [25, equation 9.100]) that its minimum in (33) is https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq189_HTML.gif which can be achieved if https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq190_HTML.gif and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq191_HTML.gif . As https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq192_HTML.gif , the term https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq193_HTML.gif approaches to zero whereas when https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq194_HTML.gif and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq195_HTML.gif , the term https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq196_HTML.gif tends to be zero. Hence, it can be concluded that if https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq197_HTML.gif and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq198_HTML.gif can be minimized with respect to https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq199_HTML.gif , the outage expression (33) can also be minimized. Here, we want to emphasize that the analytical proof for the optimality of the above mentioned approach is still an open issue. Now, the outage probability minimization problem can be turned to the problem of minimizing https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq200_HTML.gif and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq201_HTML.gif simultaneously with respect to https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq202_HTML.gif , that is, https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq203_HTML.gif , which is a multicriterion optimization problem [27]. Using the notation https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq204_HTML.gif , this multicriterion minimization problem can by scalarized by forming the weighted objective function [27]
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_Equ34_HTML.gif
(34)
where the weights for the first and second objective functions are https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq205_HTML.gif and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq206_HTML.gif , respectively. Here, we can interpret https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq207_HTML.gif as the relative importance of the second objective function with respect to the first one. Note that (34) is a difficult optimization problem. The following inequality can be easily shown:
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_Equ35_HTML.gif
(35)
Now using the upper bounds (35) and (28), the objective function in (34) can also be upperbounded as
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_Equ36_HTML.gif
(36)
where again equality holds if all https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq208_HTML.gif are equal. Using the above upper bound and resubstituting for https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq209_HTML.gif and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq210_HTML.gif , the minimization problem (34) takes the following form:
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_Equ37_HTML.gif
(37)
which is also in the familiar Rayleigh quotient form. (Since we replace the exact cost function by its upper bound, the minimization problem becomes independent of https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq211_HTML.gif .) With the help of Lagrangian multiplier method, we can show that the optimum weight vector that minimizes (37) is given by (32) which is just the solution of the transmit beamformer that maximizes the average SLR. Hence, it is clear from (32) that the minimum outage probability and maximum average SLR transmit beamformer require only the knowledge of correlation matrices and average channel power gains. We will later demonstrate, with the numerical results, that the upper bounds in (35), (28), and (36) are relatively tight for the beamformer weight derived from (32).

5. Numerical Results and Discussions

In this section, we first verify the correctness of the analytically derived PDF (17) of SLR by comparing the analytical results with the Monte-Carlo simulation results. Next, we investigate the tightness of the bounds in (29) and (36). The outage probability of SLR for the https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq212_HTML.gif th user (for conciseness, the results are shown for https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq213_HTML.gif ) obtained via theory (23) and Monte-Carlo simulations are also shown for different parameters and correlation models. However, these results are not intended to illustrate the outage performance of a particular system. This would require additional assumptions regarding power control, modulation, and channel coding. Finally, we also demonstrate that the maximum average SLR or minimum outage probability transmit beamformer also helps to significantly improve the user SINR when the user employs linear operation such as matched filtering. We consider MIMO channels in which the transmit correlations are modeled with two different methods; exponential correlation and Gaussian angle of arrival (AoA) models. Throughout all examples, we take https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq214_HTML.gif , https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq215_HTML.gif , https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq216_HTML.gif , https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq217_HTML.gif , https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq218_HTML.gif , and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq219_HTML.gif . Note that this is purely by way of example, and other values could just have easily been considered. The outage probability of SLR is presented using Monte-Carlo simulation runs during which the channels ( https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq220_HTML.gif change independently and randomly. For each channel realization, the SLR for https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq221_HTML.gif th user is computed and compared with the threshold value https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq222_HTML.gif for determining the outage probability.

5.1. Exponential Correlation Model

In this example, the amplitudes of the spatial correlations among the elements of the BS antenna array are considered to be exponentially related. With this assumption, the correlation matrices are defined as
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_Equ38_HTML.gif
(38)
where https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq223_HTML.gif represent the https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq224_HTML.gif th row and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq225_HTML.gif th column of https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq226_HTML.gif , https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq227_HTML.gif are the amplitudes of correlation coefficients and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq228_HTML.gif is the AoA of the plane wave from the https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq229_HTML.gif th point source.
The analytically obtained PDF (17) of SLR is compared with the simulation results as shown in Figure 2. In this figure, the beamformer weights are optimized according to (32) for the exponential correlation model (38). It can be observed from Figure 2 that the analytical and simulation results are in fine agreement, and hence the accuracy of the derived PDF of SLR is validated. Figure 3 displays the analytical and simulated outage probabilities of SLR versus https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq230_HTML.gif for (a) the optimized https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq231_HTML.gif from (32), (b) the non-optimized https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq232_HTML.gif ( https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq233_HTML.gif ), and (c) https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq234_HTML.gif which is the eigenvector corresponding to the maximum eigenvalue of https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq235_HTML.gif . Note that the last method simply tries to maximize the signal power toward the user of interest without even trying to suppress the leakage power toward the other users. Although this approach is highly suboptimal, it is very simple to implement, and its performance can be encouraging especially in UMTS cellular networks [28] where, due to downlink omnidirectional strong common pilot channels, the overall leakage power appears to be almost white noise. As expected, it can be observed from Figure 3 that the method (32) outperforms the other two cases. The theoretical and numerical results for different values of https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq236_HTML.gif and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq237_HTML.gif are compared in Figure 4. In Figures 2 and 3, we take https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq238_HTML.gif and in Figures 2, 3, and 4 we take https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq239_HTML.gif , https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq240_HTML.gif , https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq241_HTML.gif , https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq242_HTML.gif and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq243_HTML.gif .

5.2. Spatial Correlation Model-Gaussian Angle of Arrival (AoA)

In this example, the spatial correlation among elements of the BS antenna array is modeled according to the distribution of the AoA of the incoming plane waves at the BS from the https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq249_HTML.gif th user. The AoA is assumed to be Gaussian distributed with a standard deviation https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq250_HTML.gif of angular spreading. For this case, we consider a uniform linear array with the half-wavelength spacing. The correlation is thus given by [3]
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_Equ39_HTML.gif
(39)
where https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq251_HTML.gif is the central angle of the incoming rays to the BS from the https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq252_HTML.gif th user. We assume that the first user is located at https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq253_HTML.gif relative to the BS array broadside, and the other two users are located at https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq254_HTML.gif where we take https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq255_HTML.gif (except in Figure 6 where https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq256_HTML.gif is varied) and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq257_HTML.gif for all https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq258_HTML.gif .
The exact average SLR (27) and its lower bound (31) both versus https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq259_HTML.gif are compared in Figure 5 where the optimum weight vector is chosen according to (32). We take https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq260_HTML.gif for this figure. It can be seen from Figure 5, that the difference between the exact values of the average SLR and its lower bound is almost negligible for all https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq261_HTML.gif which in fact confirms that the beamformer (32) maximizes the average SLR with a very fine accuracy. The exact functions in (28) and (35), their corresponding upper bounds, the sum function (36) (with https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq262_HTML.gif ), and its upper bound are displayed in Figure 6 for different values of https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq263_HTML.gif where the beamformer is derived from (32). It can be observed from this figure that the bound in (28) is very tight for all values of https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq264_HTML.gif whereas that in (35) is tight for the medium and larger values of https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq265_HTML.gif . In fact, the gap between the overall exact function (36) and its upper bound is sufficiently small for all values of https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq266_HTML.gif . Figure 7 shows the outage probability of SLR versus https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq267_HTML.gif obtained via theory and simulations for different values of https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq268_HTML.gif and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq269_HTML.gif . The average SINR (5) and the average SLNR (3) of https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq270_HTML.gif th user versus the receiver noise power https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq271_HTML.gif are displayed in Figure 8 again for (a) the optimized https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq272_HTML.gif of (32), (b) the non-optimized https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq273_HTML.gif ( https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq274_HTML.gif ), and (c) https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq275_HTML.gif which is the eigenvector corresponding to the maximum eigenvalue of https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq276_HTML.gif . In this figure, the SINR and SLNR are averaged over https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq277_HTML.gif independent channel realizations, and it is considered that the receiver has perfect knowledge of instantaneous channels. It can be seen from Figure 8 that the transmit beamformer (32) based on maximization of SLR significantly helps to improve the receiver's SINR. Figures 3, 4, and 7 display that the matching between the theoretical and simulation results is very fine. This confirms the validity of the proposed theoretical expression for outage probability. It can be noticed (see Figures 3 and 8) that the beamformer, which tries to suppress the leakage power while maximizing the signal power (32), is better than the one which only maximizes the signal power of the user of interest by neglecting the leakage power (method (c). The results (Figures 4 and 7) also show that as the spatial correlation between the antenna elements increases (correlation coefficient increases or angular spreading decreases), the outage probability decreases. The latter observation can be explained from the fact that when the spatial correlation increases, the ranks of MIMO channels decrease, thereby allowing the beamformer to perform better. The best performance can even be obtained when the MIMO channels are fully correlated ( i.e., channels become rank one). It can be also observed (see Figures 4 and 7) that by increasing the BS antenna correlation, the performance can be improved more effectively than just by increasing the number of user antennas while keeping the BS antenna correlation sufficiently low. Furthermore, as expected in Figures 3, 4, and 7, the outage probability increases with increasing https://static-content.springer.com/image/art%3A10.1155%2F2009%2F679430/MediaObjects/13638_2009_Article_1721_IEq278_HTML.gif .

6. Conclusions

A fine agreement between the theoretical and simulation results for the PDF of SLR and its outage probability confirms the correctness of the proposed analysis for a multiuser MIMO downlink beamforming in a Rayleigh fading environment. The results also show that the spatial correlation between the antenna elements significantly helps to increase the performance of the SLR-based transmit beamformer in terms of the SLR outage probability. It has been found via some approximations that the transmit beamformer which maximizes the average SLR also minimizes the outage probability of the SLR.
Open AccessThis article is distributed under the terms of the Creative Commons Attribution 2.0 International License (https://​creativecommons.​org/​licenses/​by/​2.​0), which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.
Literature
1.
go back to reference Rashid-Farrokhi F, Liu KJR, Tassiulas L: Joint optimal power control and beamforming in wireless networks using antenna arrays. IEEE Transactions on Communications 1998, 46(10):1313-1324. 10.1109/26.725309CrossRef Rashid-Farrokhi F, Liu KJR, Tassiulas L: Joint optimal power control and beamforming in wireless networks using antenna arrays. IEEE Transactions on Communications 1998, 46(10):1313-1324. 10.1109/26.725309CrossRef
2.
go back to reference Schubert M, Boche H: Solution of the multiuser downlink beamforming problem with individual SINR constraints. IEEE Transactions on Vehicular Technology 2004, 53(1):18-28. 10.1109/TVT.2003.819629CrossRef Schubert M, Boche H: Solution of the multiuser downlink beamforming problem with individual SINR constraints. IEEE Transactions on Vehicular Technology 2004, 53(1):18-28. 10.1109/TVT.2003.819629CrossRef
3.
go back to reference Bengtsson M, Ottersten B: Optimal downlink beamforming using semidefinite optimization. Proceedings of the 37th Annual Allerton Conference on Communication, Control, and Computing, September 1999, Monticello, Ill, USA 987-996. Bengtsson M, Ottersten B: Optimal downlink beamforming using semidefinite optimization. Proceedings of the 37th Annual Allerton Conference on Communication, Control, and Computing, September 1999, Monticello, Ill, USA 987-996.
4.
go back to reference Foschini GJ: Layered space-time architecture for wireless communication in a fading environment when using multi-element antennas. Bell Labs Technical Journal 1996, 1(2):41-59.CrossRef Foschini GJ: Layered space-time architecture for wireless communication in a fading environment when using multi-element antennas. Bell Labs Technical Journal 1996, 1(2):41-59.CrossRef
5.
go back to reference Telatar E: Capacity of multi-antenna Gaussian channels. European Transactions on Telecommunications 1999, 10(6):585-595. 10.1002/ett.4460100604CrossRef Telatar E: Capacity of multi-antenna Gaussian channels. European Transactions on Telecommunications 1999, 10(6):585-595. 10.1002/ett.4460100604CrossRef
6.
go back to reference Chang J-H, Tassiulas L, Rashid-Farrokhi F: Joint transmitter receiver diversity for efficient space division multiaccess. IEEE Transactions on Wireless Communications 2002, 1(1):16-27. 10.1109/7693.975441CrossRef Chang J-H, Tassiulas L, Rashid-Farrokhi F: Joint transmitter receiver diversity for efficient space division multiaccess. IEEE Transactions on Wireless Communications 2002, 1(1):16-27. 10.1109/7693.975441CrossRef
7.
go back to reference Sadek M, Tarighat A, Sayed AH: A leakage-based precoding scheme for downlink multi-user MIMO channels. IEEE Transactions on Wireless Communications 2007, 6(5):1711-1721.CrossRef Sadek M, Tarighat A, Sayed AH: A leakage-based precoding scheme for downlink multi-user MIMO channels. IEEE Transactions on Wireless Communications 2007, 6(5):1711-1721.CrossRef
8.
go back to reference Sadek M, Tarighat A, Sayed AH: Active antenna selection in multiuser MIMO communications. IEEE Transactions on Signal Processing 2007, 55(4):1498-1510.MathSciNetCrossRef Sadek M, Tarighat A, Sayed AH: Active antenna selection in multiuser MIMO communications. IEEE Transactions on Signal Processing 2007, 55(4):1498-1510.MathSciNetCrossRef
9.
go back to reference Gerlach D, Paulraj A: Base station transmitting antenna arrays for multipath environments. Signal Processing 1996, 54(1):59-73. 10.1016/0165-1684(96)00093-XCrossRefMATH Gerlach D, Paulraj A: Base station transmitting antenna arrays for multipath environments. Signal Processing 1996, 54(1):59-73. 10.1016/0165-1684(96)00093-XCrossRefMATH
10.
go back to reference Zetterberg P, Ottersten B: The Spectrum efficiency of a base station antenna array system for spatially selective transmission. IEEE Transactions on Vehicular Technology 1995, 44(3):651-660. 10.1109/25.406634CrossRef Zetterberg P, Ottersten B: The Spectrum efficiency of a base station antenna array system for spatially selective transmission. IEEE Transactions on Vehicular Technology 1995, 44(3):651-660. 10.1109/25.406634CrossRef
11.
go back to reference Bengtsson M, Ottersten B: Optimal and suboptimal beamforming. In Handbook of Antennas in Wireless Communications. CRC Press, Boca Raton, Fla, USA; August 2001. Bengtsson M, Ottersten B: Optimal and suboptimal beamforming. In Handbook of Antennas in Wireless Communications. CRC Press, Boca Raton, Fla, USA; August 2001.
12.
go back to reference Song Y, Blostein SD, Cheng J: Exact outage probability for equal gain combining with cochannel interference in Rayleigh fading. IEEE Transactions on Wireless Communications 2003, 2(5):865-870. 10.1109/TWC.2003.816796CrossRef Song Y, Blostein SD, Cheng J: Exact outage probability for equal gain combining with cochannel interference in Rayleigh fading. IEEE Transactions on Wireless Communications 2003, 2(5):865-870. 10.1109/TWC.2003.816796CrossRef
13.
go back to reference Shah A, Haimovich AM: Performance analysis of optimum combining in wireless communications with rayleigh fading and cochannel interference. IEEE Transactions on Communications 1998, 46(4):473-479. 10.1109/26.664303CrossRef Shah A, Haimovich AM: Performance analysis of optimum combining in wireless communications with rayleigh fading and cochannel interference. IEEE Transactions on Communications 1998, 46(4):473-479. 10.1109/26.664303CrossRef
14.
go back to reference Shah A, Haimovich AM: Performance analysis of maximal ratio combining and comparison with optimum combining for mobile radio communications with cochannel interference. IEEE Transactions on Vehicular Technology 2000, 49(4):1454-1463. 10.1109/25.875282CrossRef Shah A, Haimovich AM: Performance analysis of maximal ratio combining and comparison with optimum combining for mobile radio communications with cochannel interference. IEEE Transactions on Vehicular Technology 2000, 49(4):1454-1463. 10.1109/25.875282CrossRef
15.
go back to reference Kandukuri S, Boyd S: Optimal power control in interference-limited fading wireless channels with outage-probability specifications. IEEE Transactions on Wireless Communications 2002, 1(1):46-55. 10.1109/7693.975444CrossRef Kandukuri S, Boyd S: Optimal power control in interference-limited fading wireless channels with outage-probability specifications. IEEE Transactions on Wireless Communications 2002, 1(1):46-55. 10.1109/7693.975444CrossRef
16.
go back to reference Papandriopoulos J, Evans J, Dey S: Outage-based optimal power control for generalized multiuser fading channels. IEEE Transactions on Communications 2006, 54(4):693-703.CrossRef Papandriopoulos J, Evans J, Dey S: Outage-based optimal power control for generalized multiuser fading channels. IEEE Transactions on Communications 2006, 54(4):693-703.CrossRef
17.
go back to reference Bengtsson M, Ottersten B: Signal waveform estimation from array data in angular spread environment. Proceedings of the 13th Asilomar Conference on Signals, Systems and Computers, November 1997 1: 355-359.CrossRef Bengtsson M, Ottersten B: Signal waveform estimation from array data in angular spread environment. Proceedings of the 13th Asilomar Conference on Signals, Systems and Computers, November 1997 1: 355-359.CrossRef
18.
go back to reference Zhou S, Giannakis GB: Optimal transmitter eigen-beamforming and space-time block coding based on channel correlations. IEEE Transactions on Information Theory 2003, 49(7):1673-1690. 10.1109/TIT.2003.813565MathSciNetCrossRefMATH Zhou S, Giannakis GB: Optimal transmitter eigen-beamforming and space-time block coding based on channel correlations. IEEE Transactions on Information Theory 2003, 49(7):1673-1690. 10.1109/TIT.2003.813565MathSciNetCrossRefMATH
19.
go back to reference Chiani M, Win MZ, Zanella A: On the capacity of spatially correlated MIMO Rayleigh-fading channels. IEEE Transactions on Information Theory 2003, 49(10):2363-2371. 10.1109/TIT.2003.817437MathSciNetCrossRefMATH Chiani M, Win MZ, Zanella A: On the capacity of spatially correlated MIMO Rayleigh-fading channels. IEEE Transactions on Information Theory 2003, 49(10):2363-2371. 10.1109/TIT.2003.817437MathSciNetCrossRefMATH
20.
go back to reference Luo J, Zeidler JR, McLaughlin S: Performance analysis of compact antenna arrays with MRC in correlated Nakagami fading channels. IEEE Transactions on Vehicular Technology 2001, 50(1):267-277. 10.1109/25.917940CrossRef Luo J, Zeidler JR, McLaughlin S: Performance analysis of compact antenna arrays with MRC in correlated Nakagami fading channels. IEEE Transactions on Vehicular Technology 2001, 50(1):267-277. 10.1109/25.917940CrossRef
21.
go back to reference Häring L, Chalise BK, Czylwik A: Dynamic system level simulations of downlink beamforming for UMTS FDD. Proceedings of IEEE Global Telecommunications Conference (GLOBECOM '03), December 2003, San Francisco, Calif, USA 1: 492-496.CrossRef Häring L, Chalise BK, Czylwik A: Dynamic system level simulations of downlink beamforming for UMTS FDD. Proceedings of IEEE Global Telecommunications Conference (GLOBECOM '03), December 2003, San Francisco, Calif, USA 1: 492-496.CrossRef
22.
go back to reference Rong H, Hiltunen K: Performance investigation of secondary scrambling codes in WCDMA systems. Proceedings of the 63rd IEEE Vehicular Technology Conference (VTC '06), May 2006, Melbourne, Australia 2: 698-702. Rong H, Hiltunen K: Performance investigation of secondary scrambling codes in WCDMA systems. Proceedings of the 63rd IEEE Vehicular Technology Conference (VTC '06), May 2006, Melbourne, Australia 2: 698-702.
23.
go back to reference Muirhead RJ: Aspects of Multivariate Statistical Theory, Wiley Series in Probability and Mathematical Statistics. Wiley, New York, NY, USA; 1982.CrossRef Muirhead RJ: Aspects of Multivariate Statistical Theory, Wiley Series in Probability and Mathematical Statistics. Wiley, New York, NY, USA; 1982.CrossRef
24.
go back to reference Zhang QT, Liu DP: A simple capacity formula for correlated diversity Rician fading channels. IEEE Communications Letters 2002, 6(11):481-483. 10.1109/LCOMM.2002.805523CrossRef Zhang QT, Liu DP: A simple capacity formula for correlated diversity Rician fading channels. IEEE Communications Letters 2002, 6(11):481-483. 10.1109/LCOMM.2002.805523CrossRef
25.
go back to reference Gradshteyn IS, Ryzhik IM: Table of Integrals, Series, and Products. 6th edition. Academic Press, New York, NY, USA; 2000. A. Jeffrey EdMATH Gradshteyn IS, Ryzhik IM: Table of Integrals, Series, and Products. 6th edition. Academic Press, New York, NY, USA; 2000. A. Jeffrey EdMATH
26.
go back to reference Iserte AP, Perez-Neira AI, Hernandez MAL: Joint beamforming strategies in OFDM-MIMO systems. Proceedings of IEEE International Conference on Acoustics, Speech, and Signal Processing (ICASSP '02), May 2002, Orlando, Fla, USA 3: 2845-2848. Iserte AP, Perez-Neira AI, Hernandez MAL: Joint beamforming strategies in OFDM-MIMO systems. Proceedings of IEEE International Conference on Acoustics, Speech, and Signal Processing (ICASSP '02), May 2002, Orlando, Fla, USA 3: 2845-2848.
27.
go back to reference Boyd S, Vandenbergh L: Convex Optimization. Cambridge University Press, Cambridge, UK; 2004.CrossRef Boyd S, Vandenbergh L: Convex Optimization. Cambridge University Press, Cambridge, UK; 2004.CrossRef
28.
go back to reference Czylwik A, Dekorsy A, Chalise BK: Smart antenna solutions for UMTS. In Smart Antennas—State of the Art, EURASIP Hindawi Book Series Edited by: Kaiser T, Boudroux Aet al.. 2005, 729-758. Czylwik A, Dekorsy A, Chalise BK: Smart antenna solutions for UMTS. In Smart Antennas—State of the Art, EURASIP Hindawi Book Series Edited by: Kaiser T, Boudroux Aet al.. 2005, 729-758.
Metadata
Title
A Multiuser MIMO Transmit Beamformer Based on the Statistics of the Signal-to-Leakage Ratio
Authors
Batu K. Chalise
Luc Vandendorpe
Publication date
01-12-2009
Publisher
Springer International Publishing
DOI
https://doi.org/10.1155/2009/679430

Other articles of this Issue 1/2009

EURASIP Journal on Wireless Communications and Networking 1/2009 Go to the issue

Premium Partner