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*Electronics*
**2019**,
*8*(1),
79;
https://doi.org/10.3390/electronics8010079

Article

LOS-Based Equal Gain Transmission and Combining in General Frequency-Selective Ricean Massive MIMO Channels

^{1}

School of Information Science and Technology, Dalian Maritime University, Dalian 116026, China

^{2}

State Key Laboratory of Integrated Services Networks, Xidian University, Xi’an 710071, China

^{*}

Author to whom correspondence should be addressed.

Received: 13 December 2018 / Accepted: 7 January 2019 / Published: 10 January 2019

## Abstract

**:**

In general frequency-selective Ricean fading environments with doubly-ended spatial correlation, this paper investigates the spectral efficiency of a broadband massive multiple-input multiple-output (MIMO) system. In particular, in order to reduce overhead of channel estimation effectively, it proposes a scheme of equal gain transmission and combining, which is only based on line- of-sight (LOS) component and has low hardware complexity. With the scheme, several interesting transmit power scaling properties without and with spatial correlation are derived when the number of antennas at the transmitter or the number of antennas at the receiver grows in an unlimited way. Furthermore, the asymptotical rate analysis is extended to the cooperative relaying scenarios with decode-and-forward and amplify-and-forward protocols, respectively, and then two novel power scaling laws are given.

Keywords:

massive MIMO; beamforming; line-of-sight; Ricean fading; frequency-selective; power scaling## 1. Introduction

Recently, massive multiple-input multiple-output (MIMO) has attracted great interest in both academia and industry, and has been a promising solution to meet the demanding spectral efficiency requirement of 5G systems [1]. Its promising benefits includes significant increase of both spectral and energy efficiencies [2,3,4]. Interestingly, the two benefits of massive MIMO can be achieved by maximum-ration transmission/maximum-ration combining (MRT/MRC) or zero-forcing (ZF) precoding/detection [3,5].

With MRT/MRC and ZF linear processing, many scholars have given various asymptotic performance analyses. In particular, the power scaling law in the limit of the large number of antennas has been widely studied in order to quantify the power savings. For Rayleigh and Ricean fading environments, with MRC and ZF detectors, authors in [3,6] analyzed uplink massive MIMO system performance. If perfect channel state information (CSI) is available, they showed that, when the number of base station (BS) antennas grows large and the transmit power of each user is scaled down proportionally to it, the ergodic achievable rate can asymptotically be equal to a positive constant.

In order to obtain the needed CSI, channel estimation must be obviously carried on [7]. However, the channel estimation will result in not only heavy overhead but also pilot contamination in multi-cells, which will become a serious problem [2,8]. For a point to point massive MIMO system in Ricean fading, to reduce the heavy overhead to estimate the CSI, we investigated a scheme with equal gain transmission /equal gain combining (EGT/EGC), which is only based on the line-of-sight (LOS) component (or say specular component) and has low hardware complexity [9]. It was showed that, with this scheme, the ergodic achievable rate can converge to that of the corresponding MRT/MRC based on the perfect CSI as the two numbers of antennas at the transmitter and receiver go to infinity. After that, we further considered the novel linear processing scheme for a downlink or uplink multiuser massive MIMO system [10,11] and showed that each user in the downlink or uplink system can have asymptotically the same rate as in the single-user case when the number of BS antennas goes without bound.

It should be pointed out that the above-mentioned results with the novel scheme have only considered uncorrelated Ricean frequency-flat fading channels without a relay [12]. Recently, we tried to develop our analysis to frequency-selective Ricean fading channels [13], but only for a very simple and special scenario [14]. The EGT/EGC linear transmission scheme is very attractive for massive MIMO systems since it enables low-complexity and inexpensive hardware [15,16,17,18]. Motivated by these facts, in this paper, we make use of a comparatively complicated and general frequency-selective Ricean fading channel model [14,19,20] to investigate further the LOS-based EGT/EGC scheme. We firstly derive several interesting power scaling properties for broadband massive MIMO systems with and without spatial correlation. In particular, it is shown that the ergodic achievable rate of LOS-based EGT/EGC scheme can have the same asymptotic value as the ergodic achievable rate of the whole CSI-based MRT/MRC scheme if the two numbers of transmit and receive antennas go without bound and with a fixed ratio. Then, we extend our asymptotical performance analysis to the cooperative relaying scenarios with decode-and-forward (DF) protocol and with amplify-and-forward (AF) protocol, respectively, and obtain two novel power scaling laws for the two scenarios. In particular, it is also shown that the ergodic achievable rate of LOS-based scheme can have the same asymptotic value as the ergodic achievable rate of the CSI-based scheme if the number of source antennas and the two numbers of transmit and receive relay antennas go without bound and with two fixed ratios, respectively.

The manuscript is organized as follows: in Section 2, the system model is introduced. In Section 3, the proposed LOS-based transmission scheme is presented and its power scaling law without correlation and with correlation is derived, respectively. Extension of our analysis to a cooperative relaying system is given in Section 4. In Section 5, the analysis results are verified by simulation. Finally, in Section 6, some concluding remarks are given.

Notation: boldface lower and upper case letters denote column vectors and matrices, respectively. The superscripts ${\left(\xb7\right)}^{\u2020}$ and ${\left(\xb7\right)}^{\mathtt{T}}$ stand for conjugate-transpose and transpose operations, respectively. The expectation operator is denoted by $\mathbb{E}\{\xb7\}$. $\alpha \sim \mathtt{CN}(0,{\delta}^{2})$ stands for a circularly symmetric complex Gaussian variable $\alpha $ which has zero mean and variance ${\delta}^{2}$.

## 2. System Model

Since a set of parallel independent frequency flat MIMO channels can be used to describe a frequency selective MIMO channel, we start with introducing the frequency flat channels [14,19].

For a point-to-point MIMO system over frequency-flat channels, we assume that it has N transmit antennas and M receive antennas. Then, we can represent a $M\times 1$ received signal vector as
where $\mathbf{z}$ denotes the additive white Gaussian noise (AWGN) vector that has zero-mean and covariance matrix ${\sigma}^{2}{\mathbf{I}}_{M}$ with ${\mathbf{I}}_{M}$ being the $M\times M$ identity matrix, $\mathbf{x}$ denotes the transmitted signal vector, ${\mathbf{H}}_{0}={[{h}_{mn}]}_{m,n=1}^{M,N}$ stands for the $M\times N$ channel matrix whose element ${h}_{mn}$ denotes the channel gain between the m-th antenna at the receiver and the n-th antenna at the transmitter, and p is the average transmitted power. The channel matrix ${\mathbf{H}}_{0}$ under Ricean fading consists of a LOS matrix and a scattered matrix, i.e.,
where ${\overline{\kappa}}_{0}=\frac{{\kappa}_{0}}{1+{\kappa}_{0}}$, ${\tilde{\kappa}}_{0}=\frac{1}{1+{\kappa}_{0}}$. Note that ${\kappa}_{0}>0$ represents the Ricean K-factor. The LOS matrix ${\overline{\mathbf{H}}}_{0}$ can be written as

$$\mathbf{y}=\sqrt{p}{\mathbf{H}}_{0}\mathbf{x}+\mathbf{z},$$

$${\mathbf{H}}_{0}=\sqrt{{\overline{\kappa}}_{0}}{\overline{\mathbf{H}}}_{0}+\sqrt{{\tilde{\kappa}}_{0}}{\tilde{\mathbf{H}}}_{0},$$

$${\overline{\mathbf{H}}}_{0}={\mathbf{r}}_{0}{\mathbf{t}}_{0}^{\mathtt{T}}.$$

Here, ${\mathbf{r}}_{0}$ denotes the specular array response at the receiver and can be expressed as
where $\theta $ is the angle of arrival of the LOS component and ${d}_{r}$ is the antenna spacing normalized by wavelength at the receiver. Similarly, ${\mathbf{t}}_{0}$ denotes the specular array response at the transmitter and can be given by
where $\varphi $ is the angle of departure of the LOS component and ${d}_{t}$ is the antenna spacing normalized by wavelength at the transmitter. The entries in the scattering matrix ${\tilde{\mathbf{H}}}_{0}$, ${[{\tilde{\mathbf{H}}}_{0}]}_{mn}\sim \mathtt{CN}(0,1)$, i.e., they are circular complex Gaussian random variables with zero mean and unit variance. Furthermore, we assume that they are independent and identically distributed (i.i.d).

$${\mathbf{r}}_{0}={[1,{e}^{j2\pi {d}_{r}sin(\theta )},\dots ,{e}^{j2\pi (M-1){d}_{r},sin(\theta )}]}^{\mathtt{T}},$$

$${\mathbf{t}}_{0}={[1,{e}^{j2\pi {d}_{t}sin(\varphi )},\dots ,{e}^{j2\pi (N-1){d}_{t}sin(\varphi )}]}^{\mathtt{T}}$$

Now, we are concerned with a broadband orthogonal frequency-division multiplexing (OFDM)-MIMO system with K subcarriers, where ideal OFDM transmission with proper cyclic prefix extension is assumed. For the k-th subcarrier, the input–output relationship is expressed as
where $\mathbf{x}$ is just the normalized signal vector, $\mathbf{z}$ is the AWGN vector, and $\mathbf{H}$ is the channel matrix. The channel matrix can be given by as
where L represents the channel delay spread, $\{{\rho}_{\ell}^{2}\}$ is the power delay profile satisfying ${\sum}_{\ell =0}^{L-1}{\rho}_{\ell}^{2}=1$, and ${\mathbf{H}}_{\ell}$ stands for the channel matrix at time delay ℓ. Furthermore, ${\mathbf{H}}_{\ell},\phantom{\rule{0.277778em}{0ex}}\ell =0,1,\cdots ,L-1$ are mutually uncorrelated, Ricean distributed, and can be expressed as in Label (2)

$$\mathbf{y}=\sqrt{p}\mathbf{H}\mathbf{x}+\mathbf{z},$$

$$\mathbf{H}=\sum _{\ell =0}^{L-1}{\rho}_{\ell}{\mathbf{H}}_{\ell}exp(-j2\pi \frac{k}{K}\ell ),$$

$${\mathbf{H}}_{\ell}=\sqrt{{\overline{\kappa}}_{\ell}}{\overline{\mathbf{H}}}_{\ell}+\sqrt{{\tilde{\kappa}}_{\ell}}{\tilde{\mathbf{H}}}_{\ell}.$$

In particular, ${\overline{\mathbf{H}}}_{\ell}={\mathbf{r}}_{\ell}{\mathbf{t}}_{\ell}^{\mathtt{T}}$ is just as in Label (3) and ${\tilde{\mathbf{H}}}_{\ell}$ is also modeled as a random matrix consisting of i.i.d. elements.

## 3. LOS-Based EGT/EGC and Power Scaling Laws

#### 3.1. The Scenario without Correlation

The scattered component of k-th subcarrier’s channel matrix can be described as

$$\tilde{\mathbf{H}}=\sum _{\ell =0}^{L-1}{\rho}_{\ell}\sqrt{{\tilde{\kappa}}_{\ell}}{\tilde{\mathbf{H}}}_{\ell}exp(-j2\pi \frac{k}{K}\ell ).$$

Now, it is assumed that $\tilde{\mathbf{H}}$ is not available, but the LOS component
can be available. In what follows, by employing only $\overline{\mathbf{H}}$, we will present a linear processing scheme with EGT/EGC and then compare it with the MRT/MRC scheme based on the perfect CSI.

$$\overline{\mathbf{H}}=\sum _{\ell =0}^{L-1}{\rho}_{\ell}\sqrt{{\overline{\kappa}}_{\ell}}{\overline{\mathbf{H}}}_{\ell}exp(-j2\pi \frac{k}{K}\ell )$$

Since $\tilde{\mathbf{H}}$ is not available, a couple of the normalized weighting vectors ${\mathbf{w}}_{t}$ and ${\mathbf{w}}_{r}$ can be chosen in such a way that the effective output signal-to-noise ratio (SNR) can become maximum. The largest eigenvalue of matrix ${\overline{\mathbf{H}}}^{\u2020}\overline{\mathbf{H}}$ is now denoted by ${\lambda}_{max}({\overline{\mathbf{H}}}^{\u2020}\overline{\mathbf{H}})$. Due to the fact that ${\mathbf{w}}_{r}^{\u2020}{\mathbf{z}}^{k}\sim \mathtt{CN}(0,{\sigma}^{2})$, the effective output signal-to-interference-plus-noise ratio (SINR) can be described as

$${\gamma}_{S}^{(k)}=\frac{p|{\mathbf{w}}_{r}^{\u2020}\overline{\mathbf{H}}{\mathbf{w}}_{t}^{\mathtt{T}\u2020}{|}^{2}}{p|{\mathbf{w}}_{r}^{\u2020}\tilde{\mathbf{H}}{\mathbf{w}}_{t}^{\mathtt{T}\u2020}{|}^{2}+{\sigma}^{2}}=\frac{p{\lambda}_{max}({\overline{\mathbf{H}}}^{\u2020}\overline{\mathbf{H}})}{p|{\mathbf{w}}_{r}^{\u2020}\tilde{\mathbf{H}}{\mathbf{w}}_{t}^{\mathtt{T}\u2020}{|}^{2}+{\sigma}^{2}}.$$

We denote by ${R}_{S}$ the ergodic achievable rate of the LOS-based scheme. Then,
where ${R}_{S}^{(k)}=\mathbb{E}\{{log}_{2}(1+{\gamma}_{S}^{(k)})\}$. We have the following results through the derivation.

$${R}_{S}=\mathbb{E}\{\frac{1}{K}\sum _{k=0}^{K-1}{log}_{2}(1+{\gamma}_{S}^{(k)})\}=\frac{1}{K}\sum _{k=0}^{K-1}{R}_{S}^{(k)},$$

**Lemma**

**1.**

Define ${\lambda}_{max}^{(k)}={\lambda}_{max}({\overline{\mathbf{H}}}^{\u2020}\overline{\mathbf{H}})$ and ${\tilde{\kappa}}_{S}={\sum}_{\ell =0}^{L-1}{\rho}_{\ell}^{2}{\tilde{\kappa}}_{\ell}.$ Then,

$${log}_{2}(1+\frac{p{\lambda}_{max}^{(k)}}{p{\tilde{\kappa}}_{S}+{\sigma}^{2}})\le {R}_{S}^{(k)}\le {log}_{2}(1+\frac{p{\lambda}_{max}^{(k)}}{{\sigma}^{2}}).$$

**Proof**

**of**

**Lemma**

**1.**

Regarding the ergodic achievable rate of the k-th subcarrier, it is easy for us to derive its following lower bound with the help of the well-known Jensen’s inequality:
where ${\mathbb{E}}_{\ell}=\mathbb{E}{|{\mathbf{w}}_{r}^{\u2020}{\tilde{\mathbf{H}}}_{\ell}{\mathbf{w}}_{t}^{\mathtt{T}\u2020}|}^{2}={\tilde{\kappa}}_{\ell}$ for $0\le \ell \le L-1$. Thus,

$${R}_{S}^{(k)}\ge {log}_{2}(1+\frac{1}{\mathbb{E}(1/{\gamma}_{S}^{(k)})})={log}_{2}(1+\frac{p{\lambda}_{max}^{(k)}}{p{\sum}_{\ell =0}^{L-1}{\rho}_{\ell}^{2}{\mathbb{E}}_{\ell}+{\sigma}^{2}}),$$

$${R}_{C}^{k}\ge {log}_{2}(1+\frac{p{\lambda}_{max}^{(k)}}{p{\tilde{\kappa}}_{S}+{\sigma}^{2}}).$$

Moreover, we can obtain from Label (11) that

$${R}_{S}^{(k)}=\mathbb{E}{log}_{2}(1+\frac{p{\lambda}_{max}^{(k)}}{p|{\mathbf{w}}_{r}^{\u2020}\tilde{\mathbf{H}}{\mathbf{w}}_{t}^{\mathtt{T}\u2020}{|}^{2}+{\sigma}^{2}})\le {log}_{2}(1+\frac{p{\lambda}_{max}^{(k)}}{{\sigma}^{2}}).$$

Thus, Lemma 1 holds. □

**Lemma**

**2.**

Let ${\overline{\kappa}}_{U}={\sum}_{\ell =0}^{L-1}{\rho}_{\ell}^{2}{\overline{\kappa}}_{\ell}.$ and ${\overline{\kappa}}_{L}=max\{{\rho}_{\ell}^{2}{\overline{\kappa}}_{\ell},0\le \ell \le L-1\}.$ Then,

$${\overline{\kappa}}_{L}\le \underset{MN\to \infty}{lim}\frac{{\lambda}_{max}^{(k)}}{MN}\le {\overline{\kappa}}_{U}.$$

**Proof**

**of**

**Lemma**

**2.**

For $0\le \ell \le L-1$ and $0\le b\le L-1$, we define ${\phi}_{\ell b}=2\pi {d}_{r}(sin({\theta}_{b})-sin({\theta}_{\ell}))$, and then have that
where
and
with ${u}_{an}=\frac{1}{N}{e}^{2\pi {d}_{t}((a-1)sin({\theta}_{b})-(n-1)sin({\theta}_{\ell}))}.$ Now, suppose that $M\ge N$. Noting that ${lim}_{M\to \infty}{\varrho}_{\ell b}=0$ for $\ell \ne b$ and $\mathrm{tr}({\mathbf{U}}_{\ell \ell})=1$, we can obtain that

$$\frac{{\overline{\mathbf{H}}}_{\ell}^{\u2020}{\overline{\mathbf{H}}}_{b}}{MN}={\varrho}_{\ell b}{\mathbf{U}}_{\ell b},$$

$${\varrho}_{\ell b}=\frac{{\mathbf{r}}_{\ell}^{\u2020}{\mathbf{r}}_{b}}{M}=\left\{\begin{array}{cc}1,\hfill & \mathrm{for}\phantom{\rule{0.277778em}{0ex}}l=b;\hfill \\ \frac{1-{e}^{jM{\phi}_{\ell b}}}{M(1-{e}^{j{\phi}_{\ell b}})},\hfill & \mathrm{for}\phantom{\rule{0.277778em}{0ex}}\ell \ne b\hfill \end{array}\right.$$

$${\mathbf{U}}_{\ell b}=\frac{{\mathbf{t}}_{\ell}^{\mathtt{T}\u2020}{\mathbf{t}}_{b}^{\mathtt{T}}}{N}={[{u}_{an}]}_{a,n=1}^{N,N}$$

$$\underset{MN\to \infty}{lim}\frac{{\lambda}_{max}({\overline{\mathbf{H}}}^{\u2020}\overline{\mathbf{H}})}{MN}\le \sum _{\ell =0}^{L-1}{\rho}_{\ell}^{2}{\overline{\kappa}}_{\ell}\underset{MN\to \infty}{lim}{\lambda}_{max}(\frac{{\overline{\mathbf{H}}}_{\ell}^{\u2020}{\overline{\mathbf{H}}}_{\ell}}{MN})={\overline{\kappa}}_{U}.$$

Moreover, we also have
since, for any ℓ, we can get when ${\mathbf{w}}_{t}=\frac{{\mathbf{t}}_{\ell}}{\sqrt{N}}$ and ${\mathbf{w}}_{r}=\frac{{\mathbf{r}}_{\ell}}{\sqrt{M}}$

$$\underset{MN\to \infty}{lim}\frac{{\lambda}_{max}({\overline{\mathbf{H}}}^{\u2020}\overline{\mathbf{H}})}{MN}\ge {\overline{\kappa}}_{L}$$

$$\underset{MN\to \infty}{lim}\frac{{\lambda}_{max}({\overline{\mathbf{H}}}^{\u2020}\overline{\mathbf{H}})}{MN}\ge \underset{MN\to \infty}{lim}\frac{|{\mathbf{w}}_{r}^{\u2020}\tilde{\mathbf{H}}{\mathbf{w}}_{t}^{\mathtt{T}\u2020}{|}^{2}}{MN}={\overline{\kappa}}_{\ell}.$$

Therefore, Lemma 2 holds when $M\ge N$. When $N\ge M$, we can also similarly prove that Lemma 2 holds, based on the fact that ${\lambda}_{max}({\overline{\mathbf{H}}}^{\u2020}\overline{\mathbf{H}})={\lambda}_{max}(\overline{\mathbf{H}}{\overline{\mathbf{H}}}^{\u2020})$. □

**Proposition**

**1.**

If $E=MNp$ be fixed as $MN\to \infty $, then we have

$${log}_{2}(1+\frac{E{\overline{\kappa}}_{L}}{{\sigma}^{2}})\le \underset{MN\to \infty}{lim}{R}_{S}\le {log}_{2}(1+\frac{E{\overline{\kappa}}_{U}}{{\sigma}^{2}}).$$

**Proof**

**of**

**Proposition**

**1.**

If $E=MNp$ is fixed when $MN\to \infty $, we readily show that Proposition 1 holds by using Lemmas 1 and 2. □

**Remark**

**1.**

This proposition gives the lower and upper bounds of the ergodic achievable rate of the LOS-based scheme. In the following special cases, we can obtain further the exact expressions of the ergodic achievable rate.

**Corollary**

**1.**

When $N=1$, we have, if $E=Mp$ be fixed as $M\to \infty ,$

$$\underset{M\to \infty}{lim}{R}_{S}={log}_{2}(1+\frac{E{\overline{\kappa}}_{U}}{{\sigma}^{2}}).$$

Similarly, when $M=1$, we also have if $E=Np$ be fixed as $N\to \infty $

$$\underset{N\to \infty}{lim}{R}_{S}={log}_{2}(1+\frac{E{\overline{\kappa}}_{U}}{{\sigma}^{2}}).$$

**Proof**

**of**

**Corollary**

**1.**

When $M=1$ or $N=1$, due to the fact that ${lim}_{MN\to \infty}\frac{{\lambda}_{max}({\overline{\mathbf{H}}}^{\u2020}\overline{\mathbf{H}})}{MN}={\overline{\kappa}}_{U}$, it easily follows that ${lim}_{MN\to \infty}{R}_{S}={log}_{2}(1+\frac{E{\overline{\kappa}}_{U}}{{\sigma}^{2}})$. □

**Corollary**

**2.**

If $E=MNp$ be fixed as $M\to \infty $ and $N\to \infty $, then we have

$$\underset{M,N\to \infty}{lim}{R}_{S}={log}_{2}(1+\frac{E{\overline{\kappa}}_{L}}{{\sigma}^{2}}).$$

**Proof**

**of**

**Corollary**

**2.**

Without loss of generality, $\overline{\mathbf{H}}$ can be rewritten as
where ${\rho}_{0}\sqrt{{\overline{\kappa}}_{0}}\ge {\rho}_{1}\sqrt{{\overline{\kappa}}_{1}}\ge \cdots \ge {\rho}_{L-1}\sqrt{{\overline{\kappa}}_{L-1}}$. We can rewrite $\overline{\mathbf{H}}$ in a matrix form as
where $\mathbf{D}$ is a $L\times L$ diagonal matrix, ${[\mathbf{D}]}_{ll}={\rho}_{\ell}\sqrt{MN{\overline{\kappa}}_{\ell}}$, and ${\mathbf{A}}_{r}$ and ${\mathbf{A}}_{t}$ are defined as follows:
and

$$\overline{\mathbf{H}}=\sum _{\ell =0}^{L-1}{\rho}_{\ell}\sqrt{{\overline{\kappa}}_{\ell}}{\mathbf{r}}_{\ell}{\mathbf{t}}_{\ell}^{\mathtt{T}}exp(-j2\pi \frac{k}{K}\ell ),$$

$$\overline{\mathbf{H}}={\mathbf{A}}_{r}\mathbf{D}{\mathbf{A}}_{t}^{\mathtt{T}},$$

$${\mathbf{A}}_{r}=\frac{1}{\sqrt{M}}[{\mathbf{r}}_{0},{\mathbf{r}}_{1},\dots ,{\mathbf{r}}_{L-1}]$$

$${\mathbf{A}}_{t}=\frac{1}{\sqrt{N}}[{\mathbf{t}}_{0},{\mathbf{t}}_{1}exp(-j2\pi \frac{k}{K}),\dots ,{\mathbf{t}}_{L-1}exp(-j2\pi \frac{k}{K}(L-1))].$$

Since both $\{{\mathbf{r}}_{0},{\mathbf{r}}_{1},\dots ,{\mathbf{r}}_{L-1}\}$ and $\{{\mathbf{t}}_{0},{\mathbf{t}}_{1},\dots ,{\mathbf{t}}_{L-1}\}$ are orthogonal vector sets when $M\to \infty $ and $N\to \infty $ [21], ${\mathbf{A}}_{r}$ and ${\mathbf{A}}_{t}$ are asymptotically unitary matrices. For matrix $\overline{\mathbf{H}}$, thus we can form a singular value decomposition (SVD) as follows
where $\mathsf{\Sigma}$ is a diagonal matrix including all singular values on its diagonal, i.e.,

$$\overline{\mathbf{H}}=\mathbf{U}\mathsf{\Sigma}{\mathbf{V}}^{\u2020}=[{\mathbf{A}}_{r}|{\mathbf{A}}_{r}^{\perp}]\mathsf{\Sigma}{[{\mathbf{A}}_{t}|{\mathbf{A}}_{t}^{\perp}]}^{\mathtt{T}},$$

$${[\mathsf{\Sigma}]}_{ll}=\left\{\begin{array}{cc}{\rho}_{\ell}\sqrt{MN{\overline{\kappa}}_{\ell}},\hfill & \mathrm{for}\phantom{\rule{0.277778em}{0ex}}0\le l\le L-1,\hfill \\ 0,\hfill & \mathrm{for}\phantom{\rule{0.277778em}{0ex}}l>L-1.\hfill \end{array}\right.$$

Then,

$$\underset{M,N\to \infty}{lim}\frac{{\lambda}_{max}^{(k)}}{MN}={\rho}_{0}^{2}{\overline{\kappa}}_{0}={\overline{\kappa}}_{L}.$$

Thus, we finally obtain the desired result. □

On the other hand, suppose that the perfect CSI is known, i.e., both of the LOS and scattered components are available at the transmitter and the receiver. Then, the weighting vectors ${\mathbf{w}}_{t}$ and ${\mathbf{w}}_{r}$ should be chosen in such a way that the exact output SNR is maximized. Thus, the resulting output SNR can be written as [11]
where ${\lambda}_{max}({\mathbf{H}}^{\u2020}\mathbf{H})$ stands for the largest eigenvalue of ${\mathbf{H}}^{\u2020}\mathbf{H}$. For the MRT/MRC scheme based on the perfect CSI, let ${R}_{P}$ represent its ergodic achievable rate, i.e., ${R}_{P}=\mathbb{E}\{\frac{1}{K}{\sum}_{k=0}^{K-1}{log}_{2}(1+{\gamma}_{P}^{(k)})\}.$ Now, we obtain the following power scaling law.

$${\gamma}_{P}^{(k)}=\frac{p}{{\sigma}^{2}}{\lambda}_{max}({\mathbf{H}}^{\u2020}\mathbf{H}),$$

**Proposition**

**2.**

When $M\to \infty $ and $N\to \infty $, suppose that $E=MNp$ is fixed and $N/M\to \mu $. We have that

$$\underset{M,N\to \infty}{lim}{R}_{P}=\underset{M,N\to \infty}{lim}{R}_{S}.$$

**Proof**

**of**

**Proposition**

**2.**

Due to the fact $\mathbf{H}=\overline{\mathbf{H}}+\tilde{\mathbf{H}}$, we can have

$$\begin{array}{c}\frac{1}{M}[{\mathbf{H}}^{\u2020}\mathbf{H}]=\frac{1}{M}[{(\overline{\mathbf{H}}+\tilde{\mathbf{H}})}^{\u2020}(\overline{\mathbf{H}}+\tilde{\mathbf{H}})]\hfill \\ =\frac{{\overline{\mathbf{H}}}^{\u2020}\overline{\mathbf{H}}}{M}+\frac{{\overline{\mathbf{H}}}^{\u2020}\tilde{\mathbf{H}}}{M}+\frac{{\tilde{\mathbf{H}}}^{\u2020}\overline{\mathbf{H}}}{M}+\frac{{\tilde{\mathbf{H}}}^{\u2020}\tilde{\mathbf{H}}}{M}.\hfill \end{array}$$

If we let
it follows that

$$\mathbf{G}=\frac{{\overline{\mathbf{H}}}^{\u2020}\tilde{\mathbf{H}}}{M}={[{g}_{uv}]}_{u,v=1}^{N,N},$$

$${g}_{uv}=\frac{1}{M}\sum _{k=1}^{M}{[{\overline{\mathbf{H}}}^{\u2020}]}_{uk}{[\tilde{\mathbf{H}}]}_{kv}.$$

With the aid of (9) and (10), we can have that $|{[{\overline{\mathbf{H}}}^{\u2020}]}_{uk}{|}^{2}\le {\overline{\kappa}}_{S}\le 1$, and ${[\tilde{\mathbf{H}}]}_{kv}\sim \mathtt{CN}(0,{\delta}^{2})$ with ${\delta}^{2}={\tilde{\kappa}}_{S}\le 1$. As ${[\tilde{\mathbf{H}}]}_{kv}$, $1\le k\le M$ are independent each other, we know that

$${g}_{uv}\sim \mathtt{CN}(0,{\sigma}_{uv}^{2}),\phantom{\rule{0.277778em}{0ex}}\phantom{\rule{0.277778em}{0ex}}{\sigma}_{uv}^{2}\le \frac{1}{M}.$$

Thus, it can follow that, when $M\to \infty $, $\mathbf{G}\to \mathbf{Q},$ where $\mathbf{Q}$ denotes a matrix with all zero elements. Similarly, we can have that, if $M\to \infty ,$

$${\mathbf{G}}^{\u2020}=\frac{{\tilde{\mathbf{H}}}^{\u2020}\overline{\mathbf{H}}}{M}\to \mathbf{Q}.$$

Now, M is assumed to be large enough. Then, we certainly have that

$$\begin{array}{ccc}{\lambda}_{max}(\frac{{\mathbf{H}}^{\u2020}\mathbf{H}}{M})\hfill & =& {\lambda}_{max}(\frac{{\overline{\mathbf{H}}}^{\u2020}\overline{\mathbf{H}}}{M}+\frac{{\tilde{\mathbf{H}}}^{\u2020}\tilde{\mathbf{H}}}{M})\hfill \\ & \le & {\lambda}_{max}(\frac{{\overline{\mathbf{H}}}^{\u2020}\overline{\mathbf{H}}}{M})+{\lambda}_{max}(\frac{{\tilde{\mathbf{H}}}^{\u2020}\tilde{\mathbf{H}}}{M}).\hfill \end{array}$$

When $M\to \infty $, suppose that $N/M\to \mu $. Then, we easily derive from ([22], Theorem 2.37), only noting that ${[\tilde{H}]}_{mn}\sim \mathtt{CN}(0,{\tilde{\kappa}}_{S})$

$${\lambda}_{max}(\frac{1}{M}{\tilde{\mathbf{H}}}^{\u2020}\tilde{\mathbf{H}})\to {\tilde{\kappa}}_{S}{(1+\sqrt{\mu})}^{2}.$$

Thus, we further get

$${\lambda}_{max}(\frac{1}{MN}{\mathbf{H}}^{\u2020}\mathbf{H})\le {\lambda}_{max}(\frac{1}{MN}{\overline{\mathbf{H}}}^{\u2020}\overline{\mathbf{H}})+{\tilde{\kappa}}_{S}{(1+\sqrt{\mu})}^{2}/N.$$

In addition, we can obtain

$${\lambda}_{max}(\frac{1}{MN}{\mathbf{H}}^{\u2020}\mathbf{H})\ge {\lambda}_{max}(\frac{1}{MN}{\overline{\mathbf{H}}}^{\u2020}\overline{\mathbf{H}}).$$

When $M\to \infty $ and $N\to \infty $, we can get, by combining (44) with (45),

$${\lambda}_{max}(\frac{1}{MN}{\mathbf{H}}^{\u2020}\mathbf{H})\to \underset{M,N\to \infty}{lim}\frac{{\lambda}_{max}^{(k)}}{MN}.$$

It should be noticed that

$$\begin{array}{c}{R}_{P}=\frac{1}{K}\sum _{k=1}^{K}\mathbb{E}{log}_{2}(1+\frac{p}{{\sigma}^{2}}{\lambda}_{max}({\mathbf{H}}^{\u2020}(k)\mathbf{H}(k)))\hfill \\ =\frac{1}{K}\sum _{k=1}^{K}\mathbb{E}{log}_{2}(1+\frac{pMN}{{\sigma}^{2}}{\lambda}_{max}(\frac{{\mathbf{H}}^{\u2020}(k)\mathbf{H}(k)}{MN})).\hfill \end{array}$$

Therefore, when $M\to \infty $ and $N\to \infty $, if $E=pMN$ is fixed, we can have finally

$$\underset{M,N\to \infty}{lim}{R}_{P}=\underset{M,N\to \infty}{lim}{R}_{S}.$$

Thus, Proposition 2 holds. □

**Remark**

**2.**

This proposition implies that, when the two numbers of antennas at the transmitter and the receiver grow large with a fixed ratio, the ergodic achievable rate of the LOS-based scheme has the same asymptotic value as the ergodic achievable rate of the whole CSI-based scheme.

#### 3.2. The Scenario with Correlation

Now, we consider extending the proposed LOS-based ECT/EGC without spatial correlation to the scenario in which there exists doubly-ended spatial correlation. The MIMO system model presented in Section 2 is necessarily modified. ${\tilde{\mathbf{H}}}_{\ell},\ell =0,1,2,\cdots ,L-1$ is now modeled as doubly-correlated Rayleigh fading, with transmit and receive correlation matrices ${\mathsf{\Psi}}_{\ell}$ and ${\mathsf{\Phi}}_{\ell}$, i.e., [12],
where ${\tilde{\mathbf{H}}}_{\ell}^{\omega}$ is an i.i.d. matrix with each entry $\sim \mathtt{CN}(0,1)$. Since the scattered component of the channel matrix remains unchanged, the needed weighting vectors ${\mathbf{w}}_{t}$ and ${\mathbf{w}}_{r}$ should also remain unchanged. The ergodic achievable rate of the scenario with spatial correlation is denoted by

$${\tilde{\mathbf{H}}}_{\ell}={[{\mathsf{\Phi}}_{\ell}]}^{1/2}{\tilde{\mathbf{H}}}_{\ell}^{\omega}{[{\mathsf{\Psi}}_{\ell}]}^{1/2},$$

$${R}_{C}=\frac{1}{K}\sum _{k=0}^{K-1}{R}_{C}^{(k)},\phantom{\rule{0.277778em}{0ex}}\phantom{\rule{0.277778em}{0ex}}{R}_{C}^{(k)}=\mathbb{E}\{{log}_{2}(1+{\gamma}_{C}^{(k)})\}.$$

With respect to ${R}_{C}$, we have the following results by a similar derivation.

**Lemma**

**3.**

$${log}_{2}(1+\frac{p{\lambda}_{max}^{(k)}}{p{\tilde{\kappa}}_{C}+{\sigma}^{2}})\le {R}_{C}^{(k)}\le {log}_{2}(1+\frac{p{\lambda}_{max}^{(k)}}{{\sigma}^{2}}),$$

**Proposition**

**3.**

If $E=MNp$ is fixed as $MN\to \infty $, then

$$\underset{MN\to \infty}{lim}{R}_{C}=\underset{MN\to \infty}{lim}{R}_{S}.$$

**Remark**

**3.**

This proposition implies that the two ergodic achievable rates with and without spatial correlation have the same asymptotic value when $MN$ goes without bound.

## 4. Cooperative Relaying Systems

#### 4.1. The Scenario with Decode-and-Forward Protocol

Ricean fading often happens in cooperative MIMO systems [23]. Therefore, we can use a Ricean MIMO channel model to describe both the source-relay and relay-destination links. Still in frequency-selective Ricean fading environments, we especially study a classical cooperative relay system with a source node, a destination node and a relay node. The relay node can be equipped with a large-scale antenna array while both the source node and the destination node can be also equipped with a large-scale antenna array. The cooperative system with the three nodes is assumed to operate in a half-duplex mode, and the replay node employs the DF protocol for transmission. Each transmission for the system can be completed through two stages. Obviously, the cooperative system is a composite of two massive MIMO subsystems: one subsystem working at the first stage and the other subsystem at the second stage. Therefore, the rate analysis results mentioned above can be applied to the cooperative relay system.

We suppose that the relay makes use of M antennas to receive and transmit data and also suppose that the source has ${N}_{1}$ antennas and the destination has ${N}_{2}$ antennas. We denote the average transmitted power at the source and the relay by ${p}_{1}$ and ${p}_{2}$, respectively. In addition, we still let ${R}_{P}$ and ${R}_{S}$ represent the ergodic achievable rates for the whole CSI-based MRT/MRC scheme and the LOS-based EGT/EGC scheme, respectively. Then, we can obtain the following power scaling property for the cooperative system.

**Proposition**

**4.**

When $M\to \infty $ and ${N}_{1}\to \infty $, let ${E}_{1}=M{N}_{1}{p}_{1}$ be fixed and ${N}_{1}/M\to {\mu}_{1}$ for the source-relay link. When $M\to \infty $ and ${N}_{2}\to \infty $, let ${E}_{2}=M{N}_{2}{p}_{2}$ be fixed and ${N}_{2}/M\to {\mu}_{2}$ for the relay-destination link. Then,

$$\underset{M,{N}_{1},{N}_{2}\to \infty}{lim}{R}_{P}=\underset{M,{N}_{1},{N}_{2}\to \infty}{lim}{R}_{S}.$$

**Proof**

**of**

**Proposition**

**4.**

From [24], it follows that the ergodic achievable rate with the perfect SCI-based MRT/MRC is written as
where ${R}_{P}^{(1)}$ and ${R}_{P}^{(2)}$ are the corresponding ergodic achievable rates of the source-relay and relay-destination transmission links, respectively. Similarly, we also have that the ergodic achievable rate with the only LOS-based EGT/EGC can be given by
where ${R}_{S}^{(1)}$ and ${R}_{S}^{(2)}$ are the corresponding ergodic achievable rates of the source-relay and relay-destination transmission links, respectively. Under the condition of Proposition 4, we get by Proposition 2
and

$${R}_{P}=min\{{R}_{P}^{(1)}/2,{R}_{P}^{(2)}/2\},$$

$${R}_{S}=min\{{R}_{S}^{(1)}/2,{R}_{S}^{(2)}/2\},$$

$$\underset{M,{N}_{1}\to \infty}{lim}{R}_{P}^{(1)}=\underset{M,{N}_{1}\to \infty}{lim}{R}_{S}^{(1)}$$

$$\underset{M,{N}_{2}\to \infty}{lim}{R}_{P}^{(2)}=\underset{M,{N}_{2}\to \infty}{lim}{R}_{S}^{(2)}.$$

Thus, it is easy to obtain the desired result (53). □

**Remark**

**4.**

This proposition implies that, when the number of source antennas and the two numbers of relay antennas at the transmitter and the receiver grow large with fixed ratios, the ergodic achievable rate of the LOS-based scheme also has the same asymptotic value as the ergodic achievable rate of the whole CSI-based scheme.

#### 4.2. The Scenario with Amplify-and-Forward Protocol

The DF is a regenerative relaying transmission strategy. Now, we consider employing a nonregenerative strategy involving AF to replace the DF. Then, we can have a power scaling law as follows.

**Proposition**

**5.**

Suppose that ${N}_{1}={N}_{2}=1$. When $M\to \infty $, let ${E}_{1}=M{p}_{1}$ and ${E}_{2}=M{N}_{2}{p}_{2}$ be fixed. Then,

$$\underset{M\to \infty}{lim}{R}_{S}={log}_{2}(1+(\frac{{E}_{1}{\overline{\kappa}}_{U1}}{{\sigma}_{1}^{2}}\xb7\frac{{E}_{2}{\overline{\kappa}}_{U2}}{{\sigma}_{2}^{2}})/(\frac{{E}_{1}{\overline{\kappa}}_{U1}}{{\sigma}_{1}^{2}}+\frac{{E}_{2}{\overline{\kappa}}_{U2}}{{\sigma}_{2}^{2}}+1)).$$

**Proof**

**of**

**Proposition**

**5.**

We denote by ${\gamma}_{S1}^{(k)}$ and ${\gamma}_{S2}^{(k)}$ the output instantaneous SNR of the source-relay and relay-destination links, respectively. From [25], we obtain that

$$\begin{array}{ccc}{R}_{S}\hfill & =& \frac{1}{K}\sum _{k=0}^{K-1}\mathbb{E}\{{log}_{2}(1+{\gamma}_{S}^{(k)})\}\hfill \\ & =& \frac{1}{K}\sum _{k=0}^{K-1}\mathbb{E}\{{log}_{2}(1+({\gamma}_{S1}^{(k)}\xb7{\gamma}_{S2}^{(k)})/({\gamma}_{S1}^{(k)}+{\gamma}_{S2}^{(k)}+1))\}.\hfill \end{array}$$

Based on the proof of Lemma 2, we can have the following asymptotical SNR expressions
and

$$\underset{M\to \infty}{lim}{\gamma}_{S1}^{(k)}=\frac{{E}_{1}{\overline{\kappa}}_{U1}}{{\sigma}_{1}^{2}}$$

$$\underset{M\to \infty}{lim}{\gamma}_{S2}^{(k)}=\frac{{E}_{1}{\overline{\kappa}}_{U2}}{{\sigma}_{2}^{2}}$$

Thus, the power scaling law (58) holds. □

## 5. Simulation Results

For OFDM-MIMO systems in frequency-selective Ricean fading channels, we in this section provide our analytical results and simulation results. In all simulations, we assume that all of these spacings between adjacent antennas at the transmitter and the receiver are $0.5$. We set the number of subcarriers $K=256$, the channel delay spread $L=3$, and the noise variance as ${\sigma}^{2}=1$. In addition, we let ${\rho}_{0}^{2}={\rho}_{1}^{2}={\rho}_{2}^{2}=1/3$, ${\theta}_{0}={\varphi}_{0}=\pi /6$, ${\theta}_{1}={\varphi}_{1}=\pi /4$, and ${\theta}_{2}={\varphi}_{2}=\pi /3$. In Figure 1 and Figure 2, the Ricean K-factor $\kappa $ is fixed and is equal to $5\phantom{\rule{0.277778em}{0ex}}\mathrm{dB}$.

In order to verify Propositions 1 and 3, we consider firstly the scenario with spatial correlation when $N=3$ and $E=20\phantom{\rule{0.277778em}{0ex}}\mathrm{dB}$. The spatial correlation among antennas is assumed to follow the exponential model, i.e., the correlation magnitude between antenna p and q can be determined by $c(p,q)={g}^{|p-q|}$, where g denotes the correlation coefficient [12]. Therefore, we represent the correlation matrices $(i,j)$-th of ${\mathsf{\Phi}}_{\ell}$ by ${[{\mathsf{\Phi}}_{\ell}]}_{ij}={({g}_{r}^{\ell})}^{|i-j|}$ and $(i,j)$-th of ${\mathsf{\Psi}}_{\ell}$ by ${[{\mathsf{\Psi}}_{\ell}]}_{ij}={({g}_{t}^{\ell})}^{|i-j|}$, respectively, $\ell =0,1,2$. Moreover, we set ${g}_{r}^{0}={g}_{r}^{1}={g}_{r}^{2}={g}_{r}$ and ${g}_{t}^{0}={g}_{t}^{1}={g}_{t}^{2}={g}_{t}$. For the correlation coefficients ${g}_{t}={g}_{r}=g=0,0.3,0.6,0.9$, as M increases from 6 to 60, Figure 1 provides a curve of the exact average rate ${R}_{C}$ and two curves of the upper and lower bounds of ${R}_{S}$. It can be observed that the exact ergodic rate ${R}_{C}$ increases as the number of receive antenna M grows large, and is always between the two bounds of ${R}_{S}$. As both of the correlation coefficients $({g}_{t},{g}_{r})$ increase, ${R}_{C}$ is closer to the upper bound, and becomes higher and higher than ${R}_{S}$. This indicates that, compared to the uncorrelated scenario, the presence of spatial correlation results in improving the rate performance under the LOS-based EGT/EGC scheme. Therefore, if the LOS-based scheme can be employed, we can achieve performance benefits from the spatial correlation, which is obviously different from the traditional point of view. This implies that it would be practical if a large-scale antenna array is compactly arranged.

Next, we consider validating Proposition 2. For that, we need to compare the ergodic achievable rate of the proposed LOS-based EGT/EGC scheme with that of the perfect CSI-based MRT/MRC scheme. We set $\mu =1/2$ when the numbers of antennas at the transmitter and receiver grow large. For the parameter $E=10,20,30\phantom{\rule{0.277778em}{0ex}}\mathrm{dB}$, as M increases from 6 to 60, Figure 2 plots the two ergodic achievable rates, ${R}_{S}$ and ${R}_{P}$. It can be found from Figure 2 that both of the ergodic achievable rates can tend to the same limit results for the given values of E. However, with an increase of E, the speed of rate convergence appears to be slower and slower.

Finally, we pay our attention to the classical DF cooperative relay system consisting of the source-relay and relay-destination links and set the identical parameters mentioned above in the two links. When ${N}_{1}={N}_{2}=6$, as M increases from 6 to 60, Figure 3 plots the two average rates ${R}_{S}$ and ${R}_{P}$ for $\kappa =5,15\phantom{\rule{0.277778em}{0ex}}\mathrm{dB}$. It can be found from Figure 3 that, with an increasing $\kappa $, both ${R}_{S}$ and ${R}_{P}$ improve and ${R}_{S}$ is closer to ${R}_{P}$. It should be noticed that ${R}_{P}$ denotes the average rate for the traditional linear processing scheme based on the whole CSI as considered in [6]. For obtaining a comprehensive comparison with the scheme based on the whole CSI in Rayleigh fading discussed in [24], Figure 3 also includes a rate curve which corresponds to $\kappa =-\infty \phantom{\rule{0.277778em}{0ex}}\mathrm{dB}$. Interestingly, with $\kappa =5\phantom{\rule{0.277778em}{0ex}}\mathrm{dB}$, the LOS-based scheme always obviously outperforms the scheme based on the whole CSI in Rayleigh fading.

## 6. Conclusions

In this paper, we have developed the transmission scheme of LOS-based EGT/EGC for point-to-point massive-MIMO systems in frequency-selective Ricean fading channels without and with spatial correlation. In particular, we have derived expressions of the system achievable rate and determined several power scaling laws. In addition, we have also generalized our analysis to the cooperative relaying scenarios with DF and AF protocols, respectively. It is shown by our simulation results that the spatial correlation can improve the system performance and thus is an advantage, which is contrary to the traditional point of view. Compared to the Rayleigh fading environments, deployment of large scale antenna arrays in Ricean fading environments would be more suitable. For instance, massive MIMO can be applied in microwave backhaul links [26].

## Author Contributions

Formal Analysis, Q.Y.; Validation, Y.S.; Writing—Original Draft Preparation, Q.Y., Y.S.; Writing—Review and Editing, D.-W.Y.; Supervision, D.-W.Y.

## Funding

This research was funded by the open research fund of State Key Laboratory of Integrated Services Networks, the Fundamental Research Funds for the Central Universities Grant No. 3132016347, and the Natural Science Foundation of Liaoning Province Grant No. 201602086.

## Conflicts of Interest

The authors declare no conflict of interest.

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**Figure 1.**The ergodic achievable rate versus the number of receive antennas for comparing the case with correlation and the case without correlation.

**Figure 2.**The ergodic achievable rate versus the number of receive antennas for comparing the LOS-based scheme with the whole CSI-based scheme.

**Figure 3.**The ergodic achievable rate versus the number of relay antennas for comparing the case with Ricean fading and the case with Rayleigh fading.

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