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

Open Access 01-12-2009 | Research Article

Achievable Rates and Resource Allocation Strategies for Imperfectly Known Fading Relay Channels

Authors: Junwei Zhang, Mustafa Cenk Gursoy

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

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Abstract

Achievable rates and resource allocation strategies for imperfectly known fading relay channels are studied. It is assumed that communication starts with the network training phase in which the receivers estimate the fading coefficients. Achievable rate expressions for amplify-and-forward and decode-and-forward relaying schemes with different degrees of cooperation are obtained. We identify efficient strategies in three resource allocation problems: (1) power allocation between data and training symbols, (2) time/bandwidth allocation to the relay, and (3) power allocation between the source and relay in the presence of total power constraints. It is noted that unless the source-relay channel quality is high, cooperation is not beneficial and noncooperative direct transmission should be preferred at high signal-to-noise ratio (SNR) values when amplify-and-forward or decode-and-forward with repetition coding is employed as the cooperation strategy. On the other hand, relaying is shown to generally improve the performance at low SNRs. Additionally, transmission schemes in which the relay and source transmit in nonoverlapping intervals are seen to perform better in the low-SNR regime. Finally, it is noted that care should be exercised when operating at very low SNR levels, as energy efficiency significantly degrades below a certain SNR threshold value.

1. Introduction

In wireless communications, deterioration in performance is experienced due to various impediments such as interference, fluctuations in power due to reflections and attenuation, and randomly-varying channel conditions caused by mobility and changing environment. Recently, cooperative wireless communication has attracted much interest as a technique that can mitigate these degradations and provide higher rates or improve the reliability through diversity gains. The relay channel was first introduced by van der Meulen in [1], and initial research was primarily conducted to understand the rates achieved in relay channels [2, 3]. More recently, diversity gains of cooperative transmission techniques have been studied in [47]. In [6], several cooperative protocols have been proposed, with amplify-and-forward (AF) and decode-and-forward (DF) being the two basic relaying schemes. The performance of these protocols are characterized in terms of outage events and outage probabilities. In [8], three different time-division AF and DF cooperative protocols with different degrees of broadcasting and receive collision are studied. Resource allocation for relay channel and networks has been addressed in several studies (see, e.g., [914]). In [9], upper and lower bounds on the outage and ergodic capacities of relay channels are obtained under the assumption that the channel side information (CSI) is available at both the transmitter and receiver. Power allocation strategies are explored in the presence of a total power constraint on the source and relay. In [10], under again the assumption of the availability of CSI at the receiver and transmitter, optimal dynamic resource allocation methods in relay channels are identified under total average power constraints and delay limitations by considering delay-limited capacities and outage probabilities as performance metrics. In [11], resource allocation schemes in relay channels are studied in the low-power regime when only the receiver has perfect CSI. Liang et al. in [12] investigated resource allocation strategies under separate power constraints at the source and relay nodes and showed that the optimal strategies differ depending on the channel statics and the values of the power constraints. Recently, the impact of channel state information (CSI) and power allocation on rates of transmission over fading relay channels are studied in [14] by Ng and Goldsmith. The authors analyzed the cases of full CSI and receiver only CSI, considered the optimum or equal power allocation between the source and relay nodes, and identified the best strategies in different cases. In general, the area has seen an explosive growth in the number of studies (see additionally, e.g., [1517], and references therein). An excellent review of cooperative strategies from both rate and diversity improvement perspectives is provided in [18] in which the impacts of cooperative schemes on device architecture and higher-layer wireless networking protocols are also addressed. Recently, a special issue has been dedicated to models, theory, and codes for relaying and cooperation in communication networks in [19].
As noted above, studies on relaying and cooperation are numerous. However, most work has assumed that the channel conditions are perfectly known at the receiver and/or transmitter sides. Especially in mobile applications, this assumption is unwarranted as randomly varying channel conditions can be learned by the receivers only imperfectly. Moreover, the performance analysis of cooperative schemes in such scenarios is especially interesting and called for because relaying introduces additional channels and hence increases the uncertainty in the model if the channels are known only imperfectly. Recently, Wang et al. in [20] considered pilot-assisted transmission over wireless sensory relay networks and analyzed scaling laws achieved by the amplify-and-forward scheme in the asymptotic regimes of large nodes, large block length, and small signal-to-noise ratio (SNR) values. In this study, the channel conditions are being learned only by the relay nodes. In [21, 22], estimation of the overall source-relay-destination channel is addressed for amplify-and-forward relay channels. In [21], Gao et al. considered both the least squares (LSs) and minimum-mean-square error (MMSE) estimators and provided optimization formulations and guidelines for the design of training sequences and linear precoding matrices. In [22], under the assumption of fixed power allocation between data transmission and training, Patel and Stüber analyzed the performance of linear MMSE estimation in relay channels. In [21, 22], the training design is studied in an estimation-theoretic framework, and mean-square errors and bit error rates, rather than the achievable rates, are considered as performance metrics. To the best of our knowledge, performance analysis and resource allocation strategies have still not been sufficiently addressed for imperfectly-known relay channels in an information-theoretic context by considering rate expressions. We note that Avestimehr and Tse in [23] studied the outage capacity of slow fading relay channels. They showed that Bursty Amplify-Forward strategy achieves the outage capacity in the low-SNR and low outage probability regime. Interestingly, they further proved that the optimality of Bursty AF is preserved even if the receivers do not have prior knowledge of the channels.
In this paper, we study the imperfectly-known fading relay channels. We assume that transmission takes place in two phases: network training phase and data transmission phase. In the network training phase, a priori unknown fading coefficients are estimated at the receivers with the assistance of pilot symbols. Following the training phase, AF and DF relaying techniques are employed in the data transmission. Our contributions in this paper are the following.
(1)
We obtain achievable rate expressions for AF and DF relaying protocols with different degrees of cooperation, ranging from noncooperative communications to full cooperation. We provide a unified analysis that applies to both overlapped and nonoverlapped transmissions of the source and relay. We note that achievable rates are obtained by considering the ergodic scenario in which the transmitted codewords are assumed to be sufficiently long to span many fading realizations.
 
(2)
We identify resource allocation strategies that maximize the achievable rates. We consider three types of resource allocation problems:
(a)
power allocation between data and training symbols,
 
(b)
time/bandwidth allocation to the relay,
 
(c)
power allocation between the source and relay if there is a total power constraint in the system.
 
 
(3)
We investigate the energy efficiency in imperfectly-known relay channels by finding the bit energy requirements in the low-SNR regime.
 
The organization of the rest of the paper is as follows. In Section 2, we describe the channel model. Network training and data transmission phases are explained in Section 3. We obtain the achievable rate expressions in Section 4 and study the resource allocation strategies in Section 5. We discuss the energy efficiency in the low-SNR regime in Section 6. Finally, we provide conclusions in Section 6. The proofs of the achievable rate expressions are relegated to the appendix.

2. Channel Model

We consider a three-node relay network which consists of a source, destination, and a relay node. This relay network model is depicted in Figure 1. Source-destination, source-relay, and relay-destination channels are modeled as Rayleigh block-fading channels with fading coefficients denoted by https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq1_HTML.gif , https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq2_HTML.gif , and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq3_HTML.gif , respectively, for each channel. Due to the block-fading assumption, the fading coefficients https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq4_HTML.gif , https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq5_HTML.gif , and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq6_HTML.gif stay constant for a block of https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq7_HTML.gif symbols before they assume independent realizations for the following block. ( https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq8_HTML.gif is used to denote a proper complex Gaussian random variable with mean https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq9_HTML.gif and variance https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq10_HTML.gif . ) In this system, the source node tries to send information to the destination node with the help of the intermediate relay node. It is assumed that the source, relay, and destination nodes do not have prior knowledge of the realizations of the fading coefficients. The transmission is conducted in two phases: network training phase in which the fading coefficients are estimated at the receivers, and data transmission phase. Overall, the source and relay are subject to the following power constraints in one block:
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_Equ1_HTML.gif
(1)
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_Equ2_HTML.gif
(2)
where https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq11_HTML.gif and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq12_HTML.gif are the training symbols sent by the source and relay, respectively, and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq13_HTML.gif and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq14_HTML.gif are the corresponding source and relay data vectors. The pilot symbols enable the receivers to obtain the minimum mean-square error (MMSE) estimates of the fading coefficients. Since MMSE estimates depend only on the total training power but not on the training duration, transmission of a single pilot symbol is optimal for average-power limited channels. The transmission structure in each block is shown in Figure 2. As observed immediately, the first two symbols are dedicated to training while data transmission occurs in the remaining duration of https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq15_HTML.gif symbols. Detailed description of the network training and data transmission phases is provided in the following section.

3. Network Training and Data Transmission

3.1. Network Training Phase

Each block transmission starts with the training phase. In the first symbol period, source transmits the pilot symbol https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq17_HTML.gif to enable the relay and destination to estimate the channel coefficients https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq18_HTML.gif and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq19_HTML.gif , respectively. The signals received by the relay and destination are
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_Equ3_HTML.gif
(3)
respectively. Similarly, in the second symbol period, relay transmits the pilot symbol https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq20_HTML.gif to enable the destination to estimate the channel coefficient https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq21_HTML.gif . The signal received by the destination is
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_Equ4_HTML.gif
(4)
In the above formulations, https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq22_HTML.gif , https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq23_HTML.gif , and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq24_HTML.gif represent independent Gaussian random variables. Note that https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq25_HTML.gif and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq26_HTML.gif are Gaussian noise samples at the destination in different time intervals, while https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq27_HTML.gif is the Gaussian noise at the relay.
In the training process, it is assumed that the receivers employ minimum mean-square-error (MMSE) estimation. We assume that the source allocates https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq28_HTML.gif fraction of its total power https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq29_HTML.gif for training while the relay allocates https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq30_HTML.gif fraction of its total power https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq31_HTML.gif for training. As described in [24], the MMSE estimate of https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq32_HTML.gif is given by
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_Equ5_HTML.gif
(5)
where https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq33_HTML.gif . We denote by https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq34_HTML.gif the estimate error which is a zero-mean complex Gaussian random variable with variance https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq35_HTML.gif Similarly, for the fading coefficients https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq36_HTML.gif and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq37_HTML.gif , we have the following estimates and estimate error variances:
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_Equ6_HTML.gif
(6)
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_Equ7_HTML.gif
(7)
With these estimates, the fading coefficients can now be expressed as
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_Equ8_HTML.gif
(8)

3.2. Data Transmission Phase

As discussed in the previous section, within a block of https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq38_HTML.gif symbols, the first two symbols are allocated to network training. In the remaining duration of https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq39_HTML.gif symbols, data transmission takes place. Throughout the paper, we consider several transmission protocols which can be classified into two categories depending on whether or not the source and relay simultaneously transmit information: nonoverlapped and overlapped transmissions. Since the practical relay node usually cannot transmit and receive data simultaneously, we assume that the relay works under half-duplex constraint. Hence, the relay first listens and then transmits. We introduce the relay transmission parameter https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq40_HTML.gif and assume that https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq41_HTML.gif symbols are allocated for relay transmission. Hence, https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq42_HTML.gif can be seen as the fraction of total time or bandwidth allocated to the relay. Note that the parameter https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq43_HTML.gif enables us to control the degree of cooperation. In nonoverlapped transmission protocol, source and relay transmit over nonoverlapping intervals. Therefore, source transmits over a duration of https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq44_HTML.gif symbols and becomes silent as the relay transmits. On the other hand, in overlapped transmission protocol, source transmits all the time and sends https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq45_HTML.gif symbols in each block.
We assume that the source transmits at a per-symbol power level of https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq46_HTML.gif when the relay is silent, and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq47_HTML.gif when the relay is in transmission. Clearly, in nonoverlapped mode, https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq48_HTML.gif . On the other hand, in overlapped transmission, we assume https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq49_HTML.gif . Noting that the total power available after the transmission of the pilot symbol is https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq50_HTML.gif , we can write
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_Equ9_HTML.gif
(9)
The above assumptions imply that power for data transmission is equally distributed over the symbols during the transmission periods. Hence, in nonoverlapped and overlapped modes, the symbol powers are https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq51_HTML.gif and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq52_HTML.gif , respectively. Furthermore, we assume that the power of each symbol transmitted by the relay node is https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq53_HTML.gif , which satisfies, similarly as above,
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_Equ10_HTML.gif
(10)
Next, we provide detailed descriptions of nonoverlapped and overlapped cooperative transmission schemes.

3.2.1. Nonoverlapped Transmission

We first consider the two simplest cooperative protocols: nonoverlapped AF where the relay amplifies the received signal and forwards it to the destination, and nonoverlapped DF with repetition coding where the relay decodes the message, reencodes it using the same codebook as the source, and forwards it. In these protocols, since the relay either amplifies the received signal or decodes it but uses the same codebook as the source when forwarding, source and relay should be allocated equal time slots in the cooperation phase. Therefore, before cooperation starts, we initially have direct transmission from the source to the destination without any aid from the relay over a duration of https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq54_HTML.gif symbols. In this phase, source sends the https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq55_HTML.gif -dimensional data vector https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq56_HTML.gif and the received signal at the destination is given by
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_Equ11_HTML.gif
(11)
Subsequently, cooperative transmission starts. At first, the source transmits the https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq57_HTML.gif -dimensional data vector https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq58_HTML.gif which is received at the the relay and the destination, respectively, as
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_Equ12_HTML.gif
(12)
In (11) and (12), https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq59_HTML.gif and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq60_HTML.gif are independent Gaussian noise vectors composed of independent and identically distributed (i.i.d.), circularly symmetric, zero-mean complex Gaussian random variables with variance https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq61_HTML.gif , modeling the additive background noise at the transmitter in different transmission phases. Similarly, https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq62_HTML.gif is a Gaussian noise vector at the relay, whose components are i.i.d. zero-mean Gaussian random variables with variance https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq63_HTML.gif . For compact representation, we denote the overall source data vector by https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq64_HTML.gif and the signal received at the destination directly from the source by https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq65_HTML.gif where https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq66_HTML.gif denotes the transpose operation. After completing its transmission, the source becomes silent, and the relay transmits an https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq67_HTML.gif -dimensional symbol vector https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq68_HTML.gif which is generated from the previously received https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq69_HTML.gif [6, 7]. Now, the destination receives
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_Equ13_HTML.gif
(13)
After substituting the estimate expressions in (8) into (11)–(13), we have
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_Equ14_HTML.gif
(14)
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_Equ15_HTML.gif
(15)
Note that we have https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq70_HTML.gif for AF and repetition coding DF. Therefore, https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq71_HTML.gif models full cooperation while we have noncooperative communications as https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq72_HTML.gif . It should also be noted that https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq73_HTML.gif should in general be chosen such that https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq74_HTML.gif is an integer. The transmission structure and order in the data transmission phase of nonoverlapped AF and repetition DF are depicted in Figure 3(a), together with the notation used for the data symbols sent by the source and relay.
For nonoverlapped transmission, we also consider DF with parallel channel coding, in which the relay uses a different codebook to encode the message. In this case, the source and relay do not have to be allocated the same duration in the cooperation phase. Therefore, source transmits over a duration of https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq75_HTML.gif symbols while the relay transmits in the remaining duration of https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq76_HTML.gif symbols. Clearly, the range of https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq77_HTML.gif is now https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq78_HTML.gif . In this case, the input-output relations are given by (12) and (13). Since there is no separate direct transmission, https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq79_HTML.gif and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq80_HTML.gif in (12). Moreover, the dimensions of the vectors https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq81_HTML.gif and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq82_HTML.gif are now https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq83_HTML.gif , while https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq84_HTML.gif and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq85_HTML.gif are vectors of dimension https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq86_HTML.gif . Figure 3(b) provides a graphical description of the transmission order for nonoverlapped parallel DF scheme.

3.2.2. Overlapped Transmission

In this category, we consider a more general and complicated scenario in which the source transmits all the time. We study AF and repetition DF, in which we, similarly as in the nonoverlapped model, have unaided direct transmission from the source to the destination in the initial duration of https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq87_HTML.gif symbols. Cooperative transmission takes place in the remaining duration of https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq88_HTML.gif symbols. Again, we have https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq89_HTML.gif in this setting. In these protocols, the input-output relations are expressed as follows:
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_Equ16_HTML.gif
(16)
Above, https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq90_HTML.gif and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq91_HTML.gif , which have respective dimensions of https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq92_HTML.gif , https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq93_HTML.gif and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq94_HTML.gif , represent the source data vectors sent in direct transmission, cooperative transmission when relay is listening, and cooperative transmission when relay is transmitting, respectively. Note again that the source transmits all the time. https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq95_HTML.gif is the relay's data vector with dimension https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq96_HTML.gif . https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq97_HTML.gif and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq98_HTML.gif are the corresponding received vectors at the destination, and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq99_HTML.gif is the received vector at the relay. The input vector https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq100_HTML.gif now is defined as https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq101_HTML.gif and we again denote https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq102_HTML.gif . If we express the fading coefficients as https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq103_HTML.gif in (16), we obtain the following input-output relations:
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_Equ17_HTML.gif
(17)
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_Equ18_HTML.gif
(18)
A graphical depiction of the transmission order for overlapped AF and repetition DF is given in Figure 3(c).
Finally, the list of notations used throughout the paper is given in Table 1.
Table 1
List of notations.
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq104_HTML.gif
Source-destination channel fading coefficient
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq105_HTML.gif
Relay-destination channel fading coefficient
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq106_HTML.gif
Relay-destination channel fading coefficient
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq107_HTML.gif
Estimate of the fading coefficient https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq108_HTML.gif
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq109_HTML.gif
Error in the estimate of the fading coefficient https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq110_HTML.gif
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq111_HTML.gif
Variance of random variables
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq112_HTML.gif
Variance of Gaussian random variables due to thermal noise
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq113_HTML.gif
Number of symbols in each block
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq114_HTML.gif
Total average power of the source in each block of https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq115_HTML.gif symbols
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq116_HTML.gif
Total average power of the relay in each block of https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq117_HTML.gif symbols
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq118_HTML.gif
Fraction of total power allocated to training by the source
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq119_HTML.gif
Fraction of total power allocated to training by the relay
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq120_HTML.gif
Pilot symbol sent by the source
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq121_HTML.gif
Pilot symbol sent by the relay
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq122_HTML.gif
Additive Gaussian noise at the destination in the interval in which the source pilot symbol is sent
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq123_HTML.gif
Additive Gaussian noise at the relay in the interval in which the source pilot symbol is sent
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq124_HTML.gif
Additive Gaussian noise at the destination in the interval in which the relay pilot symbol is sent
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq125_HTML.gif
Received signal at the destination in the interval in which the source pilot symbol is sent
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq126_HTML.gif
Received signal at the relay in the interval in which the source pilot symbol is sent
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq127_HTML.gif
Received signal at the destination in the interval in which the relay pilot symbol is sent
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq128_HTML.gif
Power of each source symbol sent in the interval in which the relay is not transmitting
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq129_HTML.gif
Power of each source symbol sent in the interval in which the relay is transmitting
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq130_HTML.gif
Power of each relay symbol
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq131_HTML.gif
Fraction of time/bandwidth allocated to the relay
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq132_HTML.gif
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq133_HTML.gif -dimensional data vector sent by the source in the noncooperative transmission mode
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq134_HTML.gif
Data vector sent by the source when the relay is listening. The dimension is https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq135_HTML.gif for AF and repetition DF, and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq136_HTML.gif for parallel DF
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq137_HTML.gif
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq138_HTML.gif -dimensional data vector sent by the source when the relay is transmitting
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq139_HTML.gif
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq140_HTML.gif -dimensional data vector sent by the relay
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq141_HTML.gif
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq142_HTML.gif -dimensional noise vector at the destination in the noncooperative transmission mode
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq143_HTML.gif
Noise vector at the destination in the interval when the relay is listening. The dimension is https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq144_HTML.gif for AF and repetition DF, and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq145_HTML.gif for parallel DF
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq146_HTML.gif
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq147_HTML.gif -dimensional noise vector at the destination in the interval when the relay is transmitting
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq148_HTML.gif
Noise vector at the relay. The dimension is https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq149_HTML.gif for AF and repetition DF, and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq150_HTML.gif for parallel DF
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq151_HTML.gif
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq152_HTML.gif -dimensional received vector at the destination in the noncooperative transmission mode
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq153_HTML.gif
Received vector at the destination in the interval when the relay is listening. The dimension is https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq154_HTML.gif for AF and repetition DF, and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq155_HTML.gif for parallel DF
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq156_HTML.gif
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq157_HTML.gif -dimensional received vector at the destination in the interval when the relay is transmitting
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq158_HTML.gif
Received vector at the relay. The dimension is https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq159_HTML.gif for AF and repetition DF, and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq160_HTML.gif for parallel DF

4. Achievable Rates

In this section, we provide achievable rate expressions for AF and DF relaying in both nonoverlapped and overlapped transmission scenarios in a unified fashion. Achievable rate expressions are obtained by considering the estimate errors as additional sources of Gaussian noise. Since Gaussian noise is the worst uncorrelated additive noise for a Gaussian model [25, Appendix], [26], achievable rates given in this section can be regarded as worst-case rates.
We first consider AF relaying scheme. The capacity of the AF relay channel is the maximum mutual information between the transmitted signal https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq161_HTML.gif and received signals https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq162_HTML.gif and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq163_HTML.gif given the estimates https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq164_HTML.gif  and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq165_HTML.gif :
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_Equ19_HTML.gif
(19)
Note that this formulation presupposes that the destination has the knowledge of https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq166_HTML.gif . Hence, we assume that the value of https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq167_HTML.gif is forwarded reliably from the relay to the destination over low-rate control links. In general, solving the optimization problem in (19) and obtaining the AF capacity is a difficult task. Therefore, we concentrate on finding a lower bound on the capacity. A lower bound is obtained by replacing the product of the estimate error and the transmitted signal in the input-output relations with the worst-case noise with the same correlation. Therefore, we consider in the overlapped AF scheme
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_Equ20_HTML.gif
(20)
as noise vectors with covariance matrices
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_Equ21_HTML.gif
(21)
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_Equ22_HTML.gif
(22)
Above, https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq168_HTML.gif denotes the conjugate transpose of the vector https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq169_HTML.gif . Note that the expressions for the nonoverlapped AF scheme can be obtained as a special case of (20)–(22) by setting https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq170_HTML.gif .
An achievable rate expression https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq171_HTML.gif is obtained by solving the following optimization problem which requires finding the worst-case noise:
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_Equ23_HTML.gif
(23)
The following results provide a general formula for https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq172_HTML.gif , which applies to both nonoverlapped and overlapped transmission scenarios.
Theorem 1.
An achievable rate for AF transmission scheme is given by
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_Equ24_HTML.gif
(24)
where https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq173_HTML.gif and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq174_HTML.gif are defined as https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq175_HTML.gif and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq176_HTML.gif . Furthermore,
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_Equ25_HTML.gif
(25)
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_Equ26_HTML.gif
(26)
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_Equ27_HTML.gif
(27)
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_Equ28_HTML.gif
(28)
where https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq177_HTML.gif denotes https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq178_HTML.gif . In the above equations and henceforth, https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq179_HTML.gif , https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq180_HTML.gif , and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq181_HTML.gif denote independent, standard Gaussian random variables. The above formulation applies to both overlapped and nonoverlapped cases. Recalling (9), if one assumes in (24)–(28) that
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_Equ29_HTML.gif
(29)
one obtains the achievable rate expression for the nonoverlapped AF scheme. Note that if https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq182_HTML.gif , the function https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq183_HTML.gif in (24). For overlapped AF, one has
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_Equ30_HTML.gif
(30)
Moreover, one knows from (10) that
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_Equ31_HTML.gif
(31)
Proof.
See Appendix .
Next, we consider DF relaying scheme. In DF, there are two different coding approaches [7], namely, repetition coding and parallel channel coding. We first consider repetition channel coding scheme. The following result provides achievable rate expressions for both nonoverlapped and overlapped transmission scenarios.
Theorem 2.
An achievable rate expression for DF with repetition channel coding transmission scheme is given by
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_Equ32_HTML.gif
(32)
where
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_Equ33_HTML.gif
(33)
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_Equ34_HTML.gif
(34)
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq184_HTML.gif , https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq185_HTML.gif , https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq186_HTML.gif https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq187_HTML.gif , https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq188_HTML.gif have the same expressions as in (25)–(28). https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq189_HTML.gif and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq190_HTML.gif are given in (29)–(31).
Proof.
See Appendix .
Finally, we consider DF with parallel channel coding and assume that nonoverlapped transmission scheme is adopted. From [13, Equation ( 6)], we note that an achievable rate expression is given by
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_Equ35_HTML.gif
(35)
Note that we do not have separate direct transmission in this relaying scheme. Using similar methods as in the proofs of Theorems 1 and 2, we obtain the following result. The proof is omitted to avoid repetition.
Theorem 3.
An achievable rate of nonoverlapped DF with parallel channel coding scheme is given by
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_Equ36_HTML.gif
(36)
where https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq191_HTML.gif , https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq192_HTML.gif and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq193_HTML.gif are given in (25)–(27) with https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq194_HTML.gif and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq195_HTML.gif defined in (29) and (31).

5. Resource Allocation Strategies

Having obtained achievable rate expressions in Section 4, we now identify resource allocation strategies that maximize these rates. We consider three resource allocation problems: https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq196_HTML.gif power allocation between training and data symbols, https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq197_HTML.gif time/bandwidth allocation to the relay, and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq198_HTML.gif power allocation between the source and relay under a total power constraint.
We first study how much power should be allocated for channel training. In nonoverlapped AF, it can be seen that https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq199_HTML.gif appears only in https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq200_HTML.gif in the achievable rate expression (24). Since https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq201_HTML.gif is a monotonically increasing function of https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq202_HTML.gif for fixed https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq203_HTML.gif , (24) is maximized by maximizing https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq204_HTML.gif . We can maximize https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq205_HTML.gif by maximizing the coefficient of the random variable https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq206_HTML.gif in (27), and the optimal https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq207_HTML.gif is given as follows:
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_Equ37_HTML.gif
(37)
where https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq208_HTML.gif denotes https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq209_HTML.gif Optimizing https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq210_HTML.gif in nonoverlapped AF is more complicated as it is related to all the terms in (24), and hence obtaining an analytical solution is unlikely. A suboptimal solution is to maximize https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq211_HTML.gif and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq212_HTML.gif separately and obtain two solutions https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq213_HTML.gif and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq214_HTML.gif , respectively. Note that expressions for https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq215_HTML.gif and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq216_HTML.gif are exactly the same as that in (37) with https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq217_HTML.gif and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq218_HTML.gif replaced by https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq219_HTML.gif and ( https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq220_HTML.gif ), and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq221_HTML.gif replaced by https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq222_HTML.gif in https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq223_HTML.gif and replaced by https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq224_HTML.gif in https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq225_HTML.gif . When the source-relay channel is better than the source-destination channel and the fraction of time over which direct transmission is performed is small, https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq226_HTML.gif is a more dominant factor and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq227_HTML.gif is a good choice for training power allocation. Otherwise, https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq228_HTML.gif might be preferred. Note that in nonoverlapped DF with repetition and parallel coding, https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq229_HTML.gif is the only term that includes https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq230_HTML.gif . Therefore, similar results and discussions apply. For instance, the optimal https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq231_HTML.gif has the same expression as that in (37). Figure 4 plots the optimal https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq232_HTML.gif as a function of https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq233_HTML.gif for different relay power constraints https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq234_HTML.gif when https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq235_HTML.gif and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq236_HTML.gif . It is observed in all cases that the allocated training power monotonically decreases with improving channel quality and converges to https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq237_HTML.gif which is independent of https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq238_HTML.gif .
In overlapped transmission schemes, both https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq246_HTML.gif and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq247_HTML.gif appear in more than one term in the achievable rate expressions. Therefore, we resort to numerical results to identify the optimal values. Figures 5 and 6 plot the achievable rates as a function of https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq248_HTML.gif and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq249_HTML.gif for overlapped AF. In both figures, we have assumed that https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq250_HTML.gif https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq251_HTML.gif  and   https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq252_HTML.gif . While Figure 5 considers high SNRs ( https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq253_HTML.gif and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq254_HTML.gif ), we assume that https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq255_HTML.gif and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq256_HTML.gif in Figure 6. In Figure 5, we observe that increasing https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq257_HTML.gif will increase achievable rate until https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq258_HTML.gif . Further increase in https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq259_HTML.gif decreases the achievable rates. On the other hand, rates always increase with increasing https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq260_HTML.gif , leaving less and less power for data transmission by the relay. This indicates that cooperation is not beneficial in terms of achievable rates and direct transmission should be preferred. On the other hand, in the low-power regime considered in Figure 6, the optimal values of https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq261_HTML.gif and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq262_HTML.gif are approximately 0.18 and 0.32, respectively. Hence, the relay in this case helps to improve the rates.
Next, we analyze the effect of the degree of cooperation on the performance in AF and repetition DF. Figures 7 and 8 plot the achievable rates as a function of https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq266_HTML.gif which gives the fraction of total time/bandwidth allocated to the relay. Achievable rates are obtained for different channel qualities given by the standard deviations https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq267_HTML.gif and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq268_HTML.gif of the fading coefficients. We observe that if the input power is high, https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq269_HTML.gif should be either https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq270_HTML.gif or close to zero depending on the channel qualities. On the other hand, https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq271_HTML.gif always gives us the best performance at low SNR levels regardless of the channel qualities. Hence, while cooperation is beneficial in the low-SNR regime, noncooperative transmissions might be optimal at high SNRs. We note from Figure 7 in which https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq272_HTML.gif that cooperation starts being useful as the source-relay channel variance https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq273_HTML.gif increases. Similar results are also observed if overlapped DF with repetition coding is considered. Hence, the source-relay channel quality is one of the key factors in determining the usefulness of cooperation in the high SNR regime. At the same time, additional numerical analysis has indicated that if SNR is further increased, noncooperative direct transmission tends to outperform cooperative schemes even in the case in which https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq274_HTML.gif . Hence, there is a certain relation between the SNR level and the required source-relay channel quality for cooperation to be beneficial. The above conclusions apply to overlapped AF and DF with repetition coding. In contrast, numerical analysis of nonoverlapped DF with parallel coding in the high-SNR regime has shown that cooperative transmission with this technique provides improvements over noncooperative direct transmission. A similar result will be discussed later in this section when the performance is analyzed under total power constraints.
In Figure 8 in which SNR is low ( https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq283_HTML.gif ), we see that the highest achievable rates are attained when there is full cooperation (i.e., when https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq284_HTML.gif ). Note that in this figure, overlapped DF with repetition coding is considered. If overlapped AF is employed as the cooperation strategy, we have similar conclusions but it should also be noted that overlapped AF achieves smaller rates than those attained by overlapped DF with repetition coding.
In Figure 9, we plot the achievable rates of DF with parallel channel coding, derived in Theorem 3, when https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq285_HTML.gif . We can see from the figure that the highest rate is obtained when both the source-relay and relay-destination channel qualities are higher than of the source-destination channel (i.e., when https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq286_HTML.gif and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq287_HTML.gif ). Additionally, we observe that as the source-relay channel improves, more resources need to be allocated to the relay to achieve the maximum rate. We note that significant improvements with respect to direct transmission (i.e., the case when https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq288_HTML.gif ) are obtained. Finally, we can see that when compared to AF and DF with repetition coding, DF with parallel channel coding achieves higher rates. On the other hand, AF and repetition coding DF have advantages in the implementation. Obviously, the relay, which amplifies and forwards, has a simpler task than that which decodes and forwards. Moreover, as pointed out in [18], if AF or repetition coding DF is employed in the system, the architecture of the destination node is simplified because the data arriving from the source and relay can be combined rather than stored separately.
In certain cases, source and relay are subject to a total power constraint. Here, we introduce the power allocation coefficient https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq292_HTML.gif and total power constraint https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq293_HTML.gif . https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq294_HTML.gif and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq295_HTML.gif have the following relations: https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq296_HTML.gif , https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq297_HTML.gif , and hence https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq298_HTML.gif . Next, we investigate how different values of https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq299_HTML.gif , and hence different power allocation strategies, affect the achievable rates. Analytical results for https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq300_HTML.gif that maximizes the achievable rates are difficult to obtain. Therefore, we again resort to numerical analysis. In all numerical results, we assume that https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq301_HTML.gif which provides the maximum of degree of cooperation. First, we consider the AF. The fixed parameters we choose are https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq302_HTML.gif  and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq303_HTML.gif . Figure 10 plots the achievable rates in the overlapped AF transmission scenario as a function of https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq304_HTML.gif for different channel conditions, that is, different values of https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq305_HTML.gif and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq306_HTML.gif . We observe that the best performance is achieved as https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq307_HTML.gif . Hence, even in the overlapped scenario, all the power should be allocated to the source and direct transmission should be preferred at these high SNR levels. Note that if direct transmission is performed, there is no need to learn the relay-destination channel. Since the time allocated to the training for this channel should be allocated to data transmission, the real rate of direct transmission is slightly higher than the point that the cooperative rates converge as https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq308_HTML.gif . For this reason, we also provide the direct transmission rate separately in Figure 10. Further numerical analysis has indicated that direct transmission outperforms nonoverlapped AF, overlapped and nonoverlapped DF with repetition coding as well at this level of input power. On the other hand, in Figure 11 which plots the achievable rates of nonoverlapped DF with parallel coding as a function of https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq309_HTML.gif , we observe that direct transmission rate, which is the same as that given in Figure 10, is exceeded if https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq310_HTML.gif and hence the source-relay channel is very strong. The best performance is achieved when https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq311_HTML.gif and therefore https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq312_HTML.gif of the power is allocated to the source.
Figures 12 and 13 plot the nonoverlapped achievable rates when https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq319_HTML.gif . In all cases, we observe that performance levels higher than those of direct transmission are achieved unless the qualities of the source-relay and relay-destination channels are comparable to those of the source-destination channel (e.g., https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq320_HTML.gif ). Moreover, we note that the best performances are attained when the source-relay and relay-destination channels are both considerably better than the source-destination channel (i.e., when https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq321_HTML.gif ). As expected, highest gains are obtained with parallel coding DF although further numerical analysis has shown that repetition coding incurs only small losses. Finally, Figure 14 plots the achievable rates of overlapped AF when https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq322_HTML.gif . Similar conclusions apply also here. However, it is interesting to note that overlapped AF rates are smaller than those achieved by nonoverlapped AF. This behavior is also observed when DF with repetition coding is considered. Note that in nonoverlapped transmission, source transmits in a shorter duration of time with higher power. This signaling scheme provides better performance as expected because it is well known that flash signaling achieves the capacity in the low-SNR regime in imperfectly known channels [27].
Table 2 summarizes the conclusions drawn and insights gained in this section on the performance of different cooperation strategies and resource allocation schemes in the high- and low-SNR regimes.
Table 2
Table 2
High-SNR Regime
(i) Cooperation employing overlapped AF or DF with repetition coding is beneficial only if the source-relay channel quality is high enough. If this is not the case or SNR is very high, noncooperative direct transmission should be employed.
 
(ii) Cooperation using nonoverlapped DF with parallel coding provides improvements over the performance of noncooperative direct transmission and achieves higher rates than those attained by overlapped AF and DF with repetition coding.
 
(iii) If the system is operating under total power constraints, all the power should be allocated to the source and hence direct transmission should be preferred over overlapped and nonoverlapped AF and overlapped and nonoverlapped DF with repetition coding.
 
(iv) Under total power constraints, only nonoverlapped DF with parallel coding outperforms noncooperative direct transmission when the source-relay channel is strong.
Low-SNR Regime
(i) Cooperation is generally beneficial.
 
(ii) The strengths of both the source-relay and relay-destination channels are important factors.
 
(iii) Nonoverlapped DF with parallel coding achieves the highest performance levels. In general, nonoverlapped transmission methods should be preferred. Also, DF provides higher gains over AF.
 
(iv) Under total power constraints, highest gains over noncooperative direct transmission are attained when both the source-relay and relay-destination channels are considerably stronger than the source-destination channel.
 
(v) Under total power constraints, noncooperative direct transmission should be preferred if the qualities of both the source-relay and relay-destination channels are comparable to that of the source-destination channel.

6. Energy Efficiency

Our analysis has shown that cooperative relaying is generally beneficial in the low-power regime, resulting in higher achievable rates when compared to direct transmission. In this section, we provide an energy efficiency perspective and remark that care should be exercised when operating at very low SNR values. The least amount of energy required to send one information bit reliably is given by https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq332_HTML.gif where https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq333_HTML.gif is the channel capacity in bits/symbol. (Note that https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq334_HTML.gif is the bit energy normalized by the noise power spectral level https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq335_HTML.gif .)In our setting, the capacity will be replaced by the achievable rate expressions and hence the resulting bit energy, denoted by https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq336_HTML.gif , provides the least amount of normalized bit energy values in the worst-case scenario and also serves as an upper bound on the achievable bit energy levels in the channel.
We note that in finding the bit energy values, we assume that https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq337_HTML.gif where https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq338_HTML.gif is the total power. The next result provides the asymptotic behavior of the bit energy as https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq339_HTML.gif decreases to zero.
Theorem 4.
The normalized bit energy in all relaying schemes grows without bound as the signal-to-noise ratio decreases to zero, that is,
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_Equ38_HTML.gif
(38)
Proof.
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq340_HTML.gif is the derivative of https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq341_HTML.gif with respect to SNR as SNR https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq342_HTML.gif 0. The key point to prove this theorem is to show that when https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq343_HTML.gif , the mutual information decreases as https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq344_HTML.gif , and hence https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq345_HTML.gif . This can be easily shown because when https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq346_HTML.gif , in all the terms, https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq347_HTML.gif , https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq348_HTML.gif , https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq349_HTML.gif , https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq350_HTML.gif , and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq351_HTML.gif in Theorems 1–3, the denominator goes to a constant while the numerator decreases as https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq352_HTML.gif . Hence, these terms diminish as https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq353_HTML.gif . Since https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq354_HTML.gif for small https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq355_HTML.gif , where https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq356_HTML.gif satisfies https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq357_HTML.gif , we conclude that the achievable rate expressions also decrease as https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq358_HTML.gif as https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq359_HTML.gif vanishes.
Theorem 4 indicates that it is extremely energy-inefficient to operate at very low https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq360_HTML.gif values. We identify the most energy-efficient operating points in numerical results. We choose the following numerical values for the fixed parameters: https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq361_HTML.gif , https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq362_HTML.gif , https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq363_HTML.gif , https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq364_HTML.gif , https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq365_HTML.gif , and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq366_HTML.gif . Figure 15 plots the bit energy curves as a function of SNR for different values of https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq367_HTML.gif in the nonoverlapped AF case. We can see from the figure that the minimum bit energy, which is achieved at a nonzero value of SNR, decreases with increasing https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq368_HTML.gif and is achieved at a lower https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq369_HTML.gif value. Figure 16 shows the minimum bit energy for different relaying schemes with overlapped or nonoverlapped transmission techniques. We observe that the minimum bit energy decreases with increasing https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq370_HTML.gif in all cases. We realize that DF is in general much more energy-efficient than AF. Moreover, we note that employing nonoverlapped rather than overlapped transmission improves the energy efficiency. We further remark that the performances of nonoverlapped DF with repetition coding and parallel coding are very close.

7. Conclusion

In this paper, we have studied the imperfectly-known fading relay channels. We have assumed that the source-destination, source-relay, and relay-destination channels are not known by the corresponding receivers a priori, and transmission starts with the training phase in which the channel fading coefficients are learned with the assistance of pilot symbols, albeit imperfectly. Hence, in this setting, relaying increases the channel uncertainty in the system, and there is increased estimation cost associated with cooperation. We have investigated the performance of relaying by obtaining achievable rates for AF and DF relaying schemes. We have considered both nonoverlapped and overlapped transmission scenarios. We have controlled the degree of cooperation by varying the parameter https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq375_HTML.gif . We have identified resource allocation strategies that maximize the achievable rate expressions. We have observed that if the source-relay channel quality is low, then cooperation is not beneficial and direct transmission should be preferred at high SNRs when amplify-and-forward or decode-and-forward with repetition coding is employed as the cooperation strategy. On the other hand, we have seen that relaying generally improves the performance at low SNRs. We have noted that DF with parallel coding provides the highest rates. Additionally, under total power constraints, we have studied power allocation between the source and relay. We have again pointed out that relaying degrades the performance at high SNRs unless DF with parallel channel coding is used and the source-relay channel quality is high. The benefits of relaying is again demonstrated at low SNRs. We have noted that nonoverlapped transmission is superior compared to overlapped one in this regime. Finally, we have considered the energy efficiency in the low-power regime and proved that the bit energy increases without bound as SNR diminishes. Hence, operation at very low SNR levels should be avoided. From the energy efficiency perspective, we have again observed that nonoverlapped transmission provides better performance. We have also noted that DF is more energy efficient than AF.

Acknowledgments

This work was supported in part by the NSF CAREER Grant CCF-0546384. The material in this paper was presented in part at the 45th Annual Allerton Conference on Communication, Control and Computing in September 2007 and in part at the 9th IEEE Workshop on Signal Processing Advances for Wireless Communications (SPAWC) in July 2008.
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.
Appendix

Appendices

A. Proof of Theorem 1

Note that in AF relaying,
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_Equ39_HTML.gif
(A1)
where the first mutual expression on the right-hand side of (A.1) is for the direct transmission and the second is for the cooperative transmission. In the direct transmission, we have
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_Equ40_HTML.gif
(A2)
In this setting, it is well known that the worst-case noise https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq376_HTML.gif is Gaussian [25, Appendix] and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq377_HTML.gif with independent Gaussian components achieves
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_Equ41_HTML.gif
(A3)
We now investigate the cooperative phase. Comparing (14) and (15) with (17) and (18), we see that nonoverlapped can be obtained as a special case of overlapped AF scheme by letting https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq378_HTML.gif . Therefore, we concentrate on the more general case of overlapped transmission. For better illustration, we rewrite the symbol-wise channel input-output relationships in the following:
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_Equ42_HTML.gif
(A4)
for https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq379_HTML.gif , and
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_Equ43_HTML.gif
(A5)
for https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq380_HTML.gif . In AF, the signals received and transmitted by the relay have the following relation:
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_Equ44_HTML.gif
(A6)
Now, we can write the channel in the vector form
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_Equ45_HTML.gif
(A7)
where https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq381_HTML.gif and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq382_HTML.gif Note that we have defined https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq383_HTML.gif , and the expression in (A.7) uses the property that https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq384_HTML.gif and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq385_HTML.gif for https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq386_HTML.gif . The input-output mutual information in the cooperative phase can now be expressed as
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_Equ46_HTML.gif
(A8)
where in (A.8) we removed the dependence on https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq387_HTML.gif without loss of generality. Note that https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq388_HTML.gif and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq389_HTML.gif are defined in (A.7). Now, we can calculate the worst-case capacity by proving that Gaussian distribution for https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq390_HTML.gif , https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq391_HTML.gif , and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq392_HTML.gif provides the worst case. We employ techniques similar to that in [25, Appendix]. Any set of particular distributions for https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq393_HTML.gif , https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq394_HTML.gif , and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq395_HTML.gif yields an upper bound on the worst case. Let us choose https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq396_HTML.gif , https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq397_HTML.gif , and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq398_HTML.gif to be zero mean complex Gaussian distributed. Then as in [6, Appendix II],
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_Equ47_HTML.gif
(A9)
where the expectation is with respect to the fading estimates. To obtain a lower bound, we compute the mutual information for the channel in (A.7) assuming that https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq399_HTML.gif is a zero-mean complex Gaussian with variance https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq400_HTML.gif , but the distributions of noise components https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq401_HTML.gif , https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq402_HTML.gif , and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq403_HTML.gif are arbitrary. In this case, we have
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_Equ48_HTML.gif
(A10)
where the inequality is due to the fact that Gaussian distribution provides the largest entropy and hence [28, Chapter 9]
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_Equ49_HTML.gif
(A11)
Above, https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq404_HTML.gif denotes the differential entropy functional. From [25, Lemma 1, Appendix], we know that
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_Equ50_HTML.gif
(A12)
for ant estimate https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq405_HTML.gif given https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq406_HTML.gif . If we substitute the linear minimum mean-square-error (LMMSE) estimate https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq407_HTML.gif , where https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq408_HTML.gif and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq409_HTML.gif are cross-covariance and covariance matrices respectively, into (A.10) and (A.12), we obtain
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_Equ51_HTML.gif
(A13)
(Here, we use the property that https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq410_HTML.gif .)Since the lower bound (A.13) applies for any noise distribution, we can easily see that
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_Equ52_HTML.gif
(A14)
From (A.9) and (A.14), we conclude that
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_Equ53_HTML.gif
(A15)
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_Equ54_HTML.gif
(A16)
In obtaining (A.16), we have used the fact that https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq411_HTML.gif . Note also that in (A.16), https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq412_HTML.gif and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq413_HTML.gif are the powers of source and relay symbols and are given in (29)–(31). Moreover, https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq414_HTML.gif and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq415_HTML.gif are the variances of the noise components defined in (20). Now, combining (23), (A.1), (A.3), and (A.16), we obtain the achievable rate expression in (24). Note that (25)–(28) are obtained by using the expressions for the channel estimates in (5)–(7) and noise variances in (21) and (22).

B. Proof of Theorem 2

For DF with repetition coding in overlapped transmission, an achievable rate expression is
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_Equ55_HTML.gif
(B1)
Note that the first and second mutual information expressions in (B.1) are for the direct transmission between the source and destination, and direct transmission between the source and relay, respectively. Therefore, as in the proof of Theorem 1, the worst-case achievable rates can be immediately seen to be equal to the first term on the right-hand side of (32) and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq416_HTML.gif , respectively.
In repetition coding, after successfully decoding the source information, the relay transmits the same codeword as the source. As a result, the input-output relation in the cooperative phase can be expressed as
https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_Equ56_HTML.gif
(B2)
where https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq417_HTML.gif From (B.2), it is clear that the knowledge of https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq418_HTML.gif is not required at the destination. We can easily see that (B.2) is a simpler expression than (A.7) in the AF case; therefore we can adopt the same methods as employed in the proof of Theorem 1 to show that Gaussian noise is the worst noise and https://static-content.springer.com/image/art%3A10.1155%2F2009%2F458236/MediaObjects/13638_2009_Article_1666_IEq419_HTML.gif is the worst-case rate.
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Metadata
Title
Achievable Rates and Resource Allocation Strategies for Imperfectly Known Fading Relay Channels
Authors
Junwei Zhang
Mustafa Cenk Gursoy
Publication date
01-12-2009
Publisher
Springer International Publishing
DOI
https://doi.org/10.1155/2009/458236

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