The development of the modern Internet-based data communication systems and ever increasing demand for bandwidth have spurred an unprecedented progress in development of high capacity wireless systems. The major trends in such systems design are the use of multiple antennas to provide capacity gains on fading channels and orthogonal frequency division multiplexing (OFDM) to facilitate the utilization of these capacity gains on rich scattering frequency-selective channels. Since the end of the last decade, there has been an explosion of interest in multiple-input multiple-output systems (MIMO) and a lot of research work has been devoted to their performance limits and methods to achieve them.
One of the fundamental issued in multiple antenna systems is the availability of the channel state information at transmitter and receiver. While it is usually assumed that the perfect channel state information (CSI) is available at the receiver, the transmitter may have perfect, partial or no CSI. In case of the single user systems, the perfect CSI at the transmitter (CSIT) allows for use of a spatial water-filling approach to achieve maximum capacity. In case of multi-user broadcast channels (the downlink), the capacity is maximized by using the so called dirty paper coding, which also depends on the availability of perfect CSIT. Such systems are usually refereed to as closed-loop as opposed to open-loop systems where there is no feedback from the receiver and the transmitter typically uses equal-power division between the antennas.
In practice, the CSI should be quantized to minimize feedback rate while providing satisfactory performance of the system. The problem has attracted attention of
community and papers provided solutions for beam-forming on flat-fading MIMO channels where the diversity gain is the main focus. Moreover, some authors dealt with frequency-selective channels and OFDM modulation although also those papers were mainly devoted to beamforming approach.
Unfortunately, availability of full CSIT is unrealistic due to the feedback delay and noise, channel estimation errors and limited feedback bandwidth, which forces CSI to be quantized at the receiver to minimize feedback rate. The problem has attracted attention of the scientific community and papers have provided solutions for single-user beamforming on flat-fading MIMO channels, where the diversity gain is the main focus. More recently, CSI quantization results were shown for multi-user zero-forcing algorithms by Jindal.
This summary is provided to introduce a selection of concepts in a simplified form that are further described below in the Detailed Description. This summary is not intended to identify key features of the claimed subject matter, nor is it intended to be used as an aid in determining the scope of the claimed subject matter.
We present a simple, flexible algorithm that is constructed with multiplexing approach to MIMO transmission, i.e., where the channel is used to transmit multiple data streams. We use a vector quantizer approach to construct code-books of water-filling covariance matrices which can be used in a wide variety of system configurations and on frequency selective channels. Moreover, we propose a solution which reduces the required average feedback rate by transmitting the indexes of only those covariance matrices which provide higher instantaneous capacity than the equal power allocation.
The foregoing aspects and many of the attendant advantages of this invention will become more readily appreciated as the same become better understood by reference to the following detailed description, when taken in conjunction with the accompanying drawings, wherein:
Embodiments will now be described with reference to the figures, in which like reference characters denote like elements, by way of example, and in which:
One of the fundamental issues in multiple antenna systems is the availability of the channel state information (CSI) at transmitter and receiver[24]. The perfect CSI at the transmitter (CSIT) enables the use of a spatial water-filling, dirty paper coding and simultaneous transmission to multiple users, allowing the systems to approach their maximum theoretical capacity. Such systems are usually referred to as closed-loop as opposed to open-loop systems where them is no feedback from the receiver. Closed-loop systems enable major increases of system capacities, allowing the operators to multiply their revenue and maintain high quality of service at the same time.
In this work, we describe a flexible approach to CSI encoding, which can be used to construct the linear modulation matrices for both single-user and multi-user networks. In both cases, the modulation matrices are composed of two independent parts: the eigenmode matrix and the diagonal power division matrix with the sum of entries on the diagonal equal to 1. The system operates as follows:
1. The receiver(s)[24] estimate(s) the respective multiple antenna channel(s).
2. Each estimated channel is decomposed using the singular value decomposition (SVD) to form the matrix of eigenmodes[30] and their respective singular values[304].
3. If the system works in the single-user mode, all entries in the codebook of transmitter eigenmode modulation matrices[32] and all entries in the codebook of transmitter power division matrices[32A] are tested at the receiver to choose their combination providing highest instantaneous capacity. The indices of the best transmitter eigenmode and power division matrices are then sent[34],[34A] back to the transmitter.
4. If the system works in the multi-user mode, all entries in the codebook of receiver eigenmode vectors[32] and all entries in the codebook of receiver mode gains[32A] are tested at the receiver[24] for best match with the estimated channel (the matching function can be chosen freely by the system designer). The indices of the best receiver eigemnode and power division matrices[94] are then sent[34] back to the transmitter.
5. Based on the received[36],[36A] indices, the transmitter chooses[38],[52],[62] the modulation matrix and uses it to transmit[40] the information to one or more users[24] at a time.
Our proposed method allows to simplify the feedback system by implementing only one set of eigenmode matrices for all values of signal-to-noise ratio (SNR) and a much smaller set of power division matrices that differ slightly for different values of SNR. As a result, the required feedback bit rate is kept low and constant throughout the whole range of SNR values of interest. The additional advantage of the splitting of the modulation matrix into two parts is that it can lower the feedback hit rate for slowly-varying channels. If the eigeninodes of the channel stay within the same region for an extended period of time, additionally, nested encoding can be performed to increase the resolution of the CSIT and improve the system capacity.
The actual design of the receiver and transmitter eigenmode and power division matrices can be done using numerical or analytical methods and is not the object of this disclosure. However, our method allows for actual implementations of systems closely approaching the theoretical capacities of MIMO channels without putting any unrealistic demand on the feedback link throughput. This is a major improvement compared to the other state-of-the art CSI quantization methods, which experience problems approaching the theoretical capacities and suffer from the early onset of capacity ceiling due to inter-user interference at relatively low SNR.
We assume that the communication system consists of a transmitter equipped with nT antennas[22] and a receiver[24] with nR antennas[26]. A general frequency selective fading channel is modeled by a set of channel matrices Hj of dimension nR×nT defined for each sub-carrier j=0,1, . . . NOFDM−1. The received signal at the jth sub-carrier is then given by the nR-dimensional vector yj defined as
y
j
=H
j
x
j
+n
j (1)
where xj is the nTdimensional vector of the transmitted signal and nj is the nR-dimensional vector consisting of independent circular complex Gaussian entries with zero mean and variance 1. Moreover, we assume that power is allocated equally across all sub-carriers |xj|2=P.
If the transmitter has access to the perfect channel state information about the matrix Hj, it can select the signaling vector xj to maximize the closed-loop system capacity
where Qj=E[xjxjH]. Unfortunately, optimizing the capacity in (2) requires a very large feedback rate to transmit information about optimum Qj (or correspondingly Hj) which is impractical. Instead, we propose using a limited feedback link, with the transmitter choosing from a set of matrices {circumflex over (Q)}(n).
Using the typical approach involving singular value decomposition and optimum water-filling, we can rewrite (1) as
y
j
=H
j
x
j
+n
j=(UjDjVjH)(Vj{tilde over (x)}j)+nj (3)
where E[{tilde over (x)}j{tilde over (x)}jH]=Sj constrained with Tr (Sj)=P is a diagonal matrix describing optimum power allocation between the eigenmodes in Vj. Based on (3), the set of matrices Qj=VjSjVjH, maximizes capacity in (2).
To construct the most efficient vector quantizer for channel feedback, the straightforward approach would be to jointly optimize signal covariance matrices {circumflex over (Q)} for all sub-carriers at once. Such an approach, however, is both complex and impractical, since any change of channel description and/or power level would render the optimized quantizer suboptimal. Instead, we propose an algorithm which separately quantizes information about eigenmode matrices Vj in codebook {circumflex over (V)} and power allocation Sj in codebook Ŝ. Note that the first variable depends only on channel description and not on the power level P which simplifies the design.
We optimize the quantizers {circumflex over (V)} and Ŝ for flat-fading case and we apply them separately for each sub-carrier in case of OFDM modulation. Although such an approach is sub-optimal, it allows a large degree of flexibility since different system setups can be supported with the same basic structure.
We assume that the receiver[24] has perfect channel state information (CSIR) and attempts to separate[30] the eigenmode streams {tilde over (x)}j in (3) by multiplying yj with UjH. However, if the transmitter uses quantized eigenmode matrix set with limited cardinality, the diagonalization of {tilde over (x)}j will not be perfect. To model this, we introduce a heuristic distortion metric which is expressed as
γv(n;H)=∥DVH{circumflex over (V)}(n)−D∥F (4)
where {circumflex over (V)}(n) is the nth entry in the predefined set of channel diagonalization matrices and ∥⋅∥F is the Frobenius norm. We omitted subscript entries j in (4) for the clarity of presentation.
We assume that n=0,1, . . . 2N
V
i
={H:γv(i;H)<γv(j;H) for all j≠i}. (5)
It can be shown that minimizing this metric should, on average, lead to maximizing the ergodic capacity of the channel with the quantized feedback (when γ(n;H)=0 the channel becomes perfectly diagonalized). The optimum selection of {circumflex over (V)} and regions Vi in (5) is an object of our current work. Here, however, we use a simple iterative heuristic based on a modified form of the Lloyd algorithm, which has very good convergence properties and usually yields good results. The algorithm starts by creating a codebook of centroids {circumflex over (V)} and, based on these results, divides the quantization space into regions Vi. The codebook is created as follows:[50]
1. Create a large training set of L random matrices H(l).[46]
2. For each random matrix H(l), perform singular value decomposition to obtain D(l) and V(l) as in (3).
3. Set iteration counter i=0. Create a set of 2N
4. For each matrix Ĥ(n) calculate corresponding {circumflex over (V)}(i)(n) using singular value decomposition.
5. For each training element H(l) and codebook entry {circumflex over (V)}(i)(n) calculate the metric in (4). For every l choose indexes nopt(l) corresponding to the lowest values of γv(n;H(l)).
6. Calculate a new set {circumflex over (V)}(i+1)(n) as a form of spherical average of all entries V(l) corresponding to the same index n using the following method. (The direct averaging is impossible since it does not preserve orthogonality between eigenvectors.) For all n calculate the subsets L(n)={l:nopt(l)=n} and if their respective cardinalities |L(n)|≠0 the corresponding matrices
where 1O is an nT×nT all-zero matrix with the exception of the upper-left corner element equal to 1. Finally, using singular value decomposition, calculate {circumflex over (V)}(i+1)(n) from
(i+1)(n)={circumflex over (V)}(i+1)(n)W({circumflex over (V)}(l+1)(n))H (7)
where W is a dummy variable.
7. Calculate the average distortion metric
v
(i+1=1/LΣlγv(nopt(i);H(l)).
8. If distortion metric fulfills |
Upon completion of the above algorithm, the set of vectors {circumflex over (V)} can be used to calculate the regions in (5). The results of the codebook optimization are presented in
Having optimized[50] power-independent entries in the codebook of channel eigenmode matrices {circumflex over (V)}, the next step is to create a codebook for power allocation Ŝ[118]. We use a distortion metric defined as
where Ŝ(k) is the kth entry in the predefined set of channel water-filling matrices and {circumflex over (V)}(nopt)V is the entry in the {circumflex over (V)} codebook that minimizes metric (4) for the given H. We use k=0,1, . . . 2N
Similarly to the previous problem, we divide the whole space of channel realizations H into 2N
S
i(P)={H:γs(i;H;P)<γs(j;H;P) for all j≠i}. (9)
and to create the codebook Ŝ, we use the following method:
1. Create a large training set of L random matrices H(l).
2. For each random matrix H(l), perform water-filling operation to obtain optimum covariance matrices Q(l) and S(l).
3. Set iteration counter i=0. Create[100],[104] a set of 2N
4. For every codebook entry Ŝ(i)(k) and matrix Q(l) calculate[112] the metric as in (8). Choose[106] indexes kopt(l) corresponding to the lowest values of γS(k;H(l);P).
5. If γS(kopt(l);H(l);P)>γeq(H(l);P) where γeq(H(l);P) is the metric corresponding to equal-power distribution defined as
set the corresponding entry kopt(l)=2N
6. For all k=0,1, . . . 2N
7. Calculate the average distortion metric
8. If distortion metric fulfills |
The set of vectors Ŝ is then used to calculate the regions in (9). Since waterfilling strongly depends on the power level P and {circumflex over (V)}, optimally the Ŝ should be created for every power level and number of bits NV in eigenvector matrix codebook. As an example, the results of the above optimization are presented in
An interesting property of the above algorithm is that it automatically adjusts the number of entries in Ŝ according to the number of entries in {circumflex over (V)}. For low values of NV, even if the algorithm for selection of Ŝ is started with high NS, the optimization process will reduce the search space by reducing cardinality |L(k)| of certain entries to 0. As a result, for NV=2,3, NS=1 will suffice, while for NV=4, the algorithm will usually converge to NS=2. This behavior can be easily explained since for low resolution of the channel eigenvector matrices {circumflex over (V)} only low precision is necessary for describing Ŝ. Only with increasing NV, the precision NS becomes useful.
The vector quantizers from the previous sections are first applied to a flat-fading channel case. In such a case, the elements or each matrix H in (1) are independent circular complex Gaussian elements, normalized to unit variance.
The system operation can now be described as follows:
1. The receiver[24] estimates the channel matrix H.
2. The receiver[24] localizes the region Vi according to (5) and stores its index as nopt.[32]
3. Using nopt, the receiver[24] places H in a region Si according to (9) and stores its index as kopt.
4. If the resulting system capacity using the predefined codebook entries is higher than the capacity of equal power distribution as in
C(nopt,kopt)>log2 det[I+P/nTHHH] (13)
indexes nopt and kopt are fed back to the transmitter.[34],[36]
5. The transmitter uses[40],[38A] the received indices of a codebook entries to process its signal. If there is no feedback, power is distributed equally between the antennas[22].
Using the above algorithm, the system's performance is lower-bounded by the performance of the corresponding open-loop system and improves if the receiver [24] finds a good match between the channel realization and the existing codebook entries. The salient advantage of such an approach is its flexibility and robustness to the changes of channel model. If there are no good matches in the codebook, the feedback link is not wasted and the transmitter uses the equal power distribution. The disadvantage of the system is that the feedback link is characterized by a variable bit rate.
In case of the frequency-selective channel, flat fading algorithm is applied to the separate OFDM sub-carriers. Although this approach is clearly sub-optimal, it allows us to use a generic vector quantizer trained to the typical flat-fading channel in a variety of other channels.
In general case, the feedback rate for such an approach would be upper-bounded by NOFDM(NV+ND). However, as pointed out by Kim et al., the correlation between the adjacent sub-carriers in OFDM systems can be exploited to reduce the required feedback bit rate by proper interpolating between the corresponding optimum signalling vectors. In this work, we use a simpler method which allows the receiver[24] to simply group adjacent M sub-carriers and perform joint optimization using the same codebook entry for all of them (such methods are sometimes called clustering).
We tested the system on 2×2 MIMO and 4×4 MIMO channels with varying SNR and feedback rates. We tested 2×2 MIMO channel with NV=2,3,4 and ND=1, corresponding to total feedback rate of between 3 and 5 bits. Correspondingly, in case of 4×4 MIMO, we used NV=10,12,14 and ND=2, corresponding to total feedback rate between 12 and 16 bits. We define an additional parameter called feedback frequency, v which defines how often the receiver[24] requests a specific codebook entry instead of equal power distribution and an average feedback bit rate as Rb=v(NV=NS).
It is also interesting to note that increasing the quality of quantization increases the feedback frequency v. This is a consequence of the fact that there is a higher probability of finding a good transmit signal covariance matrix when there are a lot of entries in the codebook.
We have simulated the 2×2 MIMO system using the OFDM modulation with carrier frequency: fc=2 GHz; signal bandwidth; B=5 MHz, number of sub-carriers: NOFDM=256; ITU-R M.1225 vehicular A channel model with independent channels for all pairs of transmit and receive antennas[22] [26]; the guard interval equal to the maximum channel delay.
The results of simulations are presented in
We assume that the communication system consists of a transmitter equipped with nT antennas[22] and K≥nT mobile receivers[24] with identical statistical properties and nR(k) antennas [26], where k=1,2, . . . K. The mobile user channels are modeled by a set of i.i.d. complex Gaussian channel matrices Hk of dimension nR(k)×nT. (Throughout the document we use the upper-case bold letters to denote matrices and lower-case bold letters to denote vectors.) The received signal of the kth user is then given by the nR(k)-dimensional vector yk defined as
y
k
=H
k
x+n
k (14)
where x is the nT-dimensional vector of the transmitted signal and nk is the nR(k)-dimensional vector consisting of independent circular complex Gaussian entries with zero means and unit variances. Finally, we assume that the total transmit power at each transmission instant is equal to P. The above assumptions cover a wide class of wireless systems and can easily be further expanded to include orthogonal frequency division multiplexing (OFDM) on frequency-selective channels or users with different received powers (due to varying path loss and shadowing).
Although theoretically it is possible to design the optimum CSI quantizer for the above canonical version of the system, such an approach may be impractical. For example, subsets of receivers[24] with different numbers of receive antennas[26] would require different CSI codebooks and quantizer design for such a system would be very complex. To alleviate this problem, we assume that the base station treats each user as if it was equipped with only one antenna[26], regardless of the actual number of antennas[26] it may have. While suboptimal, such an approach allows any type of a receiver[24] to work with any base station and may be even used to reduce the quantization noise as shown by Jindal. We call such system setup virtual multiple-input single-output (MISO) since, even though physically each transmitter-receiver link may be a MIMO link, from the base station's perspective it behaves like MISO.
We follow the approach of Spencer et al., where each user performs singular value decomposition of Hk=UkSkVkH[30] and converts its respective Hk to a nT-dimensional vector hk as
hk=ukHHk=skmaxvkh (15)
[42] where skmax is the largest singular value[30A] of Sk and uk and vk are its Corresponding vectors[30] from the unitary matrices Uk and Vk, respectively.
Based on (15), the only information that is fed[36],[36A] back from[34],[34A] the receivers[24] to the transmitter is the information about the vectors hk, which vastly simplifies the system design and allows for easy extensions. For example, if multiple streams per receiver are allowed, the channel information for each stream can be quantized using exactly the same algorithm.
In this section, we present typical approaches for the system design when full CSIT is available. As a simple form of multi-user selection diversity, we define a subset of active users with cardinality nT as S. Furthermore, for each subset S, we define a matrix H[S]=[h1T, h2T, . . . , hnTT]T, whose rows are equal to the channel vectors hk of the active users.
The upper-bound for system sum-rate is obtained when the users are assumed to be able to cooperate. With such an assumption, it is possible to perform singular value decomposition of the joint channel as H[S]=U[S]S[S]VH [S]. Defining si as the entries on the diagonal of S[S] allows to calculate the maximum sum-rale of a cooperative system as
where ξ[S] is the solution of the water-filling equation Σi=1n
In practice, the receivers[24] cannot cooperate and the full diagonalization of the matrix H[S] is impossible. The problem can still be solved by using linear zero-forcing (ZF) followed by non-linear dirty paper preceding, which effectively diagonalizes the channels to the active users. The matrix H[S] is first QR-decomposed as H[S]=L[S]Q[S], where L[S] is lower triangular matrix and Q[S] is a unitary matrix. After multiplying the input vector x by Q[S]H, the resulting channel is equal to L[S], i.e., the first user does not suffer from any multi-user interference (MUI), the second user receives interference only from the first user, etc.
In this case, non-causal knowledge of the previously encoded signals can be used in DPC encoder allowing the signal for each receiver[24] i>1 to be constructed in such a way that the previously encoded signals for users k<i, are effectively canceled at the ith receiver[24]. Since the effective channel matrix is lower triangular, the channel will be diagonalized after the DPC, with Ii being the entries on the diagonal of L[S]. This leads to maximum sum-rate calculation as
where ξ[Sord] is the solution of the water-filling equation. Note that, as opposed to (16), the maximization is performed over ordered versions of the active sets S.
Even though, theoretically, the above approach solves the problem of the receiver[24] non-cooperation, its inherent problem is the absence of effective, low complexity DPC algorithms. Moreover, since dirty-paper coding requires full CSIT it is likely that systems employing DPC would require significantly higher quality of channel feedback than simpler, linear precoding systems.
We use the linear block diagonalization approach, which eliminates MUI by composing the modulation matrix B[S] of properly chosen null-space eigenmodes for each set S. For each receiver[24] iϵ∈S, the ith row of the matrix H[S] is first deleted to form H[Si]. In the next step, the singular value decomposition is performed[30],[30A] to yield H[Si]=U[Si]S[Si]VH[Si]. By setting the ith column of B[S] to be equal to the rightmost vector of V[Si], we force the signal to the ith receiver[24] to be transmitted in the null-space of the other users and no MUI will appear. In other words, the channel will be diagonalized with di being the entries on the diagonal of H[S]B[S]. This leads to formula
where ξ[S] is the solution of the water-filling equation.
As an example,
The systems discussed so far are usually analyzed with assumption that, at any given time, the transmitter will have full information about the matrices [S]. Unfortunately, such an assumption is rather unrealistic and imperfect CSIT may render solutions relying on full CSIT useless.
In practice, the receivers[24] win quantize the information about their effective channel vectors hk[30] as ĥk[32], according to some optimization criterion. Based on this information, the transmitter will select[38],[52],[62] the best available modulation matrix {circumflex over (B)} from the predefined transmitter codebook and perform water-filling using the best predefined power division matrix {circumflex over (D)}. Regardless of the optimization criterion, the finite cardinality of the vector codebooks will increase MUI and lower system throughput.
The fundamental difference between CSI encoding in single-user and multiple-user systems is that during normal system operation, each receiver[24] chooses its vector ĥk without any cooperation with other receivers[24]. This means that the design of optimum codebook for hk must precede the design of codebooks {circumflex over (B)} and {circumflex over (D)}. Based on (15), one can see that channel state information in form of the vector hk consists of the scalar value of channel gain[30A] skmax and the eigenmode[30] νkH. Since these values are independent, we propose an algorithm which separately quantizes the information about eigenmodes[32] in codebook {circumflex over (v)} and amplitude gains[32A] in codebook ŝ.
We assume that Nv is the number of bits per channel realization in the feedback link needed to represent the vectors vk in (15). We divide the space of all possible v's into 2N
νi={v:γv(i;v)<γv(j;v) for all j≠i} (19)
where γv(n; v) is a distortion function. Within each region νi, we define a centroid vector {circumflex over (v)}(i)[49], which will be used as a representation of the region. The design of the codebook {circumflex over (v)} can be done analytically and/or heuristically using for example the Lloyd algorithm. In this work, we define the distortion function as the angle between the actual vector v and {circumflex over (v)}(i): γv(i;v)=cos−1({circumflex over (v)}(i)·v), which has been shown by Roh and Rhao to maximize ergodic capacity, and use Lloyd algorithm to train[47] the vector quantizer. Note that the construction of {circumflex over (v)} is independent of the transmit power.
We assume that Ns is the number of bits per channel realization in the feedback link needed to represent the scalar skmax in (15). We divide the space of all possible channel realizations s=skmax into 2N
s
i
={s:|ŝ(i)−s|<|ŝ(j)−s|for all j≠i} (20)
where ŝ(i) [100] are scalar centroids representing regions si. In this work, we perform the design[102] of the codebook ŝ using the classical non-uniform quantizer design algorithm with distortion function given by quadratic function of the quantization error as ∈(i;s)=(s−ŝ(i))2.
The construction of the codebook ŝ is generally dependent on the transmit power level. However, as pointed out above the differences between the codebooks ŝ for different power regions are quite small. This allows us to create only one codebook ŝ and use it for all transmit powers.
The calculation of the modulation matrix {circumflex over (B)} is based on the given codebook {circumflex over (v)}. We assume that the quantization[32] of the channel eigenmodes is performed at the receiver[24] side and each user transmits[34] back its codebook index ik. The indices are then used at the transmitter side to select[38] [52] [62] the modulation matrix {circumflex over (B)} (i1, i2, . . . iK). Since, from the linear transmitter point of view, ordering of the users is not important, we will use the convention that the indices (i1, i2, . . . iK) are always presented in the ascending order. For example, in a system with K=2, nT=2 and 1-bit vector quantizers {circumflex over (v)}, there will exist only three possible modulation matrices corresponding to sets of {circumflex over (v)} indices (1,1), (1,2) and (2,2).
In the context of vector quantizing, the design of the modulation matrices can no longer be based on the algorithm presented in Section VII.C. Using this method with quantized versions of hk produces wrong result when identical indices ik, are returned and the receiver[24] attempts to jointly optimize transmission to the users with seemingly identical channel vectors ĥk. Instead, we propose the following algorithm to optimize the set of matrices {circumflex over (B)}(i1, i2, . . . iK):
1. Create a large set of NnT random matrices[46] Hk, where N is the number of training sets with nT users each.
2. For each random matrix Hk, perform singular value decomposition[68] and obtain bk[70] as in (15).
3. For each vector hk store[74] the index ik of the corresponding entry {circumflex over (v)}(ik).
4. Divide[76] the entire set of matrices Hk into N sets with nT elements each.
5. Sort[78] the indices ik within each set l in the ascending order. Map[78] all unique sets of sorted indices to a set of unique indices IB (for example (1,1)→IB=1; (1,2)→IB=2; (2,2)→IB=3 . . . ).
6. In each set l, reorder the corresponding channel vectors hk according to their indices ik and calculate[80] the optimum Bl using the method from Section VII.C.
7. Calculate[84] a set {circumflex over (B)} (IB) as a column-wise spherical average of all entries Bl corresponding to the same[82] index IB.
After calculation of |IB| modulation matrices {circumflex over (B)}, the remaining part of system design is the calculation of the water-filling matrices {circumflex over (D)}, which divide the powers between the eigenmodes at the transmitter. The procedure for creation of codebook {circumflex over (D)}[118] is similar to the above algorithm, with the difference that the entries ŝ(nk) are used instead of {circumflex over (v)}(ik), and the spherical averaging of the water-filling matrices is performed diagonally, not column-wise. Explicitly:
1. Create a large set of NnT random matrices[46] Hk, where N is the number of training sets with nT users each.
2. For each random matrix Hk, perform singular value decomposition[104] and obtain hk as in (15).
3. For each vector hk store the index nk of the corresponding entry ŝ (nk).[106]
4. Divide the entire set of matrices Hk into N sets with nT elements each.[108]
5. Sort the indices nk within each set l in the ascending order. Map all unique sets of sorted indices to a set of unique indices ID (for example (1, 1)→ID=1; (1, 2)→ID=2; (2,2)→ID=3 . . . ).[110]
6. In each set l, reorder the corresponding channel vectors hk according to their indices nk and calculate the optimum Dl using the method of water-filling from Section VII.C.[112]
7. Calculate[116] a set {circumflex over (D)}(ID) as a diagonal spherical average of all entries Dl corresponding to the same[114] index ID.
The matrices {circumflex over (B)} and {circumflex over (D)} are used in the actual system in the following way:
1. The K mobile receivers[24] estimate[30],[30A] their channels and send the indices ik[34] and nk[34A] of the corresponding receiver quantizer entries {circumflex over (v)} (ik)[32] and ŝ (nk)[32A] to the base station.
2. The transmitter forms l sets of users corresponding to all combinations of nT users out of K. Within each set l, the indices ik[58] and nk[63] are sorted in the ascending order and mapped to their respective indices IB(l)[60] and ID(l)[64];
b 3. Within each set l, the matrices {circumflex over (B)} [IB(l)]0 [52],[62] and {circumflex over (D)} [ID(l)] [54],[38A] are used to estimate[56],[66] instantaneous sum-rate R(l).
4. The base station flags the set of users providing highest R(l) as active for the next transmission epoch.
5. The transmitter uses the selected matrices to transmit information.
The above algorithm does not assume any previous knowledge of the channel and the feedback rate required to initially acquire the channel may be high. In order to reduce it on slowly varying channels, we propose a nested quantization method shown in
We have implemented our system using a base station with nT=2 and a set of K mobile receivers[24] with identical statistical properties and nR(k)=nT=2. We have varied the number of users from 2 to 10 and optimized vector quantizers using methods presented above. Each system setup has been simulated using 10,000 independent channel realizations.
Note that further feedback rate reduction can be achieved with the algorithm presented by Jindal. However, we will not present these results here.
In case of multiple user systems, multi-user diversity may be achieved by a simple time-division multiplexing mode (when only one user at a time is given the full bandwidth of the channel) or scheduling the transmission to multiple user[24] at a time. Here we analyze the former approach and assume that the base station will schedule only one user[24] for transmission.
If the system throughput maximization is the main objective of the system design, the transmitter must be able to estimate[56] the throughput of each of the users, given the codebook indices it received from each of them. Assuming that the kth user returned indices requesting the eigenmode codeword {circumflex over (V)}k and power allocation codeword Ŝk, the user's actual throughput is given as
R
k
single=log2 det[In
Using singular value decomposition of channel matrix Hk and equality det[In
R
k
single=log2 det[In
where Ek=VkH{circumflex over (V)}k is a matrix representing the match between the actual eigenmode matrix of the channel and its quantized representation (with perfect match Ek=In
In practice, the actual realization of Ek will not be known at the transmitter, and its mean quantized value Êk, matched to {circumflex over (V)}k must be used instead. Similarly, the transmitter must use a quantized mean value {circumflex over (D)}k, which is matched to the reported water-filling matrix Ŝk. This leads to the selection criterion for the optimum user[24] kopt.
Similarly to single-user selection, also in the case of multi-user selection the choice of active users must be made based on incomplete CSIT. The quantized CSI will result in appearance of multi-user interference. We represent this situation using variable Êk,l={circumflex over (v)}kH[{circumflex over (B)}S].,l, which models the dot product of the quantized eigenmode {circumflex over (v)}kH reported by the kth user in the set S, and the lth vector in the selected modulation matrix[52] {circumflex over (B)}S.
Moreover, assuming that the quantized singular value of the kth user in the set S is given by {circumflex over (d)}k and the transmitter uses power allocation matrix[54] ŜS, the estimated sum-rate of the subset S is given as[56]
Note that, due to the finite resolution of the vector quantizer, the multi-user interference will lower the max sum-rate Rmulti(S)<Rmax for all S.
Based on (24) the choice of the active set of users is then performed as
One can also modify the algorithm presented in section II.A as follows: we use a simple iterative heuristic based on a modified form of the Lloyd algorithm, which has very good convergence properties. The algorithm starts by creating a random codebook of centroids {circumflex over (V)} and iteratively updates it until the mean distortion metric changes become smaller than a given threshold.
The algorithm works as follows:
1. Create a large training set of L random matrices Hl.[46]
2′ For each random matrix Hl, perform singular value decomposition to obtain Vl as in (3).
3′ Align orientation of each vector in Vl to lie within the same 2nT-dimensional hemisphere.
4. Set iteration counter i=0. Create a set of 2N
5. For each matrix Ĥ(n), calculate corresponding {circumflex over (V)}(i)(n) using singular value decomposition.
6. Align orientation of each vector in {circumflex over (V)}(i)(n) to lie within the same 2nTdimensional hemisphere.
7. For each training element Hl and codebook entry {circumflex over (V)}(i)(n), calculate the metric in (4). For every l, choose the index nopt(l) corresponding to the lowest value of γv(n;Hl). Calculate the subsets L(n)={l:nopt(l)=n} for all n.
8. Calculate new matrix {circumflex over (V)}(i+1)(n) as a constrained spherical average
{circumflex over (V)}(i+l)(n)=
9. For each region n, where cardinality |L(n)|≠0, calculate the mean eigenmode match matrix
10. Calculate the average distortion metric
V
(i+l)=1/LΣlγv(nopt(l);Hl)
11. If the distortion metric fulfills |
Upon completion of the above algorithm, the final set of vectors {circumflex over (V)} can be used to calculate the regions Vi in (5).
The design of the transmitter modulation matrices presented in section IX.C can be modified as follows: we propose the following algorithm to optimize the set of matrices {circumflex over (B)}(i1, i2, . . . in
1. Create a large set of LnT random matrices Hl, where L is the number of training sets with nT users each.
2. For each random matrix Hl, perform singular value decomposition[68] and obtain hl[70] as in (15).
3. Align orientation of each vector hl to lie within the same 2nT dimensional hemisphere.
4. For each vector hl, store[74] the index il of the corresponding entry {circumflex over (v)}(il).
5. Divide[76] the entire set of matrices Hl into L sets with nT elements each.
6. Sort[78] the indices il within each set in the ascending order. Map[78] all unique sets of sorted eigenmode indices il to a set of unique modulation matrix indices IB (for example, if nT=2: (1,1)→IB=1; (1,2)→IB=2; (2,2)→IB=3 . . . ).
7. In each set L(IB)={l:(i1, i2, . . . in
8. Calculate[84] the set {circumflex over (B)}(IB) as a column-wise spherical average of all entries Bl corresponding to the same[82] index IB as
∀n=1,2, . . . n
After completion of the above algorithm, the transmitter will have the set of |IB| modulation matrices {circumflex over (B)}(IB) corresponding to all sorted combinations of the channel eigenmode indices that can be reported by the receivers.
To clarify our notation for spherical average used in (26) and (28), we outline a method to calculate a spherical average of a set of unit-length vectors, and a spherical average of a set of unitary matrices, preserving the mutual perpendicularity of the component vectors. We use the notation
where the unit-length vector x is found using one of the constrained non-linear optimization algorithms.
In case of the spherical average of a set of unitary matrices, denoted as
Immaterial modifications may be made to the embodiments described here without departing from what is covered by the claims.
While illustrative embodiments have been illustrated and described, it will be appreciated that various changes can be made therein without departing from the spirit and scope of the invention.
This application is a continuation of U.S. application Ser. No. 16/436,532, filed Jun. 10, 2019, which is a continuation of U.S. application Ser. No. 14/628,570, filed Feb. 23, 2015, which issued as U.S. Pat. No. 10,320,453 on Jun. 11, 2019, which is a continuation of U.S. application Ser. No. 13/289,957, filed Nov. 4, 2011, which issued as U.S. Pat. No. 8,971,467 on Mar. 3, 2015, which is a division of U.S. application Ser. No. 11/754,965, filed May 29, 2007, which issued as U.S. Pat. No. 8,116,391 on Feb. 14, 2012, which claims the benefit of U.S. Provisional Patent Application No. 60/808,806, filed May 26, 2006, the entire disclosure of which is incorporated herein by reference.
Number | Date | Country | |
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60808806 | May 2006 | US |
Number | Date | Country | |
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Parent | 11754965 | May 2007 | US |
Child | 13289957 | US |
Number | Date | Country | |
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Parent | 16436532 | Jun 2019 | US |
Child | 17063213 | US | |
Parent | 14628570 | Feb 2015 | US |
Child | 16436532 | US | |
Parent | 13289957 | Nov 2011 | US |
Child | 14628570 | US |