One of the most promising solutions for increased spectral efficiency in high capacity wireless systems is the use of multiple antennas on fading channels. The fundamental issue in such systems is the availability of the channel state information (CSI) at transmitters and receivers. In general, if the receivers and transmitter have an access to CSI, the system throughput can be significantly increased. While it is usually assumed that perfect CSI is available at the receivers, the transmitter may only have partial CSI available 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. There is described here an improvement in the quantization of channel state information in a multiple antenna system.
A multi-tiered CSI vector quantizer (VQ) is provided for time-correlated channels. The VQ operates for example by quantizing channel state information by reference to both current channel state information and a prior channel state quantization. A system is also provided that uses multi-tiered CSI quantizers. Enhanced signaling between the transmitter and receivers is provided in order to facilitate the use of multi-tiered CSI quantizers. These and other aspects of the device and method are set out in the claims, which are incorporated here by reference.
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:
In a multiple antenna system as for example shown in
A vector quantizer (VQ) with multi-tiered quantization is aimed at transmission channels with memory, in which there is a need to reduce the feedback bandwidth and allow the system to automatically adjust the quantizer resolution to the rate of channel changes. In an exemplary design of a multi-tiered CSI vector quantizer (i.e., the description of centroids and Voronoi regions) for multiple-input, multiple-output (MIMO) channels with memory, the VQ uses multiple optimization steps.
In the typical CSI VQ, the quantization of the channel vector space can be illustrated as in
The quantization error can be decreased if the CSI VQ resolution is increased using more bits in feedback link.
The typical trajectory 28 of CSI vectors is partially predictable in a sense that the channel realizations between consecutive transmission epochs within the same frequency band are correlated. The correlation increases with decreasing relative speeds of receiver-transmitter pairs with the net effect of trajectories being statistically contained within a given Voronoi region for a predictable amount of time. The time metrics may be quantitative described in various ways such as using time metrics called eigenmode coherence time and singular value coherence time. In CSI VQ context, the longer the coherence time, the less frequent the changes in VQ indices that need to be reported back to the transmitter.
A multi-tiered VQ allows for a significant reduction of the feedback rate for systems in which channel coherence times are fairly long. During the design of the quantizer, the Voronoi regions are optimized according to any chosen criterion in 2, 3, 4 and more tiers, in which consecutive Voronoi regions are embedded in the previous ones as shown for example in
In the example of
The following notation is used in describing an exemplary multi-tiered VQ:
A system using a dual VQ codebook design for quantization of channel state information in a multiple antenna system is shown in
In
Referring to
The rationale behind re-using one of the m tier centroids at design phase of (m+1)-tier centroids and Voronoi regions (see bullet 5d above) is that the same set of modulation matrices can be used in a system where different users report their quantized channel information using different VQ tiers. As all m-tier centroids are contained in (m+1)-tier centroids, the effective indices can be easily used to decide which centroid must be used.
The algorithm from “Quantization of channel state information in multiple antenna systems” is as follows:
For the case of a single receiver active at a time, we introduce a heuristic distortion metric which is expressed as
γV(n;H)=∥DVH{circumflex over (V)}(n)−D∥F (1)
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 (1) for the clarity of presentation.
We assume that n=0, 1, . . . 2N
Vi={H:γV(i;H)<γV(j;H) for all j≠i}. (2)
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:
Upon completion of the above, algorithm, the set of vectors {circumflex over (V)} can be used to calculate the regions in (2).
Having optimized 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. 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) is the entry in {circumflex over (V)} codebook that minimizes metric (1) 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
Si(P)={H:γS(i;H;P)<γS(j;H;P) for all j≠i}. (7)
and to create the codebook Ŝ, we use the following method:
The set of vectors Ŝ is then used to calculate the regions in (7). Since water-filling 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. (2).
In the multi-user case, we follow the approach of Spencer et al, where each user performs singular value decomposition of Hk=UkSkVkH and converts its respective Hk to a nT-dimensional vector hk as
hk=ukHHk=skmaxvkH (11)
where skmax is the largest singular value of Sk and uk and vk are its corresponding vectors from the unitary matrices Uk and Vk, respectively.
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 iεS, 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 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 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.
We assume that Nν is the number of bits per than channel realization in the feedback link needed to represent the vectors vk in (11). We divide the space of all possible v's into 2N
νi={v:γν(i;v)<γν(j;v) for all j≠i} (13)
where γν(n;v) is a distortion function. Within each region νi we define a centroid vector {circumflex over (v)}(i), 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): γν(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 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 (11). We divide the space of all possible channel realizations s=smax into 2N
si={s:|ŝ(i)−s|<|ŝ(j)−s| for all j≠i} (14)
where ŝ(i) are scalar centroids representing regions si. In this work, we perform the design of the codebook ŝ using the classical non-uniform quantizer design algorithm with distortion function given by quadratic function of the quantization error as ε(i;s)=(s−ŝ(i))2.
The construction of the codebook ŝ is generally dependent on the transmit power level. However, 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 tar 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 of the channel eigenmodes is performed at the receiver side and each user transmits back its codebook index ik. The indices are then used at the transmitter side to select 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 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 for the single user case. Using this method with quantized versions of hk produces wrong result when identical indices ik are returned and the receiver 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):
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)} 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:
Referring to
The set of indices mk at the receivers should be matched to the indices mk at the transmitter. If the transmitter uses the index mk that corresponds to the wrong mk-tier of the receiver VQ, the resulting loss of performance may be very significant. In general, the index of the quantized channel vector at the transmitter is reconstructed as:
AAAABBBCCC . . . .
where AAAA corresponds to m=1 tier N1 indexing bits, BBB corresponds to m=2 tier N2 indexing bits etc. (see
At any given time, the transmitter receives only m-tier index bits (AAAA, BBB, CCC etc.) and it must be able to establish which tier those bits correspond to. For example, there must be a signaling method allowing the transmitter to distinguish between two consecutive transmissions such as BBB, BBB where the channel vector moved away from one tier-2 centroid to another, from the BBB, CCC transmission, where the channel vector stayed in the same tier-2 region BBB and tier-3 quantization was used in the CCC word.
Various methods may be used for transmitting index information from the receiver to the transmitter such as:
In the course of the system operation, it may happen that some of the transmitter indices Mk will no longer be synchronized with corresponding receiver indices mk. Such a situation will typically happen when one of the feedback messages from a receiver has not been detected at the transmitter (i.e., the transmitter lacks channel quantization index for the current transmission epoch) or the received message with the indexing information does not agree with the expected quantization tier m.
In practical communication systems, two erroneous situations can occur:
Various methods may be used to solve the problem such as:
In
In the claims, the word “comprising” is used in its inclusive sense and does not exclude other elements being present. The indefinite article “a” before a claim feature does not exclude more than one of the feature being present. Each one of the individual features described here may be used in one or more embodiments and is not, by virtue only of being described here, to be construed as essential to all embodiments as defined by the claims.
Immaterial modifications may be made to the embodiments described here without departing from what is covered by the claims.
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Child | 13083375 | US |