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arXiv:1901.08186 · IEEE International Symposium on Information Theory (ISIT)

Explicit Polar Codes with Small Scaling Exponent

Hanwen Yao, Arman Fazeli, Alexander Vardy

Published Jul 1, 2019• 29 citations
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Abstract

Polar coding gives rise to the first explicit family of codes that provably achieve capacity for a wide range of channels with efficient encoding and decoding. But how fast can polar coding approach capacity as a function of the code length? In finite-length analysis, the scaling between code length and the gap to capacity is usually measured in terms of the scaling exponent μ. It is well known that the optimal scaling exponent, achieved by random binary codes, is μ = 2. It is also well known that the scaling exponent of conventional polar codes on the binary erasure channel (BEC) is μ = 3.627, which falls far short of the optimal value. On the other hand, it was recently shown that polar codes derived from ℓ × ℓ binary polarization kernels approach the optimal scaling exponent μ = 2 on the BEC as ℓ→∞, with high probability over a random choice of the kernel. Herein, we focus on explicit constructions of ℓ×ℓ binary kernels with small scaling exponent for ℓ ≤ 64. In particular, we exhibit a sequence of binary linear codes that approaches capacity on the BEC with quasi-linear complexity and scaling exponent μℓtransforms an underlying BEC into ℓ bit-channels W1, W2>,..., Wℓ. The erasure probabilities of W1, W2>,..., Wℓ, known as the polarization behavior of Kℓ, determine the resulting scaling exponent μ(Kℓ). We first introduce a class of self-dual binary kernels and prove that their polarization behavior satisfies a strong symmetry property. This reduces the problem of constructing Kℓto that of producing a certain nested chain of only ℓ/2 self-orthogonal codes. We use nested cyclic codes, whose distance is as high as possible subject to the orthogonality constraint, to construct the kernels K32and K64. In order to evaluate the polarization behavior of K32and K64, two alternative trellis representations (which may be of independent interest) are proposed. Using the resulting trellises, we show that μ(K32) = 3.122 and explicitly compute over half of the polarization-behavior coefficients for K64, at which point the complexity becomes prohibitive. To complete the computation, we introduce a Monte-Carlo interpolation method, which produces the estimate μ(K64) ≃ 2.87. We augment this estimate with a rigorous proof that μ(K64) <; 2.97.

DOI
10.1109/isit.2019.8849741

Related papers

Finite-Length Scaling for Polar Codes

Hamed Hassani, Kasra Alishahi, Rudiger L. Urbanke

Consider a binary-input memoryless output-symmetric channel\(W\). Such a channel has a capacity, call it\(I(W)\), and for any\(R<I(W)\)and strictly positive constant\(P_{\rm e}\)we know that we can construct a coding scheme that allows transmission at rate\(R\)with an error probability not exceeding\(P_{\rm e}\). Assume now that we let the rate\(R\)tend to\(I(W)\)and we ask how we have to scale the blocklength\(N\)in order to keep the error probability fixed to\(P_{\rm e}\). We refer to this as the finite-length scaling behavior. This question was addressed by Strassen as well as Polyanskiy, Poor, and Verdu, and the result is that\(N\)must grow at least as the square of the reciprocal of\(I(W)-R\). Polar codes are optimal in the sense that they achieve capacity. In this paper, we are asking to what degree they are also optimal in terms of their finite-length behavior. Since the exact scaling behavior depends on the choice of the channel, our objective is to provide scaling laws that hold universally for all binary-input memoryless output-symmetric channels. Our approach is based on analyzing the dynamics of the un-polarized channels. More precisely, we provide bounds on (the exponent of) the number of subchannels whose Bhattacharyya constant falls in a fixed interval\([a,b]\). Mathematically, this can be stated as bounding the sequence\(\bigl \{{1}/{n} \log {\rm {Pr}}(Z_{n} \!\in \! [a,b])\bigr \}_{n \in \mathbb {N}}\), where\(Z_{n}\)is the Bhattacharyya process. We then use these bounds to derive tradeoffs between the rate and the block-length. The main results of this paper can be summarized as follows. Consider the sum of Bhattacharyya parameters of subchannels chosen (by the polar coding scheme) to transmit information. If we require this sum to be smaller than a given value\(P_{\rm e}>0\), then the required block-length\(N\)scales in terms of the rate\(R < I(W)\)as\(N \geq {\alpha }/{(I(W)-R)^{\underline {\mu }}}\), where\(\alpha \)is a positive constant that depends on\(P_{\rm e}\)and\(I(W)\). We show that\(\underline {\mu } = 3.579\)is a valid choice, and we conjecture that indeed the value of\(\underline {\mu }\)can be improved to\(\underline {\mu }=3.627\), the parameter for the binary erasure channel. Also, we show that with the same requirement on the sum of Bhattacharyya parameters, the block-length scales in terms of the rate like\(N \leq {\beta }/{(I(W)-R)^{\overline {\mu }}}\), where\(\beta \)is a constant that depends on\(P_{\rm e}\)and\(I(W)\), and\(\overline {\mu }=6\).

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Scaling Exponent of List Decoders with Applications to Polar Codes

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Motivated by the significant performance gains which polar codes experience under successive cancellation list decoding, their scaling exponent is studied as a function of the list size. In particular, the error probability is fixed and the trade-off between block length and back-off from capacity is analyzed. A lower bound is provided on the error probability under $\rm MAP$ decoding with list size $L$ for any binary-input memoryless output-symmetric channel and for any class of linear codes such that their minimum distance is unbounded as the block length grows large. Then, it is shown that under $\rm MAP$ decoding, although the introduction of a list can significantly improve the involved constants, the scaling exponent itself, i.e., the speed at which capacity is approached, stays unaffected for any finite list size. In particular, this result applies to polar codes, since their minimum distance tends to infinity as the block length increases. A similar result is proved for genie-aided successive cancellation decoding when transmission takes place over the binary erasure channel, namely, the scaling exponent remains constant for any fixed number of helps from the genie. Note that since genie-aided successive cancellation decoding might be strictly worse than successive cancellation list decoding, the problem of establishing the scaling exponent of the latter remains open.

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Or Ordentlich, Yury Polyanskiy

Consider a binary linear code of length N, minimum distance d-{\min}, transmission over the binary erasure channel with parameter 0 < \epsilon < 1 or the binary symmetric channel with parameter 0 < \epsilon < \frac{1}{2}, and block-MAP decoding. It was shown by Tillich and Zemor that in this case the error probability of the block-MAP decoder transitions 'quickly' from \delta to 1-\delta for any \delta > 0 if the minimum distance is large. In particular the width of the transition is of order O(1/\sqrt{d-{\min}}). We strengthen this result by showing that under suitable conditions on the weight distribution of the code, the transition width can be as small as \Theta(1/N^{\frac{1}{2}-\kappa}), for any \kappa > 0, even if the minimum distance of the code is not linear. This condition applies e.g., to Reed-Mueller codes. Since \Theta(1/N^{\frac{1}{2}}) is the smallest transition possible for any code, we speak of 'almost' optimal scaling. We emphasize that the width of the transition says nothing about the location of the transition. Therefore this result has no bearing on whether a code is capacity-achieving or not. As a second contribution, we present a new estimate on the derivative of the EXIT function, the proof of which is based on the Blowing-Up Lemma.

•Jun 1, 2018•16 citations
Polar coding gives rise to the first explicit family of codes that provably achieve capacity for a wide range of channels with efficient encoding and decoding. But how fast can polar coding approach capacity as a function of the code length? In finite-length analysis, the scaling between code length and the gap to capacity is usually measured in terms of the scaling exponent μ. It is well known that the optimal scaling exponent, achieved by random binary codes, is μ = 2. It is also well known that the scaling exponent of conventional polar codes on the binary erasure channel (BEC) is μ = 3.627, which falls far short of the optimal value. On the other hand, it was recently shown that polar codes derived from ℓ × ℓ binary polarization kernels approach the optimal scaling exponent μ = 2 on the BEC as ℓ→∞, with high probability over a random choice of the kernel. Herein, we focus on explicit constructions of ℓ×ℓ binary kernels with small scaling exponent for ℓ ≤ 64. In particular, we exhibit a sequence of binary linear codes that approaches capacity on the BEC with quasi-linear complexity and scaling exponent μℓtransforms an underlying BEC into ℓ bit-channels W1, W2>,..., Wℓ. The erasure probabilities of W1, W2>,..., Wℓ, known as the polarization behavior of Kℓ, determine the resulting scaling exponent μ(Kℓ). We first introduce a class of self-dual binary kernels and prove that their polarization behavior satisfies a strong symmetry property. This reduces the problem of constructing Kℓto that of producing a certain nested chain of only ℓ/2 self-orthogonal codes. We use nested cyclic codes, whose distance is as high as possible subject to the orthogonality constraint, to construct the kernels K32and K64. In order to evaluate the polarization behavior of K32and K64, two alternative trellis representations (which may be of independent interest) are proposed. Using the resulting trellises, we show that μ(K32) = 3.122 and explicitly compute over half of the polarization-behavior coefficients for K64, at which point the complexity becomes prohibitive. To complete the computation, we introduce a Monte-Carlo interpolation method, which produces the estimate μ(K64) ≃ 2.87. We augment this estimate with a rigorous proof that μ(K64) <; 2.97.
Consider a binary-input memoryless output-symmetric channelWWW. Such a channel has a capacity, call itI(W)I(W)I(W), and for anyR<I(W)R<I(W)R<I(W)and strictly positive constantPeP_{\rm e}Pe​we know that we can construct a coding scheme that allows transmission at rateRRRwith an error probability not exceedingPeP_{\rm e}Pe​. Assume now that we let the rateRRRtend toI(W)I(W)I(W)and we ask how we have to scale the blocklengthNNNin order to keep the error probability fixed toPeP_{\rm e}Pe​. We refer to this as the finite-length scaling behavior. This question was addressed by Strassen as well as Polyanskiy, Poor, and Verdu, and the result is thatNNNmust grow at least as the square of the reciprocal ofI(W)−RI(W)-RI(W)−R. Polar codes are optimal in the sense that they achieve capacity. In this paper, we are asking to what degree they are also optimal in terms of their finite-length behavior. Since the exact scaling behavior depends on the choice of the channel, our objective is to provide scaling laws that hold universally for all binary-input memoryless output-symmetric channels. Our approach is based on analyzing the dynamics of the un-polarized channels. More precisely, we provide bounds on (the exponent of) the number of subchannels whose Bhattacharyya constant falls in a fixed interval[a,b][a,b][a,b]. Mathematically, this can be stated as bounding the sequence{1/nlog⁡Pr(Zn ⁣∈ ⁣[a,b])}n∈N\bigl \{{1}/{n} \log {\rm {Pr}}(Z_{n} \!\in \! [a,b])\bigr \}_{n \in \mathbb {N}}{1/nlogPr(Zn​∈[a,b])}n∈N​, whereZnZ_{n}Zn​is the Bhattacharyya process. We then use these bounds to derive tradeoffs between the rate and the block-length. The main results of this paper can be summarized as follows. Consider the sum of Bhattacharyya parameters of subchannels chosen (by the polar coding scheme) to transmit information. If we require this sum to be smaller than a given valuePe>0P_{\rm e}>0Pe​>0, then the required block-lengthNNNscales in terms of the rateR<I(W)R < I(W)R<I(W)asN≥α/(I(W)−R)μ‾N \geq {\alpha }/{(I(W)-R)^{\underline {\mu }}}N≥α/(I(W)−R)μ​, whereα\alpha αis a positive constant that depends onPeP_{\rm e}Pe​andI(W)I(W)I(W). We show thatμ‾=3.579\underline {\mu } = 3.579μ​=3.579is a valid choice, and we conjecture that indeed the value ofμ‾\underline {\mu }μ​can be improved toμ‾=3.627\underline {\mu }=3.627μ​=3.627, the parameter for the binary erasure channel. Also, we show that with the same requirement on the sum of Bhattacharyya parameters, the block-length scales in terms of the rate likeN≤β/(I(W)−R)μ‾N \leq {\beta }/{(I(W)-R)^{\overline {\mu }}}N≤β/(I(W)−R)μ​, whereβ\beta βis a constant that depends onPeP_{\rm e}Pe​andI(W)I(W)I(W), andμ‾=6\overline {\mu }=6μ​=6.
Consider the transmission of a polar code of block length N and rate R over a binary memoryless symmetric channel W and let Pebe the block error probability under successive cancellation decoding. In this paper, we develop new bounds that characterize the relationship of the parameters R, N, Pe, and the quality of the channel W quantified by its capacity I(W) and its Bhattacharyya parameter Z(W). In previous work, two main regimes were studied. In the error exponent regime, the channel W and the rate R-√N. In the scaling exponent approach, the channel W and the error probability Pe are fixed and it was proved that the gap to capacity I(W) - R scales as N-1/μ. Here, μ is called scaling exponent and this scaling exponent depends on the channel W. A heuristic computation for the binary erasure channel (BEC) gives μ = 3.627 and it was shown that, for any channel W, 3.579 ≤ μ ≤ 5.702. Our contributions are as follows. First, we provide the tighter upper bound μ <;≤ 4.714 valid for any W. With the same technique, we obtain the upper bound μ ≤ 3.639 for the case of the BEC; this upper bound approaches very closely the heuristically derived value for the scaling exponent of the erasure channel. Second, we develop a trade-off between the gap to capacity I(W)- R and the error probability Pe as the functions of the block length N. In other words, we neither fix the gap to capacity (error exponent regime) nor the error probability (scaling exponent regime), but we do consider a moderate deviations regime in which we study how fast both quantities, as the functions of the block length N, simultaneously go to 0. Third, we prove that polar codes are not affected by error floors. To do so, we fix a polar code of block length N and rate R. Then, we vary the channel W and study the impact of this variation on the error probability. We show that the error probability Pe scales as the Bhattacharyya parameter Z(W) raised to a power that scales roughly like VN. This agrees with the scaling in the error exponent regime.
Polar codes constructed with large polarization kernels were recently proven to be able to achieve optimal finite-length scaling properties. However, straightforward decoding for large kernel polar codes introduces a complexity coefficient that is exponential to the kernel sizes, which makes such codes generally believed to be impractical. In this paper, we present a new method that decodes large kernel polar codes with a complexity coefficient that is polynomial to the kernel sizes. This could facilitate the implementation of large kernel polar codes for practical use in the future.Successive cancellation decoding for large kernel polar codes requires calculation on the probabilities of its bit channels. Similar to conventional polar codes, those bit channels follow a recursive relation, which make this calculation boil down to computing the probabilities for bit channels of a single polarization kernel. This kernel-level computation can be shown equivalent to soft-output maximum-likelihood (ML) decoding on a single bit of a linear block code. In our proposed method, we first use linear operations to represent the considered linear block code as a polar code with dynamically frozen bits, and then use a modified polar list decoder to get an approximate value on the soft-output of the desired bit. This method is motivated by the observation that at short block lengths, polar list decoding with a large enough list size can well-approximate ML decoding. The proposed low-complexity method allows us to decode polar codes constructed with a 64 × 64 polarization kernel with scaling exponent µ ≈ 2.87 for the first time.
A pruned variant of polar coding is proposed for binary erasure channel (BEC). Fix any BEC. For sufficiently small ε > 0, we construct a series of capacity achieving codes with block length N = ε-4.9, code rate R = Capacity - O(ε), block error probability P = ε, and encoding and decoding time complexity bC = O(log|log ε|) per information bit. The given per-bit complexity bC is log-logarithmic in N, in Capacity - R, and in P. Beyond BEC, there is a generalization: Fix a prime q and fix a symmetric, q-ary-input, discrete-output memoryless channel. For sufficiently small ε > 0, we construct a series of error correction codes with block length N = ε-constant, code rate R = Capacity - O(ε), block error probability P = ε, and encoding and decoding time complexity bC = O(log|log ε|) per information bit. Over general channels, this family of codes has the lowest per-bit time complexity among all capacity-achieving codes known to date.
Motivated by the significant performance gains which polar codes experience under successive cancellation list decoding, their scaling exponent is studied as a function of the list size. In particular, the error probability is fixed and the trade-off between block length and back-off from capacity is analyzed. A lower bound is provided on the error probability under MAP\rm MAPMAP decoding with list size LLL for any binary-input memoryless output-symmetric channel and for any class of linear codes such that their minimum distance is unbounded as the block length grows large. Then, it is shown that under MAP\rm MAPMAP decoding, although the introduction of a list can significantly improve the involved constants, the scaling exponent itself, i.e., the speed at which capacity is approached, stays unaffected for any finite list size. In particular, this result applies to polar codes, since their minimum distance tends to infinity as the block length increases. A similar result is proved for genie-aided successive cancellation decoding when transmission takes place over the binary erasure channel, namely, the scaling exponent remains constant for any fixed number of helps from the genie. Note that since genie-aided successive cancellation decoding might be strictly worse than successive cancellation list decoding, the problem of establishing the scaling exponent of the latter remains open.
Consider a binary linear code of length N, minimum distance d-{\min}, transmission over the binary erasure channel with parameter 0 < \epsilon < 1 or the binary symmetric channel with parameter 0 < \epsilon < \frac{1}{2}, and block-MAP decoding. It was shown by Tillich and Zemor that in this case the error probability of the block-MAP decoder transitions 'quickly' from \delta to 1-\delta for any \delta > 0 if the minimum distance is large. In particular the width of the transition is of order O(1/\sqrt{d-{\min}}). We strengthen this result by showing that under suitable conditions on the weight distribution of the code, the transition width can be as small as \Theta(1/N^{\frac{1}{2}-\kappa}), for any \kappa > 0, even if the minimum distance of the code is not linear. This condition applies e.g., to Reed-Mueller codes. Since \Theta(1/N^{\frac{1}{2}}) is the smallest transition possible for any code, we speak of 'almost' optimal scaling. We emphasize that the width of the transition says nothing about the location of the transition. Therefore this result has no bearing on whether a code is capacity-achieving or not. As a second contribution, we present a new estimate on the derivative of the EXIT function, the proof of which is based on the Blowing-Up Lemma.