Doc.: IEEE 802.11-15/1289r0 Submission November 2015 Thomas Handte, SonySlide 1 Non-Uniform Constellations for 1024-QAM Date: 2015/11/08 Authors:

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doc.: IEEE /1289r0 Submission November 2015 Thomas Handte, SonySlide 1 Non-Uniform Constellations for 1024-QAM Date: 2015/11/08 Authors:

doc.: IEEE /1289r0 Submission Motivation 1024-QAM has been adopted for 11ax as an optional feature [1] –“1024-QAM is an optional feature for SU and MU using resource units equal to or larger than 242 tones in 11ax.” –Advantages 25% increase in spectral efficiency compared to 256-QAM Throughput up to 1.25 Gbps per spatial stream (160MHz, code rate 5/6, short GI) ≈10 Gbps aggregate throughput with 8 spatial streams [2] It has been shown [2, 3] for uniform constellations (UCs) that –1024-QAM MCS are selected with very high probability in indoor scenarios –1024-QAM provides an average throughput gain of >20% in most indoor scenarios However, non-uniform constellations (NUCs) are superior to UCs –NUCs provide SNR gains compared to UCs –NUCs are more robust against impairments such as phase noise and quantization Performance of 1024-QAM in 11ax can be increased by NUCs  Average throughput gain and selection probability of 1024-QAM MCS will increase November 2015 Slide 2Thomas Handte, Sony

doc.: IEEE /1289r0 Submission Outline Details on the proposed NUCs for 1024-QAM Complexity Analysis –Comparison of decoding complexity Performance Results –AWGN channel w/ and w/o phase noise w/ and w/o quantization effects –Performance in fading channels November 2015 Slide 3Thomas Handte, Sony

doc.: IEEE /1289r0 Submission Introduction Different types of NUCs can be distinguished –1D NUC High level of symmetry Amplitude levels of real and imaginary part are the same Bit labels of real and imaginary part can be separated –2D NUC Quadrant symmetry Amplitude levels of real and imaginary part are independent Bit labels can not be separated between real and imaginary part Comparison of NUC types –1D NUC performance gain over UC same complexity as UC –2D NUC even larger performance gain over UCs [4] higher complexity than 1D NUCs or UCs November 2015 Slide 4Thomas Handte, Sony 1D NUC: 16-QAM 2D NUC: 16-QAM

doc.: IEEE /1289r0 Submission 1D NUCs –Performance gain at negligible additional decoding complexity (see slide 7, [4]) Different NUCs for each code rate –Optimized for FEC operating point with specific code rate (CR) Optimized bit labeling –Matches optimally to existing.11 WLAN system No changes at FEC or other blocks required No need for a dedicated bit interleaver Proposed NUCs for 1024-QAM November 2015 Slide 5Thomas Handte, Sony

doc.: IEEE /1289r0 Submission Proposed NUCs for 1024-QAM (cont.) November 2015 Slide 6Thomas Handte, Sony

doc.: IEEE /1289r0 Submission 1D NUC correspond to a UC with non-uniform amplitude levels –Real and imaginary part can be independently demodulated In case of 1024-QAM, 2x32 metrics are sufficient for the demapping process which is the same for UCs –No additional complexity –Metric computation requires the consideration of the non-uniform shape Requires only a modification of the amplitude levels of the signal points within the demapper look-up tables –No additional complexity 1D NUCs yield no additional decoding complexity Decoding Complexity of 1D NUCs November 2015 Slide 7Thomas Handte, Sony

doc.: IEEE /1289r0 Submission 1024-QAM: Regular UC and NUC LDPC, approx. LLR Message length: 1000 bytes AWGN, channel model D Considered impairments: –w/ and w/o phase noise (PN) PN model according to evaluation methodology [5] –w/ and w/o quantization Fixed point quantization between FFT and demapper Performance compared at FER = Simulation Parameters November 2015 Slide 8Thomas Handte, Sony

doc.: IEEE /1289r0 Submission Results: Influence of Phase Noise November 2015 Slide 9 NUCs have similar degradation as UCs under PN influence –NUCs are even more robust against PN than UCs Small additional NUC gain Thomas Handte, Sony MCS10 CR 3/4 MCS11 CR 5/6

doc.: IEEE /1289r0 Submission Results: Quantization November 2015 Slide 10 Quantization between FFT and Demapper –Fixed-point implementation Number format: sign + 1 bit pre comma + M bits post comma Thomas Handte, Sony sgnb1b1 b2b2 …bMbM a1a1

doc.: IEEE /1289r0 Submission Results: Quantization (cont.) November 2015 Slide 11 NUC gain is maintained in presence of quantization –NUCs even show an additional gain compared to UCs for reasonable quantization Thomas Handte, Sony here: SNR gain = 0 dB

doc.: IEEE /1289r0 Submission Results: Fading Channel November 2015 Slide 12 Channel model D, time-varying –NUCs show an additional gain compared to UCs in fading channel Thomas Handte, Sony

doc.: IEEE /1289r0 Submission Conclusion Investigation of non-uniform constellations (NUCs) for 1024-QAM The proposed NUCs –achieve a gain of 0.3 dB –have no additional decoding complexity –maintain / even increase their gain over UCs in presence of Phase noise Quantization Fading channel November 2015 Slide 13Thomas Handte, Sony

doc.: IEEE /1289r0 Submission References ax Specification Framework for TGax ax 1024 QAM Proposal ax Investigation on 1024 QAM feasibility in 11ax ax Non-uniform Constellations for higher Order QAMs ac-tgac Functional requirements and evaluation methodology November 2015 Slide 14Thomas Handte, Sony

doc.: IEEE /1289r0 Submission TABLES November 2015 Slide 15Thomas Handte, Sony

doc.: IEEE /1289r0 Submission NUC for MCS10 (CR 3/4) November 2015 Slide 16Thomas Handte, Sony Amplitude level real part imaginary part b3b4b5b8b9b3b4b5b8b Re(z q ) Uniform ‑ u 15 ‑ u 14 ‑ u 13 ‑ u 12 ‑ u 11 ‑ u 10 ‑u9‑u9 ‑u8‑u8 ‑u7‑u7 ‑u6‑u6 ‑u5‑u5 ‑u4‑u4 ‑u3‑u3 ‑u2‑u2 ‑u1‑u1 NUC b3b4b5b8b9b3b4b5b8b Re(z q ) Uniform 1u1u1 u2u2 u3u3 u4u4 u5u5 u6u6 u7u7 u8u8 u9u9 u 10 u 11 u 12 u 13 u 14 u 15 NUC b0b1b2b6b7b0b1b2b6b Im(z q ) Uniform ‑ u 15 ‑ u 14 ‑ u 13 ‑ u 12 ‑ u 11 ‑ u 10 ‑u9‑u9 ‑u8‑u8 ‑u7‑u7 ‑u6‑u6 ‑u5‑u5 ‑u4‑u4 ‑u3‑u3 ‑u2‑u2 ‑u1‑u1 NUC b0b1b2b6b7b0b1b2b6b Im(z q ) Uniform 1u1u1 u2u2 u3u3 u4u4 u5u5 u6u6 u7u7 u8u8 u9u9 u 10 u 11 u 12 u 13 u 14 u 15 NUC

doc.: IEEE /1289r0 Submission NUC for MCS11 (CR 5/6) November 2015 Slide 17Thomas Handte, Sony Amplitude level real part imaginary part b0b3b5b7b8b0b3b5b7b Re(z q ) Uniform ‑ u 15 ‑ u 14 ‑ u 13 ‑ u 12 ‑ u 11 ‑ u 10 ‑u9‑u9 ‑u8‑u8 ‑u7‑u7 ‑u6‑u6 ‑u5‑u5 ‑u4‑u4 ‑u3‑u3 ‑u2‑u2 ‑u1‑u1 NUC b0b3b5b7b8b0b3b5b7b Re(z q ) Uniform 1u1u1 u2u2 u3u3 u4u4 u5u5 u6u6 u7u7 u8u8 u9u9 u 10 u 11 u 12 u 13 u 14 u 15 NUC b1b2b4b6b9b1b2b4b6b Im(z q ) Uniform ‑ u 15 ‑ u 14 ‑ u 13 ‑ u 12 ‑ u 11 ‑ u 10 ‑u9‑u9 ‑u8‑u8 ‑u7‑u7 ‑u6‑u6 ‑u5‑u5 ‑u4‑u4 ‑u3‑u3 ‑u2‑u2 ‑u1‑u1 NUC b1b2b4b6b9b1b2b4b6b Im(z q ) Uniform 1u1u1 u2u2 u3u3 u4u4 u5u5 u6u6 u7u7 u8u8 u9u9 u 10 u 11 u 12 u 13 u 14 u 15 NUC

doc.: IEEE /1289r0 Submission Straw Poll #1 Do you agree to add to the TG Specification Frame work document? Modulation “Non-uniform constellations shall be used for 1024-QAM” November 2015 Thomas Handte, SonySlide 18

doc.: IEEE /1289r0 Submission Straw Poll #2 Do you agree to add to the TG Specification Frame work document? Modulation “1024-QAM shall use non-uniform constellations for code rates 3/4 and 5/6 with amplitude levels and bit labels defined in slide 16 and 17, respectively?” November 2015 Thomas Handte, SonySlide 19

doc.: IEEE /1289r0 Submission APPENDIX November 2015 Slide 20Thomas Handte, Sony

doc.: IEEE /1289r0 Submission Example: How to get the bit labeling November 2015 Slide 21Thomas Handte, Sony

doc.: IEEE /1289r0 Submission Example: How to get the bit labeling (cont.) b1b2b3b6b7b1b2b3b6b Re(z q ) Uniform ‑ u 15 ‑ u 14 ‑ u 13 ‑ u 12 ‑ u 11 ‑ u 10 ‑u9‑u9 ‑u8‑u8 ‑u7‑u7 ‑u6‑u6 ‑u5‑u5 ‑u4‑u4 ‑u3‑u3 ‑u2‑u2 ‑u1‑u1 NUC b1b2b3b6b7b1b2b3b6b Re(z q ) Uniform 1u1u1 u2u2 u3u3 u4u4 u5u5 u6u6 u7u7 u8u8 u9u9 u 10 u 11 u 12 u 13 u 14 u 15 NUC November 2015 Slide 22Thomas Handte, Sony b0b4b5b8b9b0b4b5b8b Im(z q ) Uniform ‑ u 15 ‑ u 14 ‑ u 13 ‑ u 12 ‑ u 11 ‑ u 10 ‑u9‑u9 ‑u8‑u8 ‑u7‑u7 ‑u6‑u6 ‑u5‑u5 ‑u4‑u4 ‑u3‑u3 ‑u2‑u2 ‑u1‑u1 NUC b0b4b5b8b9b0b4b5b8b Im(z q ) Uniform 1u1u1 u2u2 u3u3 u4u4 u5u5 u6u6 u7u7 u8u8 u9u9 u 10 u 11 u 12 u 13 u 14 u 15 NUC real part imaginary part