Space Time Block Coding for SC PHY in 11ay

Slides:



Advertisements
Similar presentations
Cyclic Shift Diversity Design for IEEE aj (45GHz)
Advertisements

Institute of Communications Engineering, NCTU 1 Unit 2 Synchronization.
a By Yasir Ateeq. Table of Contents INTRODUCTION TASKS OF TRANSMITTER PACKET FORMAT PREAMBLE SCRAMBLER CONVOLUTIONAL ENCODER PUNCTURER INTERLEAVER.
Department of electrical and computer engineering An Equalization Technique for High Rate OFDM Systems Mehdi Basiri.
Doc.: IEEE / 710r0 Submission May 2015 Variable Length Guard Interval for 45GHz Date: Authors: NameAffiliationsAddressPhone Feng.
Doc.:IEEE /0206r0 Submission January 2015 Shiwen He, Haiming Wang Pilot Design for OFDM PHY for aj(45 GHz) Authors/contributors: Date:
1 CFO Estimation with ICI Cancellation for OFDM Systems 吳宗威.
Muhammad Imadur Rahman1, Klaus Witrisal2,
Doc.: IEEE /1391r0 Submission Nov Yakun Sun, et. Al.Slide 1 About SINR conversion for PHY Abstraction Date: Authors:
Doc.: IEEE /1399r0 Submission November 2014 Multi-Carrier Training Field for OFDM Transmission in aj (45GHz) Authors/contributors: Date:
Doc.: IEEE / 0710r1 Submission May 2015 Gigaray Communication Variable Length Guard Interval for 45GHz Date: Authors: NameAffiliationsAddressPhone .
OFDM Presented by Md. Imdadul Islam.
Submission doc.: IEEE 11-13/1059r0 September 2013 Dongguk Lim, LG ElectronicsSlide 1 PHY Abstraction for HEW Evaluation Methodology Date: Authors:
Submission doc.: IEEE /1088r0 September 2015 Daewon Lee, NewracomSlide 1 LTF Design for Uplink MU-MIMO Date: Authors:
Doc.: IEEE /0205r0 Submission Jan 2015 Shiwen He, Haiming Wang Slide 1 Time Domain Multiplexed Pilots Design for IEEE802.11aj(45 GHz) SC PHY Authors/contributors:
Doc.: IEEE /0363r2 Submission Pilot Value Definitions May 2012 Yongho Seok (LG Electronics), Hongyuan Zhang (Marvell)Slide 1 Date:
Introduction to OFDM and Cyclic prefix
بسم الله الرحمن الرحيم Lecture (12) Dr. Iman Abuel Maaly The Discrete Fourier Transform Dr. Iman Abuel Maaly University of Khartoum Department of Electrical.
Doc.: IEEE /0994r1 Submission July 2016 Intel CorporationSlide 1 EDMG STF and CEF Design for SC PHY in 11ay Date: Authors:
Doc.: IEEE /0632r1 Submission May 2016 Intel CorporationSlide 1 Performance Analysis of Robust Transmission Modes for MIMO in 11ay Date:
SC PHY EDMG-CEF Design for Channel Bonding x3
Homework 3 1. Suppose we have two four-point sequences x[n] and h[n] as follows: (a) Calculate the four-point DFT X[k]. (b) Calculate the four-point DFT.
Consideration of PHY design for 1.08GHz channel
Space-Time and Space-Frequency Coded Orthogonal Frequency Division Multiplexing Transmitter Diversity Techniques King F. Lee.
EDMG-CEF Extension for SC MIMO
OFDM Pilots Definition in 11ay
EDMG-STF for OFDM Date: Authors: May 2017 Name Company
Length 1344 LDPC codes for 11ay
MIMO Coding for SC PHY in 11ay
EDMG Header-B Encoding and Modulation for SC PHY in 11ay
Clarification on TRN Subfield Definition for MIMO
1MHz SIG Field Discussions
EDMG STF for OFDM in 2,3,4CB Date: Authors: July 2017 Name
MCS 1 LDPC Encoding Method Modification in 11ay
Channel Estimation Field for EDMG OFDM PHY in 11ay
Rate 7/8 LDPC Code for 11ay Date: Authors:
Rate 7/8 (1344,1176) LDPC code Date: Authors:
OFDM Signal Parameters Definition in 11ay
Symbol Blocking and Guard Interval Definition for SC MIMO in 11ay
EDMG TRN Subfields Definition for SC PHY
Fast Fourier Transforms Dr. Vinu Thomas
I-Q Decoupled OFDM: A Solution to I/Q Imbalance
Hybrid Beamforming Protocol Design Details
Channel Estimation 黃偉傑.
Month Year doc.: IEEE yy/xxxxr0 Mar 2017
4.1 DFT In practice the Fourier components of data are obtained by digital computation rather than by analog processing. The analog values have to be.
Discussions on HE SIG-A Structure
Chapter 8 The Discrete Fourier Transform
Submission Title: [Proposed resolution to MIMO CES]
Pilot Value Definitions
Packet structure for SC EDMG PPDU for each GI length
I-Q Decoupled OFDM Modulation
Pilot Sequence for VHT-DATA
Hybrid Beamforming Protocol Design Details
MIMO Coding for SC PHY in 11ay
Month Year doc.: IEEE yy/xxxxr0 January 2008
May 2016 doc.: IEEE /XXXXr0 May 2016
Optimizing OOK Waveform for High Data Rate WUS
STBC for OFDM PHY in 11ay Date: Authors: May 2017 May 2017
Submission Title: [Proposed resolution to MIMO CES]
Joint Coding and Modulation Diversity for ah
Header-A Definition for EDMG Control Mode
11ac 80MHz Transmission Flow
Header-A Definition for EDMG Control Mode
Strawmodel ac Specification Framework
Repetition and interleaver design for MCS0-Rep2
Discussion on Rank Adaptation
PHY Performance Evaluation with 60 GHz WLAN Channel Models
Clarification on TRN Subfield Definition for MIMO
EDMG STF and CEF Design for SC PHY in 11ay
Presentation transcript:

Space Time Block Coding for SC PHY in 11ay April 2017 doc.: IEEE 802.11-16/XXXXr0 April 2017 Space Time Block Coding for SC PHY in 11ay Date: 2017-04-11 Authors: Intel Corporation Intel Corporation

April 2017 Introduction This presentation proposes a Space Time Block Code (STBC) for SC PHY, [1]. Intel Corporation

SC Symbol Blocking for STBC April 2017 SC Symbol Blocking for STBC The proposed STBC scheme applies coding to the data part of the SC symbol block and utilizes symbol blocking structure defined in [1]. It performs mapping of a single spatial stream (NSS = 1) to two space-time streams (NSTS = 2). The STBC code combining is performed in frequency domain in a similar way as for OFDM in 11n/ac, [2]. Intel Corporation

SC Symbol Blocking for STBC (Cont’d) April 2017 SC Symbol Blocking for STBC (Cont’d) STBC coding: Input – two SC symbol blocks xNSPB and yNSPB, NSPB defines the number of symbols per SC block; For example, let’s define NSPB = 448 as in case of normal GI type; (x448(n), y448(n)) blocks are mapped to the first space-time stream; (-y*448(-n), x*448(-n)) blocks are mapped to the second space-time stream; (g1,64(n), g2,64(n)) are two Guard Intervals (GIs) of length 64 for space-time stream 1 and 2 accordingly; Figure below illustrates the proposed structure, (-n) defines reverse of symbols in time, * defines complex conjugation; Intel Corporation

Signals Definition Transmit signals in frequency domain: April 2017 STS#1: XT1(k) = X(k) + G1(k); YT2(k) = Y(k) + G1(k); where: X = DFT(x), Y = DFT(y), G1 = DFT(g1), G2 = DFT(g2); Intel Corporation

Signals Definition (Cont’d) April 2017 Signals Definition (Cont’d) Received signals in frequency domain: Time interval T1: RT1(k) = H1(k)*X(k) – ph(k)*H2(k)*Y*(k) + H1(k)*G1(k) + H2(k)*G2(k) + ZT1(k); Time interval T2: RT2(k) = ph(k)*H2(k)*X*(k) + H1(k)*Y(k) + H1(k)*G1(k) + H2(k)*G2(k) + ZT2(k); where: ph(k) = exp(+j(2π/512)*Δt*k), Δt = 65 chips; ZT1(k) and ZT2(k) – AWGN ~CN(0, σ2) noise samples; Intel Corporation

Signals Definition (Cont’d) April 2017 Signals Definition (Cont’d) Phasor explanation for STS#2: x*(-n) = ( x*(447), x*(446), …, x*(0), 00, 01, …, 063 ); Phasor operation applied in frequency domain makes cyclic shift in time domain as follows: x~(n) = (x*(0), 00, 01, …, 063, x*(447), x*(446), …, x*(1) ); Due to the property of DFT provided in Appendix, this gives complex conjugated subcarriers in frequency domain, i.e. X*(k) = DFT(x~(n)); Hence, DFT(x*(-n)) * exp(-j(2π/512)*65*k) = X*(k); and DFT(x*(-n)) = X*(k) * exp(+j(2π/512)*65*k); The same derivation is applicable for y*(-n) signal; Phasor can be treated as a part of H2 channel; Intel Corporation

April 2017 Demodulation Method The combining method is similar to OFDM 11n/ac, the difference is that MMSE solution is used: The estimated X^(k) and Y^(k) signals can be written as follows: This provides data estimation in the frequency domain, which in turn can be transformed to the time domain applying IDFT to get x^(n) and y^(n) estimations; Intel Corporation

Demodulation Method (Cont’d) April 2017 Demodulation Method (Cont’d) MMSE equalizer for GI part: The equalizer solution considered at the previous slide provides a “perfect” equalization of the data part only, but NOT for the GI part of the signal; After conversion to the time domain GI sequences will not be “perfectly" equalized; Due to the fact that GI signals are known to receiver, they can be pre-calculated during channel estimation stage as follows: The g~1 and g~2 signals can be used for phase tracking in time domain as known GIs; Intel Corporation

April 2017 SP/M Do you agree: to include the text from (11-17-0587-00-00ay 30 5 6 4 3 Space Time Block Coding) defining SC STBC scheme to the spec draft? Intel Corporation

Appendix April 2017 DFT complex conjugation property: DFT: Complex conjugated sample in frequency domain: Specific example for N = 4: Can be rewritten: Using: Reordering: In general case: Intel Corporation

References Draft P802.11ay_D0.3 IEEE802.11-2016 April 2017 Intel Corporation