Doc.: IEEE 802.15-04/0326r0 Submission July 2004 C. Razzell, PhilipsSlide 1 Project: IEEE P802.15 Working Group for Wireless Personal Area Networks (WPANs)

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doc.: IEEE /0326r0 Submission July 2004 C. Razzell, PhilipsSlide 1 Project: IEEE P Working Group for Wireless Personal Area Networks (WPANs) Submission Title: [APD plots and their implications for MB-OFDM UWB interference] Date Submitted: [9 July, 2004] Source: [Charles Razzell] Company [Philips] Address [1109, McKay Drive, San Jose, CA 95131, USA] Voice:[ ], FAX: [ ], Re: [An often cited reason for no-votes in a down-selection process ] Abstract:[Presents simulated APD plots for MB-OFDM and discusses implications for interference] Purpose:[Consider how MB-OFDM compares to other UWB waveforms anticipated by FCC rules.] Notice:This document has been prepared to assist the IEEE P It is offered as a basis for discussion and is not binding on the contributing individual(s) or organization(s). The material in this document is subject to change in form and content after further study. The contributor(s) reserve(s) the right to add, amend or withdraw material contained herein. Release:The contributor acknowledges and accepts that this contribution becomes the property of IEEE and may be made publicly available by P

doc.: IEEE /0326r0 Submission July 2004 C. Razzell, PhilipsSlide 2 APD Plots and their Implications for MB-OFDM

doc.: IEEE /0326r0 Submission July 2004 C. Razzell, PhilipsSlide 3 Amplitude Probability Distributions APD methodology is favored by the NTIA in assessing interference impact of UWB waveforms For non-Gaussian interference, APD plots provide helpful insight into potential impact on victim receivers. For full impact assessment, knowledge of the victim system’s modulation scheme and FEC performance is needed

doc.: IEEE /0326r0 Submission July 2004 C. Razzell, PhilipsSlide 4 Example APD plot (for Guassian Noise) Amplitude (A) in dB is plotted as the Ordinate 1-CDF(A) is plotted as the Abscissa Plotting the natural log of the probabilities on a log scale provides scaling similar to Rayleigh graph paper. P(A>10dB) = exp(-10) = 4.54x10 -5 ; P(A>-30dB) = exp(-0.001) = 0.999

doc.: IEEE /0326r0 Submission July 2004 C. Razzell, PhilipsSlide 5 APD plots for continuous OFDM signals as bandwidth is varied. As the number of sub-carriers used increases, the approximation to the AWGN APD plot improves. This can be expected due to the Central Limit Theorem.

doc.: IEEE /0326r0 Submission July 2004 C. Razzell, PhilipsSlide 6 Simulated APD plots for continuous and 3-band OFDM, using 128 sub-carriers Signal/interferer is normalized to unit power 0dBW. Probability of noise amplitude exceeding signal amplitude is given by abscissa value at the intersection of a horizontal SIR line with the APD curve. 1.8%

doc.: IEEE /0326r0 Submission July 2004 C. Razzell, PhilipsSlide 7 Simulated APD plots for continuous and 3-band OFDM, using 128 sub-carriers Comparing the same two systems at 13% probability brings them closer together. An indicative approximation of uncoded BER is sometimes taken as ~½P(A>ord.). (Depends on modulation scheme) 13%

doc.: IEEE /0326r0 Submission July 2004 C. Razzell, PhilipsSlide 8 Suggested Probability for comparing systems Suggest P(A>ord.)=1.8% Corresponding pseudo uncoded “BER” is 0.9% Any reasonable FEC should perform well under this number of input errors Region to the left of P(A>ord.)=1.8% may not be significant for digital victim receivers For AWGN this “error rate” occurs with SNR=6dB, which seems a reasonable operating point for a digital receiver.

doc.: IEEE /0326r0 Submission July 2004 C. Razzell, PhilipsSlide 9 Simulated APD Curves for OFDM and Impulse Radios in 50MHz bandwidth 10MHz PRF impulse radio has nearly identical APD to 1/3 duty cycle OFDM in region of interest. 3MHz and 1MHz PRF radios have significantly higher SIR ratios corresponding to the 1.8% P(A>ord.) line than the 3- band OFDM system. All these impulse radios would be permitted under current part 15f legislation. 1.8%

doc.: IEEE /0326r0 Submission July 2004 C. Razzell, PhilipsSlide 10 Consideration of one dominant UWB interferer is worst case analysis The above analysis assumes that the dominant source of noise/interference is a single instance of the considered waveform For this to be true: –A single interferer must be very close to the victim receiver Path loss of ~63dB, corresponds 4GHz in free space –The link margin of that receiver must allow room for the interferer overwhelm the thermal noise floor of the victim receiver This will not be true if: –The additive combination of several uncoordinated UWB interferers combines to approximate a Guassian APD (due to the CLT).

doc.: IEEE /0326r0 Submission July 2004 C. Razzell, PhilipsSlide 11 Summation of 5 MB-OFDM Signals with randomly chosen delays (50 trials)

doc.: IEEE /0326r0 Submission July 2004 C. Razzell, PhilipsSlide 12 APD plots of 1/3 duty cycle OFDM combined with thermal receiver noise

doc.: IEEE /0326r0 Submission July 2004 C. Razzell, PhilipsSlide 13 Conclusions Using the NTIA APD methodology for the worst-case scenario of a single dominant interferer shows: –That the required SIRs for impulse radios with PRFs in the 1- 10MHz range are all greater than the SIR needed for the 3-band OFDM waveform, assuming a 50MHz victim receiver bandwidth. This applies in the probability range from 1.8% to 13%, which is considered most important. –Similar conclusions apply to lower victim receiver bandwidths after applying a proportional scaling to the impulse radio PRFs. Interference caused by a population of MB-OFDM devices will have a more benign aggregate APD. Receiver thermal noise and other external interference sources will have a mitigating effect on the APD of an interfering MB-OFDM signal

BACKUP SLIDES

doc.: IEEE /0326r0 Submission July 2004 C. Razzell, PhilipsSlide 15 Appendix 1: Simulation Methodology Short MATLAB scripts were used to create all the plots The OFDM signal was created by concatenating 200 inverse FFTs, where the inputs to each IFFT were complex QPSK random sequences of length 128. To simulate 1/3 duty cycle, an all-zeros vector of length ( ) was added after each IFFT result. The resultant signal was normalized to unit power For each considered amplitude the fraction of samples in the whole sequence exceeding the level A was recorded

doc.: IEEE /0326r0 Submission July 2004 C. Razzell, PhilipsSlide 16 Simulation Methodology for Impulse Radio Random BPSK sequences of length 100 were upsampled by a factor of Fs/PRF by zero insertion A Root Raised Cosine filter of bandwidth 50MHz was use applied to the upsampled bi- polar signal After scaling the signal to unit power, the fraction of samples in the whole sequence exceeding the level A was recorded and plotted

doc.: IEEE /0326r0 Submission July 2004 C. Razzell, PhilipsSlide 17 Appendix 2: Analytic Expression for APD (I.e. 1-CDF) of OFDM waveforms

doc.: IEEE /0326r0 Submission July 2004 C. Razzell, PhilipsSlide 18 Analytic Expression for APD (I.e. 1- CDF) of OFDM waveforms

doc.: IEEE /0326r0 Submission July 2004 C. Razzell, PhilipsSlide 19 Analytically derived APD plot for MB- OFDM % APD plots d = 3*165/128; % duty cycle ratio x=linspace(-20,20); rsq=10.^(x/10); apd3=-rsq/d - log(d); apd=-rsq; semilogx(apd,x,apd3,x) xlabel('ln(P(A>ordinate))') ylabel('Amplitude [dB]') grid