thenyquistchannel · 11/29/2013  · thenyquistchannel theoptimumpulsespectrum:p opt(f)= p e 2b 0...

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The Nyquist Channel Young W. Lim November 29, 2013

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Page 1: TheNyquistChannel · 11/29/2013  · TheNyquistChannel theoptimumpulsespectrum:P opt(f)= p E 2B 0 rect(f=2B 0) theNyquistchannel: thePAMsystemwithP opt(f) I thegoalofreducingtherequriedsystembandwidth

The Nyquist Channel

Young W. Lim

November 29, 2013

Page 2: TheNyquistChannel · 11/29/2013  · TheNyquistChannel theoptimumpulsespectrum:P opt(f)= p E 2B 0 rect(f=2B 0) theNyquistchannel: thePAMsystemwithP opt(f) I thegoalofreducingtherequriedsystembandwidth

Copyright (c) 2011-2013 Young W. Lim. Permission is granted to copy, distribute and/or modify this document under the termsof the GNU Free Documentation License, Version 1.2 or any later version published by the Free Software Foundation; with noInvariant Sections, no Front-Cover Texts, and no Back-Cover Texts. A copy of the license is included in the section entitled "GNUFree Documentation License".

Page 3: TheNyquistChannel · 11/29/2013  · TheNyquistChannel theoptimumpulsespectrum:P opt(f)= p E 2B 0 rect(f=2B 0) theNyquistchannel: thePAMsystemwithP opt(f) I thegoalofreducingtherequriedsystembandwidth

The ISI Problem

the overall pulse spectrum P(f )

the optimum solution for the pulse shapingI zero intersymbol interferenceI minimum transmission bandwidth possible

yi = aip0 +∞

∑k=−∞

k 6=i

akpi−k i = 0,±1,±2, · · ·

T b

a[i] p [i] y [i]

y [i]=∑k

a [k]p [i−k]

T b

Discrete LTI System

Page 4: TheNyquistChannel · 11/29/2013  · TheNyquistChannel theoptimumpulsespectrum:P opt(f)= p E 2B 0 rect(f=2B 0) theNyquistchannel: thePAMsystemwithP opt(f) I thegoalofreducingtherequriedsystembandwidth

Zero ISI Condition

yi = aip0+∞

∑k=−∞

k 6=i

akpi−k i = 0,±1,±2, · · ·

yi = aip0 for all i ⇐⇒

p0 =√

E for i = 0,pi =0 for all i 6= 0

T b 2T b−T b−2T b

√E

p [i ]

Page 5: TheNyquistChannel · 11/29/2013  · TheNyquistChannel theoptimumpulsespectrum:P opt(f)= p E 2B 0 rect(f=2B 0) theNyquistchannel: thePAMsystemwithP opt(f) I thegoalofreducingtherequriedsystembandwidth

To Find the Optimum Pulse Shape popt(t)

yi =√

Eai for all i ⇐⇒

p0 =√

E for i = 0,pi =0 for all i 6= 0

pi = p(iTb) =⇒ popt(t) =?

I the sampling rate is equal to the bit rate R = 1/TbI the bandlimited pulse p(t) for the interval −B0 < f < +B0

interpolate pi = p(iTb) keeping the bandwidthB0as small as possibleBut the Nyquist sampling theorem gives

I the minimum sampling rate in terms of a signal’s bandwidth

Page 6: TheNyquistChannel · 11/29/2013  · TheNyquistChannel theoptimumpulsespectrum:P opt(f)= p E 2B 0 rect(f=2B 0) theNyquistchannel: thePAMsystemwithP opt(f) I thegoalofreducingtherequriedsystembandwidth

Interpolation

Interpolation Formula: strictly bandlimited signal g(t), bandwidth W

g(t) =∞

∑n=−∞

g( n2W )sinc(2W t−n)

reconstructing the original signal g(t)from the sequence of sample values {g(n/2W )}the sinc function sinc(2W t): an interpolation function

pi = p(iTb) : sampling p(t) at a uniform bit rate R = 1/Tb

the pulse shape p(t) in terms of its sample values

p(t) =∞

∑i=−∞

p(

i2B0

)sinc(2B0t− i)

Page 7: TheNyquistChannel · 11/29/2013  · TheNyquistChannel theoptimumpulsespectrum:P opt(f)= p E 2B 0 rect(f=2B 0) theNyquistchannel: thePAMsystemwithP opt(f) I thegoalofreducingtherequriedsystembandwidth

The Optimum Pulse Shape popt(t) - Zero ISI

The interpolated pulse shape

p(t) =∞

∑i=−∞

p(

i2B0

)sinc(2B0t− i)

Substitute the following equations for zero ISII p0 =

√E for i = 0,

I pi =0 for all i 6= 0

p(t) = p(

02B0

)sinc(2B0t−0)

popt(t) =√

Esinc(2B0t) =√

Esin(2πB0t)2πB0T

Page 8: TheNyquistChannel · 11/29/2013  · TheNyquistChannel theoptimumpulsespectrum:P opt(f)= p E 2B 0 rect(f=2B 0) theNyquistchannel: thePAMsystemwithP opt(f) I thegoalofreducingtherequriedsystembandwidth

The Optimum Pulse Shape popt(t) - Minimum Bandwidth

popt(t) =√

Esinc(2B0t) =√

Esin(2πB0t)2πB0T

when transmitting symbols via the bandlimited baseband channelI the maximum frequency that is allowed by the channel : B0I the upper bound for the bit rate R = 1/Tb is obtained byI 1

21

Tb≤ Bo : the bandwidth, the half of the bit rate 1/Tb

I the lower bound for the required bandwidthI bandwidth ≥ Nyquitst Bandwidth B0 = 1

2R

T s T s T s T s

f =1

2T s

f >1

2T s

Page 9: TheNyquistChannel · 11/29/2013  · TheNyquistChannel theoptimumpulsespectrum:P opt(f)= p E 2B 0 rect(f=2B 0) theNyquistchannel: thePAMsystemwithP opt(f) I thegoalofreducingtherequriedsystembandwidth

The Optimum Pulse Spectrum

the optimum pulse shape function and spectrum

popt(t) =√

Esinc(2B0t) =√

Esin(2πB0t)2πB0T

P(f ) =√

E2B0

for −B0 < f < +B0,P(f ) = 0 otherwise

B0 the minimum transmission bandwidthI a brick-wall function (a rectangular function)

√Erect(f /2B0)

I no frequencies fo absolute value exceeding half the bit rateI bandwdith=⇒ B0 = 1

2R = 12Tb

I if rect(t/Tb) pulse is used, its spectrum becomes Tbsinc(f Tb)I the first zero crossing of Tbsinc(f Tb) : 1/Tb = RI bandwdith=⇒ B = R = 1

Tb

zero intersymbol interference

Page 10: TheNyquistChannel · 11/29/2013  · TheNyquistChannel theoptimumpulsespectrum:P opt(f)= p E 2B 0 rect(f=2B 0) theNyquistchannel: thePAMsystemwithP opt(f) I thegoalofreducingtherequriedsystembandwidth

The Nyquist Channel

the optimum pulse spectrum :Popt(f ) =√

E2B0

rect(f /2B0)

the Nyquist channel : the PAM system with Popt(f )

I the goal of reducing the requried system bandwidthI the channel with the minimum bandwidthI bandwidth ≥ Nyquitst Bandwidth B0 = 1

2Tb

the optimum pluse shape : popt(t) =√

Esinc(2B0t) =√

Esin(2πB0t)2πB0T

the impulse response popt(t) of the ideal low pass filter Popt(f )

I zero crossigns at k/2B0 = kTbI shifted pulses of popt(t−kTb) has no effect at zero crossingsI zero ISI

Page 11: TheNyquistChannel · 11/29/2013  · TheNyquistChannel theoptimumpulsespectrum:P opt(f)= p E 2B 0 rect(f=2B 0) theNyquistchannel: thePAMsystemwithP opt(f) I thegoalofreducingtherequriedsystembandwidth

The Problems in The Nyquist Channel

the optimum pulse spectrum :Popt(f ) =√

E2B0

rect(f /2B0)

P(f ) is flat from −B0and +B0and zero elsewherephysically unrealizable (the abrupt transitions at ±B0)

the optimum pluse shape : popt(t) =√

Esinc(2B0t) =√

Esin(2πB0t)2πB0t

p(t) decreases as 1/|t| for large |t|relatively decays slowly (related to the abrupt transition at ±B0)no margin error in sampling times in the receiver

Page 12: TheNyquistChannel · 11/29/2013  · TheNyquistChannel theoptimumpulsespectrum:P opt(f)= p E 2B 0 rect(f=2B 0) theNyquistchannel: thePAMsystemwithP opt(f) I thegoalofreducingtherequriedsystembandwidth

Nyquist Rate - Definition 1

upper bound for the symbol rate in the bandlimited channelgiven a bandwidth B0

Bandlimited Channel

H ( f )B0 Hz

×

×

maxfreq

R≤ 2B0

Symbol Rate

bandwidth ≥ Nyquitst Bandwidth B0 = 12R = 1

2Tb

given a symbol rate R

Page 13: TheNyquistChannel · 11/29/2013  · TheNyquistChannel theoptimumpulsespectrum:P opt(f)= p E 2B 0 rect(f=2B 0) theNyquistchannel: thePAMsystemwithP opt(f) I thegoalofreducingtherequriedsystembandwidth

Nyquist Rate - Definition 2

lower bound for the sampling rate in the bandlimited signalgiven a bandwidth B0

B0 Hz

samplingBandlimited Signal

reconstructing R≥ 2B0

Sampling Rate

sampling frequency ≥ Nyquist Rate = 2B0

sampling period ≤ Nyquist Interval = 1/2B0

Page 14: TheNyquistChannel · 11/29/2013  · TheNyquistChannel theoptimumpulsespectrum:P opt(f)= p E 2B 0 rect(f=2B 0) theNyquistchannel: thePAMsystemwithP opt(f) I thegoalofreducingtherequriedsystembandwidth

Reference

[1] S. Haykin, M Moher, “Introduction to Analog and DigitalCommunications”, 2ed