section 3 1 digital mod tech v7
TRANSCRIPT
8/4/2019 Section 3 1 Digital Mod Tech v7
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Digital modulation techniquesSignal Space Analysis
Receiver Structure and Sufficient StatisticsError Probability Analysis and the Union Bound
Passband modulation
Chapter 3: Physical-layer transmission techniques
Section 3.1: Digital modulations
Mobile communications - Chapter 3: Physical-layer transmissions Section 3.1: Digital modulations 1
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Digital modulation techniquesSignal Space Analysis
Receiver Structure and Sufficient StatisticsError Probability Analysis and the Union Bound
Passband modulation
Advantages over analog modulationMain considerations in digital modulation techniquesTypical types of digital modulation techniques
Advantages over analog modulation
The advances over the last several decades in hardware anddigital signal processing have made digital transceivers muchcheaper, faster, and more power-efficient than analogtransceivers.
More importantly, digital modulation offers a number of otheradvantages over analog modulation, including:
higher data rates,powerful error correction techniques,resistance to channel impairments,
more efficient multiple access strategies, andbetter security and privacy.
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Digital modulation techniquesSignal Space Analysis
Receiver Structure and Sufficient StatisticsError Probability Analysis and the Union Bound
Passband modulation
Advantages over analog modulationMain considerations in digital modulation techniquesTypical types of digital modulation techniques
Advantages over analog modulation (cont.)
Digital transmissions consist of transferring information in theform of bits over a communications channel.
The bits are binary digits taking on the values of either 1 or 0.These information bits are derived from the informationsource, which may be a digital source or an analog source thathas been passed through an A/D converter.
Both digital and A/D converted analog sources may becompressed to obtain the information bit sequence.
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Digital modulation techniquesSignal Space Analysis
Receiver Structure and Sufficient StatisticsError Probability Analysis and the Union Bound
Passband modulation
Advantages over analog modulationMain considerations in digital modulation techniquesTypical types of digital modulation techniques
Main considerations in digital modulation techniques
Digital modulation consists of mapping the information bitsinto an analog signal for transmission over the channel.
Detection consists of determining the original bit sequencebased on the signal received over the channel.
The main considerations in choosing a particular digitalmodulation technique are:
high data ratehigh spectral efficiency (minimum bandwidth occupancy)high power efficiency (minimum required transmit power)robustness to channel impairments (minimum probability of biterror)low power/cost implementation
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Di i l d l i h i
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Digital modulation techniquesSignal Space Analysis
Receiver Structure and Sufficient StatisticsError Probability Analysis and the Union Bound
Passband modulation
Advantages over analog modulationMain considerations in digital modulation techniquesTypical types of digital modulation techniques
Typical types of digital modulation techniques
Often the previous ones are conflicting requirements, and thechoice of modulation is based on finding the technique thatachieves the best tradeoff between these requirements.
There are two main categories of digital modulation:
amplitude/phase modulationfrequency modulation
Frequency modulation typically has a constant signal envelopeand is generated using nonlinear techniques, this modulation
is also called constant envelope modulation or nonlinearmodulation
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Di it l d l ti t h i
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Digital modulation techniquesSignal Space Analysis
Receiver Structure and Sufficient StatisticsError Probability Analysis and the Union Bound
Passband modulation
Advantages over analog modulationMain considerations in digital modulation techniquesTypical types of digital modulation techniques
Typical types of digital modulation techniques (cont.)
Amplitude/phase modulation is also called linear modulation.
Linear modulation generally has better spectral propertiesthan nonlinear modulation, since nonlinear processing leads tospectral broadening.
However, amplitude and phase modulation embeds theinformation bits into the amplitude or phase of thetransmitted signal, which is more susceptible to variationsfrom fading and interference.
Mobile communications - Chapter 3: Physical-layer transmissions Section 3.1: Digital modulations 6
Digital modulation techniques
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Digital modulation techniquesSignal Space Analysis
Receiver Structure and Sufficient StatisticsError Probability Analysis and the Union Bound
Passband modulation
Advantages over analog modulationMain considerations in digital modulation techniquesTypical types of digital modulation techniques
Typical types of digital modulation techniques (cont.)
In addition, amplitude and phase modulation techniquestypically require linear amplifiers, which are more expensiveand less power efficient than the nonlinear amplifiers that canbe used with nonlinear modulation.
Thus, the general tradeoff of linear versus nonlinearmodulation is one of better spectral efficiency for the formertechnique and better power efficiency and resistance tochannel impairments for the latter technique.
Mobile communications - Chapter 3: Physical-layer transmissions Section 3.1: Digital modulations 7
Digital modulation techniques Rational
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Digital modulation techniquesSignal Space Analysis
Receiver Structure and Sufficient StatisticsError Probability Analysis and the Union Bound
Passband modulation
RationalSignal and system modelGeometric representation of signalsPractical examplesSignal space representation
Rational
Digital modulation encodes a bit stream of finite length intoone of several possible transmitted signals.
Intuitively, the receiver minimizes the probability of detectionerror by decoding the received signal as the signal in the set of possible transmitted signals that is closest to the one received.
Determining the distance between the transmitted andreceived signals requires a metric for the distance betweensignals.
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Digital modulation techniques Rational
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Digital modulation techniquesSignal Space Analysis
Receiver Structure and Sufficient StatisticsError Probability Analysis and the Union Bound
Passband modulation
RationalSignal and system modelGeometric representation of signalsPractical examplesSignal space representation
Rational (cont.)
By representing signals as projections onto a set of basisfunctions, we obtain a one-to-one correspondence between theset of transmitted signals and their vector representations.
Thus, we can analyze signals in finite-dimensional vectorspace instead of infinite-dimensional function space, usingclassical notions of distance for vector spaces.
In this section we show:
how digitally modulated signals can be represented as vectors
in an appropriately-defined vector space, andhow optimal demodulation methods can be obtained from thisvector space representation.
This general analysis will then be applied to specificmodulation techniques in later sections.
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Digital modulation techniques Rational
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Digital modulation techniquesSignal Space Analysis
Receiver Structure and Sufficient StatisticsError Probability Analysis and the Union Bound
Passband modulation
RationalSignal and system modelGeometric representation of signalsPractical examplesSignal space representation
Transmitted signal
Transmitter Receiver
+
n(t)
AWGN Channel
s(t)i 1 K
m ={b ,...,b } ^1 K
m ={b ,...,b }^ ^r(t)
Figure 1: Communication system model over AWGN channel (i.e., aspecial case of wireless channel).
Consider a communication system model as shown in theabove figure.
Every seconds, the sytem sends = log2 bits of information through the channel for a data rate of = / bits per second (bps).
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Digital modulation techniques Rational
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g qSignal Space Analysis
Receiver Structure and Sufficient StatisticsError Probability Analysis and the Union Bound
Passband modulation
Signal and system modelGeometric representation of signalsPractical examplesSignal space representation
Transmitted signal (cont.)
There are = 2 possible sequences of bits and each bitsequence of length comprises a message = {1,..., } ∈ , where = {1,..., } is the set of all such messages.
The message has probability of being selected fortransmission, where
=1 = 1.
Suppose that message is to be transmitted over theAWGN channel during the time interval [0, ). Since the
channel is analog, the message must be embedded into ananalog signal for channel transmission.
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Digital modulation techniques Rational
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g qSignal Space Analysis
Receiver Structure and Sufficient StatisticsError Probability Analysis and the Union Bound
Passband modulation
Signal and system modelGeometric representation of signalsPractical examplesSignal space representation
Transmitted signal (cont.)
Therefore, each message ∈ is mapped to a uniqueanalog signal () ∈ = {1(),..., ()} where () isdefined on the time interval [0, ) and has energy
= 0
2 (), = 1,...,. (1)
When messages are sent sequentially, the transmittedsignal becomes a sequence of the corresponding analog signals
as follows() =
( − ). (2)
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Digital modulation techniques Rational
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gSignal Space Analysis
Receiver Structure and Sufficient StatisticsError Probability Analysis and the Union Bound
Passband modulation
Signal and system modelGeometric representation of signalsPractical examplesSignal space representation
Transmitted and received signals
In the aforementioned model, the transmitted signal is sentthrough an AWGN channel where a white Gaussian noiseprocess () of power spectral density /2 is added to formthe received signal
() = () + (). (3)
T0 2T 3T 4T
s (t)1 1 1
2s (t−T)
s (t−2T) s (t−3T)
s(t)
...
m
1
m
1
m
1
m2
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Digital modulation techniquesS S
RationalS
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Signal Space AnalysisReceiver Structure and Sufficient Statistics
Error Probability Analysis and the Union BoundPassband modulation
Signal and system modelGeometric representation of signalsPractical examplesSignal space representation
Received signal
Given (), the receiver must determine the best estimate of which () ∈ was transmitted during each transmissioninterval [0, ).
This best estimate of () is mapped to a best estimate of
the message () ∈ and the receiver produces this best
estimate = 1,..., of the transmitted bit sequence.
The goal of the receiver design in estimating the transmittedmessage is to minimize the probability of message error
= =1
( ∕= ∣ sent) ( sent) (4)
over each time interval [0, ).
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Digital modulation techniquesSi l S A l i
RationalSi l d d l
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Signal Space AnalysisReceiver Structure and Sufficient Statistics
Error Probability Analysis and the Union BoundPassband modulation
Signal and system modelGeometric representation of signalsPractical examplesSignal space representation
Introduction
By representing the signals {(), = 1,..., } geometrically,one can solve for the optimal receiver design in AWGNchannels based on a minimum distance criterion.
Note that, wireless channels typically have a time-varying
impulse response in addition to AWGN. We will consider theeffect of an arbitrary channel impulse response on digitalmodulation performance in the next sections.
The basic premise behind a geometrical representation of
signals is the notion of a basis set.
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Digital modulation techniquesSi l S A l sis
RationalSi l d s st d l
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Signal Space AnalysisReceiver Structure and Sufficient Statistics
Error Probability Analysis and the Union BoundPassband modulation
Signal and system modelGeometric representation of signalsPractical examplesSignal space representation
Basis function representation of signals
Specifically, using a Gram-Schmidt orthogonalizationprocedure, it can be shown that any set of real energysignals = {1(),..., ()} defined on [0, ) can berepresented as a linear combination of
≤ real
orthogonal basis functions {1(),..., ()}.We say that these basis functions span the set .Each signal {() ∈ } can be represented by
() =
=1 , (), 0≤
< , (5)
where
, =
0
() () (6)
is a real coefficient representing the pro jection.Mobile communications - Chapter 3: Physical-layer transmissions Section 3.1: Digital modulations 16
Digital modulation techniquesSignal Space Analysis
RationalSignal and system model
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Signal Space AnalysisReceiver Structure and Sufficient Statistics
Error Probability Analysis and the Union BoundPassband modulation
Signal and system modelGeometric representation of signalsPractical examplesSignal space representation
Basis function representation of signals (cont.)
These basis functions have the following property 0
() () =
1 = ,
0
∕= .
(7)
The basis set consists of the sine and cosine functions
1() =
2
cos (2 ) (8)
and
2() =
2
sin(2 ) . (9)
where 2 is used to obtain
0 2 () = 1, = 1, 2.
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Digital modulation techniquesSignal Space Analysis
RationalSignal and system model
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Signal Space AnalysisReceiver Structure and Sufficient Statistics
Error Probability Analysis and the Union BoundPassband modulation
Signal and system modelGeometric representation of signalsPractical examplesSignal space representation
Basis functions in linear passband modulation techniques
With these basis functions, one only obtain an approximationto (7), since
0
21() =
2
0
0.5 [1 + cos (4 )] = 1+sin (4 )
4 (10)
The numerator in the second term of (10) is bounded by 1,and for ≫ 1 the denominator of this term is very large.As a result, this second term can be neglected.
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Digital modulation techniquesSignal Space Analysis
RationalSignal and system model
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Signal Space AnalysisReceiver Structure and Sufficient Statistics
Error Probability Analysis and the Union BoundPassband modulation
Signal and system modelGeometric representation of signalsPractical examplesSignal space representation
Basis functions in linear passband modulation (cont.)
With these basis functions, one can have 0
1()2() =2
0
0.5sin(4 ) =− cos(4 )
4 ≈ 0
(11)where the approximation is taken as an equality as ≫ 1.
With the basis set 1() =
2/ cos (2 ) and2() =
2/ sin (2 ), the basis function representation
(5) corresponds to the complex representation of () in
terms of its in-phase and quadrature components with anextra factor of
2/ as follows
() = ,1
2
cos (2 ) + ,2
2
sin(2 ) . (12)
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Digital modulation techniquesSignal Space Analysis
RationalSignal and system model
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Signal Space AnalysisReceiver Structure and Sufficient Statistics
Error Probability Analysis and the Union BoundPassband modulation
Signal and system modelGeometric representation of signalsPractical examplesSignal space representation
Basis functions in linear passband modulation (cont.)
In practice, the basis set may include a baseband pulse-shapingfilter () to improve the spectral characteristics of the transmittedsignal:
() = ,1() cos (2 ) + ,2() sin (2 ) (13)
where the simplest pulse shape that satisfy (7) is the rectangularpulse shape () =
2/ , 0 ≤ < .
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Digital modulation techniquesSignal Space Analysis
RationalSignal and system model
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g p yReceiver Structure and Sufficient Statistics
Error Probability Analysis and the Union BoundPassband modulation
g yGeometric representation of signalsPractical examplesSignal space representation
Definitions used in signal space representation
We denote the coefficients {,} as a vectors = [,1,...,, ] ∈ ℛ which is called the signal
constellation point corresponding to the signal ().
The signal constellation consists of all constellation points
{s1, ..., s }.
Given the basis functions {1(),..., ()} there is aone-to-one correspondence between the transmitted signal() and its constellation point s.
The representation of () in terms of its constellation points ∈ ℛ is called:
its signal space representation andthe vector space containing the constellation is called thesignal space .
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Digital modulation techniquesSignal Space Analysis
RationalSignal and system model
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Receiver Structure and Sufficient StatisticsError Probability Analysis and the Union Bound
Passband modulation
Geometric representation of signalsPractical examplesSignal space representation
Definitions used in signal space representation (cont.)
A two-dimensional signal space is illustrated in the belowfigure, where we show s ∈ ℛ2 with the th axis of ℛ2
corresponding to the basis function (), = 1, 2.
=4, K=2
0011
01
10
M=8, K=3
000
001
011
110
100
010
110
101
si1
si2
si1
si2
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Digital modulation techniquesSignal Space Analysis
RationalSignal and system model
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Receiver Structure and Sufficient StatisticsError Probability Analysis and the Union Bound
Passband modulation
Geometric representation of signalsPractical examplesSignal space representation
Definitions used in signal space representation (cont.)
With this signal space representation we can analyze theinfinite-dimensional functions () as vectors s infinite-dimensional vector space ℛ2.
This greatly simplifies the analysis of the system performance
as well as the derivation of the optimal receiver design.
Signal space representations for common modulationtechniques like MPSK and MQAM are two-dimensional(corresponding to the in-phase and quadrature basis
functions).In order to analyze signals via a signal space representation,we need to use some definitions for the vector characterizationin the vector space ℛ .
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Digital modulation techniquesSignal Space Analysis
R i S d S ffi i S i i
RationalSignal and system modelG i i f i l
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Receiver Structure and Sufficient StatisticsError Probability Analysis and the Union Bound
Passband modulation
Geometric representation of signalsPractical examplesSignal space representation
Definitions used in signal space representation (cont.)
In particular, the length of a vector in ℛ is defined as
∥s∥ =
⎷
=12,. (14)
The distance between two signal constellation points s and s
is thus
∥s − s∥ = ⎷ =1
(, − ,)2 = 0
(() − ())2 .
(15)
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Digital modulation techniquesSignal Space Analysis
R i St t d S ffi i t St ti ti
RationalSignal and system modelG t i t ti f i l
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Receiver Structure and Sufficient StatisticsError Probability Analysis and the Union Bound
Passband modulation
Geometric representation of signalsPractical examplesSignal space representation
Definitions used in signal space representation (cont.)
Finally, the inner product ⟨(), ()⟩ between two realsignals () and () on the interval [0, ) is defined as
⟨(), ()
⟩=
0
()(). (16)
Similarly, the inner product ⟨s, s⟩ between two real vectors is
⟨s, s
⟩= ss =
0
()() =
⟨(), ()
⟩. (17)
It is noted that two signals are orthogonal if their innerproduct is zero.
Mobile communications - Chapter 3: Physical-layer transmissions Section 3.1: Digital modulations 25
Digital modulation techniquesSignal Space Analysis
Receiver Structure and Sufficient StatisticsGeneral resultsProofs of sufficient statistics for optimal detection
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Receiver Structure and Sufficient StatisticsError Probability Analysis and the Union Bound
Passband modulation
Proofs of sufficient statistics for optimal detectionDecision regions and criterion
Receiver structure and sufficient statistics
Given the channel output () = () + (), 0 ≤ < , wenow investigate the receiver structure to determine whichconstellation point s or, equivalently, which message , wassent over the time interval [0, ).
A similar procedure is done for each time interval[ , ( + 1) ).
We would like to convert the received signal () over eachtime interval into a vector, since it allows us to work in
finite-dimensional vector space to estimate the transmittedsignal.
However, this conversion should not compromise theestimation accuracy. For this conversion, consider the receiverstructure shown in the next figure.
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Digital modulation techniquesSignal Space Analysis
Receiver Structure and Sufficient StatisticsGeneral resultsProofs of sufficient statistics for optimal detection
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Receiver Structure and Sufficient StatisticsError Probability Analysis and the Union Bound
Passband modulation
Proofs of sufficient statistics for optimal detectionDecision regions and criterion
Receiver structure and sufficient statistics (cont.)
)()()( t nt st r i
³T
dt 0()
³
T
dt 0 ()
111, r n si
)(1 t I
)(t N
I
N N N ir n s ,
Find ii
mm ˆ
As shown in the above figure, the components of signal andnoise vectors are determined by
, = 0
() (), (18)
and
=
0
() (). (19)
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Digital modulation techniquesSignal Space Analysis
Receiver Structure and Sufficient StatisticsGeneral resultsProofs of sufficient statistics for optimal detection
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Receiver Structure and Sufficient StatisticsError Probability Analysis and the Union Bound
Passband modulation
Proofs of sufficient statistics for optimal detectionDecision regions and criterion
Receiver structure and sufficient statistics (cont.)
We can rewrite () as
() =
=1(, + ) () + () =
=1 () + (),
(20)where = , + and () = () −
=1 ()denotes the remainder noise.
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Digital modulation techniquesSignal Space Analysis
Receiver Structure and Sufficient StatisticsGeneral resultsProofs of sufficient statistics for optimal detection
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Receiver Structure and Sufficient StatisticsError Probability Analysis and the Union Bound
Passband modulation
Proofs of sufficient statistics for optimal detectionDecision regions and criterion
Proofs of sufficient statistics for optimal detection
If we can show that the optimal detection of the transmittedsignal constellation point s given received signal () does notmake use of the remainder noise (), then the receiver canmake its estimate of the transmitted message as afunction of r = (1,..., ) alone.
In other words, r = (1,..., ) is a sufficient statistic for ()in the optimal detection of the transmitted messages.
Let exam the distribution of r. Since () is a Gaussian
random process, if we condition on the transmitted signal() then the channel output () = () + () is also aGaussian random process and r = [1,..., ] is a Gaussianrandom vector.
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Digital modulation techniquesSignal Space Analysis
Receiver Structure and Sufficient StatisticsGeneral resultsProofs of sufficient statistics for optimal detection
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Error Probability Analysis and the Union BoundPassband modulation
pDecision regions and criterion
Proofs of sufficient statistics for optimal detection (cont.)
Recall that = , + . Thus, conditioned on thetransmitted constellation s, we have
∣s = [ ∣s] = [, + ∣,] = , (21)
since n(t) has zero mean, and
∣s =
− ∣s2
= [, + − ,∣,]2 =
2
.
(22)
With Cov [
∣s
] =
− ( −
)∣s
= [
]and some manipulations, one can have
[ ] = 02
0
()() =
0/2 =
0 ∕= .. (23)
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Digital modulation techniquesSignal Space Analysis
Receiver Structure and Sufficient StatisticsGeneral resultsProofs of sufficient statistics for optimal detection
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Error Probability Analysis and the Union BoundPassband modulation
pDecision regions and criterion
Proofs of sufficient statistics for optimal detection (cont.)
Thus, conditioned on the transmitted constellation s, the ’sare uncorrelated and, since they are Gaussian and also
independent. Moreover,
2
= 0/2.
We have shown that, conditioned on the transmittedconstellation s, is a Gauss-distributed random variable thatis independent of , ∕= and has mean , and variance 0/2.
Thus, the conditional distribution of r is given by
(r∣s sent) =
=1
( ∣) =1
( 0)/2
exp
⎡⎣− 1
0
=1
( − ,)2
⎤⎦ .
(24)
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Digital modulation techniquesSignal Space Analysis
Receiver Structure and Sufficient StatisticsGeneral resultsProofs of sufficient statistics for optimal detection
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Error Probability Analysis and the Union BoundPassband modulation
Decision regions and criterion
Proofs of sufficient statistics for optimal detection (cont.)
It is also straightforward to show that [ ()∣s] = 0 forany , 0 ≤ < . Thus, since conditioned on s and ()are Gaussian and uncorrelated, they are independent.
Also, since the transmitted signal is independent of the noise,, is independent of the process ().
We now discuss the receiver design criterion and show it is notaffected by discarding ().
The goal of the receiver design is to minimize the probability
of error in detecting the transmitted message givenreceived signal ().
To minimize = (
∕= ∣()) = 1 − (
= ∣()), we
maximize (
= ∣()).
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Digital modulation techniquesSignal Space AnalysisReceiver Structure and Sufficient Statistics
E P b bili A l i d h U i B d
General resultsProofs of sufficient statistics for optimal detectionD i i i d i i
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Error Probability Analysis and the Union BoundPassband modulation
Decision regions and criterion
Proofs of sufficient statistics for optimal detection (cont.)
Therefore, the receiver output
given received signal ()
should correspond to the message that maximizes ( sent∣()).
Since there is a one-to-one mapping between messages andsignal constellation points, this is equivalent to maximizing ( sent
∣()).
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Digital modulation techniquesSignal Space AnalysisReceiver Structure and Sufficient Statistics
E P b bilit A l i d th U i B d
General resultsProofs of sufficient statistics for optimal detectionD i i i d it i
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Error Probability Analysis and the Union BoundPassband modulation
Decision regions and criterion
Proofs of sufficient statistics for optimal detection (cont.)
Recalling that () is completely described by = (1,..., )and (), we have
(s sent
∣()) = ((,1,...,, ) sent
∣(1,..., , ()))
= ((,1,...,, ) sent, (1,..., ), ())
((1,..., ), ())
= ((,1,...,, ) sent, (1,..., )) (())
((1,..., )) (())
= ((,1,...,, ) sent∣(1,..., )) . (25)
where the third equality follows from the fact that the () isindependent of both (1,..., ) and of (,1,...,, ).
Mobile communications - Chapter 3: Physical-layer transmissions Section 3.1: Digital modulations 34
Digital modulation techniquesSignal Space AnalysisReceiver Structure and Sufficient Statistics
Error Probabilit Anal sis and the Union Bo nd
General resultsProofs of sufficient statistics for optimal detectionDecision regions and criterion
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Error Probability Analysis and the Union BoundPassband modulation
Decision regions and criterion
Proofs of sufficient statistics for optimal detection (cont.)
This analysis shows that (1,..., ) is a sufficient statistic for
() in detecting , in the sense that the probability of erroris minimized by using only this sufficient statistic to estimatethe transmitted signal and discarding the remainder noise.
Since r is a sufficient statistic for the received signal (), wecall r the received vector associated with ().
Mobile communications - Chapter 3: Physical-layer transmissions Section 3.1: Digital modulations 35
Digital modulation techniquesSignal Space AnalysisReceiver Structure and Sufficient Statistics
Error Probability Analysis and the Union Bound
General resultsProofs of sufficient statistics for optimal detectionDecision regions and criterion
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Error Probability Analysis and the Union BoundPassband modulation
Decision regions and criterion
Decision regions
As aforementioned, the optimal receiver minimizes errorprobability by selecting the detector output
that maximizes
the probability of correct detection
1 − = ( sent∣r received).In other words, given a received vector r, the optimal receiverselects
= corresponding to the constellation s that
satisfies (s∣r) > (s
∣r) ,
∀
∕= (26)
where (s∣r) ≜ (s sent∣r received) for the sake of notational simplicity.
Mobile communications - Chapter 3: Physical-layer transmissions Section 3.1: Digital modulations 36
Digital modulation techniquesSignal Space AnalysisReceiver Structure and Sufficient Statistics
Error Probability Analysis and the Union Bound
General resultsProofs of sufficient statistics for optimal detectionDecision regions and criterion
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Error Probability Analysis and the Union BoundPassband modulation
Decision regions and criterion
Decision regions(cont.)
Thus, the decision regions ( 1,..., ) corresponding to(s1, ...,s ) are the subsets of the signal space ℛ anddefined by
= (r : (s∣r) > (s ∣r) , ∀ ∕= ) . (27)
Once the signal space has been partitioned by decisionregions, for a received vector r ∈ , the optimal receiveroutputs the message estimate =
The receiver processing consists of ) computing the receivedvector r from (), ) finding which decision region contains r, and ) outputting the corresponding message .
Mobile communications - Chapter 3: Physical-layer transmissions Section 3.1: Digital modulations 37
Digital modulation techniquesSignal Space AnalysisReceiver Structure and Sufficient Statistics
Error Probability Analysis and the Union Bound
General resultsProofs of sufficient statistics for optimal detectionDecision regions and criterion
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Error Probability Analysis and the Union BoundPassband modulation
Decision regions and criterion
An example on decision regions
This process is illustrated in the below figure, that shows atwo-dimensional signal space with four decision regions 1,..., 4 corresponding to four constellations s1, ..., s4.The received vector r lies in region 1, so the receiver willoutput the message
1as the best message estimate given
received vector r.
φ (t)1
φ (t)2
s
s
s
s1
2
3
4
1
ZZ3
Z2
Z4
x
Mobile communications - Chapter 3: Physical-layer transmissions Section 3.1: Digital modulations 38
Digital modulation techniquesSignal Space AnalysisReceiver Structure and Sufficient Statistics
Error Probability Analysis and the Union Bound
General resultsProofs of sufficient statistics for optimal detectionDecision regions and criterion
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o obab ty a ys s a d t e U o ou dPassband modulation
ec s o eg o s a d c te o
Decision criterion
Using Bayes rule, one can have
(s∣r) = (r∣s) (s)
(r). (28)
To minimize error probability, the receiver output = corresponds to the constellation point s that maximizes (s∣r), i.e., the detected transmitted constellation point scan be determined by
s = arg maxs
(r∣s) (s) (r)
= arg maxs
(r∣s) (s) , = 1,...,
(29)where the second equality follows from the fact that (r) isnot a function of s
Mobile communications - Chapter 3: Physical-layer transmissions Section 3.1: Digital modulations 39
Digital modulation techniquesSignal Space AnalysisReceiver Structure and Sufficient Statistics
Error Probability Analysis and the Union Bound
General resultsProofs of sufficient statistics for optimal detectionDecision regions and criterion
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y yPassband modulation
g
Decision criterion (cont.)
Assuming that transmitted messages are equally likely(i.e., (s) = 1/ ), (29) becomes
s = arg maxs
(r∣s) , = 1,...,. (30)
Let define the likelihood function associated with the receiveras
(s) = (r∣s) . (31)
Given a received vector r, a maximum likelihood (ML)receiver outputs = corresponding to the constellationpoint s that maximizes (s).
Mobile communications - Chapter 3: Physical-layer transmissions Section 3.1: Digital modulations 40
Digital modulation techniquesSignal Space AnalysisReceiver Structure and Sufficient Statistics
Error Probability Analysis and the Union Bound
General resultsProofs of sufficient statistics for optimal detectionDecision regions and criterion
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Passband modulation
Decision criterion (cont.)
Since the log function is increasing in its argument,maximizing s is equivalent to maximizing the log likelihoodfunction, defined as (s) = log (s). Using (24) for (s) = log (s) yields
(s) = − 1
0
=1
( − ,)2
+constant = − 1
0∥r− s∥2+constant.
(32)
Based on (30), the detected transmitted constellation point s can
be determined by the ML criterion as
s = arg mins
∥r− s∥2 , = 1,...,. (33)
Mobile communications - Chapter 3: Physical-layer transmissions Section 3.1: Digital modulations 41
Digital modulation techniquesSignal Space AnalysisReceiver Structure and Sufficient Statistics
Error Probability Analysis and the Union Bound
General resultsProofs of sufficient statistics for optimal detectionDecision regions and criterion
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Passband modulation
Decision criterion (cont.)
Under the aforementioned assumption of equiprobable
(transmitted) messages , the ML structure minimizes theprobability of detection error at the receiver.
Under the aforementioned assumption of equiprobable(transmitted) messages , the ML structure minimizes theprobability of detection error at the receiver.
Mobile communications - Chapter 3: Physical-layer transmissions Section 3.1: Digital modulations 42
Digital modulation techniquesSignal Space AnalysisReceiver Structure and Sufficient Statistics
Error Probability Analysis and the Union BoundP b d d l i
Error probabilityThe union bound on error probability
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Passband modulation
Error probability of ML detection
With ( sent) = 1/ , the error probability of the ML receiver:
s1
s
s
s
s
s
s
s
2
3
4
5
6
7
8
0
1Z
1
dmin
r=s +n
=
=1
(r /∈ ∣ sent) ( sent)
= 1
=1
(r /∈ ∣ sent)
= 1 − 1
=1
(r ∈ ∣ sent)
= 1 − 1
=1
(r∣) r
= 1 − 1
=1
(r = s + n∣s) r
Mobile communications - Chapter 3: Physical-layer transmissions Section 3.1: Digital modulations 43
Digital modulation techniquesSignal Space AnalysisReceiver Structure and Sufficient Statistics
Error Probability Analysis and the Union BoundP b d d l ti
Error probabilityThe union bound on error probability
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Passband modulation
The union bound on error probability
As observed, (34) gives an exact solution to the errorprobability but it is impossible to solve this error probability inclosed-form. Therefore, the union bound on error probabilityis investigated.
Let , denote the event that ∥r − s∥ < ∥r − s∥ given thatthe constellation point s was sent.
If the event , occurs, then the constellation point will bedecoded in error since the transmitted constellation point s is
not the closest constellation point to the received vector r.However, event , does not necessarily imply that s will bedecoded instead of s, since there may be anotherconstellation point s with ∥r− s∥ < ∥r − s∥ < ∥r − s∥.
Mobile communications - Chapter 3: Physical-layer transmissions Section 3.1: Digital modulations 44
Digital modulation techniquesSignal Space AnalysisReceiver Structure and Sufficient Statistics
Error Probability Analysis and the Union BoundPassband modulation
Error probabilityThe union bound on error probability
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Passband modulation
The union bound on error probability (cont.)
The constellation point is decoded correctly if ∥r − s∥ < ∥r − s∥ ∀ ∕= . Therefore,
( sent) =
⎛⎜⎜⎝
=1∕=
,
⎞⎟⎟⎠ ≤
=1∕=
(,) . (35)
where the inequality follows from the union bound onprobability.More specifically, (,) can be determined by
(,) = (∥s − r∥ < ∥s − r∥ ∣ sent)
= (∥s − (s + n)∥ < ∥s − (s + n)∥)
= (∥n + s − s∥ < ∥n∥)
= 2
∥n
∥ ∥s
−s
∥cos <
−∥s
−s
∥2
Mobile communications - Chapter 3: Physical-layer transmissions Section 3.1: Digital modulations 45
Digital modulation techniquesSignal Space AnalysisReceiver Structure and Sufficient Statistics
Error Probability Analysis and the Union BoundPassband modulation
Error probabilityThe union bound on error probability
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Passband modulation
The union bound on error probability (cont.)
Since ⟨n, s − s⟩ = ∥n∥ ∥s − s∥ cos , one will have
= ∥n∥ cos = ⟨n,s−s⟩∥s−s∥ is a Gaussian random variable with
zero-mean and variance 0/2
As a result, (,) can be simplified to
(,) =
< −∥s − s∥
2
=
>
,2
= ∞,/2
1√ 0
exp−2
0 = ,√
2 0 .
Mobile communications - Chapter 3: Physical-layer transmissions Section 3.1: Digital modulations 46
Digital modulation techniquesSignal Space AnalysisReceiver Structure and Sufficient Statistics
Error Probability Analysis and the Union BoundPassband modulation
Error probabilityThe union bound on error probability
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Passband modulation
The union bound on error probability (cont.)
Substituting (36) into (35), one can have
( sent) ≤ =1∕=
,√2 0
. (36)
where the function, (), is defined as the probability thata Gaussian random variable with zero-mean and variance of 1 is bigger than , i.e.,
() = ( > ) = ∞
1√2
exp−2
2 . (37)
Summing (36) over all possible messages yields the union bound
=
=1
() ( sent) ≤ 1
=1
=1∕=
,√2 0
. (38)
Mobile communications - Chapter 3: Physical-layer transmissions Section 3.1: Digital modulations 47
Digital modulation techniquesSignal Space AnalysisReceiver Structure and Sufficient Statistics
Error Probability Analysis and the Union BoundPassband modulation
Error probabilityThe union bound on error probability
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Passband modulation
The union bound on error probability (cont.)
Note that the function cannot be solved in closed-form. Itcan be obtained from the complementary error function as
() = 12erfc
√ 2
.
One can upper bound () with the closed-form expression
() ≤ 1
√
2exp
−2/2
. (39)
and this bound is quite tight for ≫ 0.
Let define the minimum distance of the constellation as = min, ,, one can simplify (41) with looser bound
≤ ( − 1)
√
2 0
. (40)
Mobile communications - Chapter 3: Physical-layer transmissions Section 3.1: Digital modulations 48
Digital modulation techniquesSignal Space Analysis
Receiver Structure and Sufficient StatisticsError Probability Analysis and the Union Bound
Passband modulation
Error probabilityThe union bound on error probability
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The union bound on error probability (cont.)
Using (39) for the function yields a closed-form bound
≤
− 1
√
exp−2
4 0 . (41)
Note that for binary modulation ( = 2), there is only oneway to make an error and is the distance between thetwo signal constellation points, so the bound is exact
= √
2 0
. (42)
Mobile communications - Chapter 3: Physical-layer transmissions Section 3.1: Digital modulations 49
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Digital modulation techniquesSignal Space Analysis
Receiver Structure and Sufficient StatisticsError Probability Analysis and the Union Bound
Passband modulation
Error probabilityThe union bound on error probability
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Bit error rate (cont.)
With such a mapping, assuming that mistaking a signalconstellation for a constellation other than its nearestneighbors has a very low probability, we can make theapproximation
≈ 2
. (43)
The most common form of mapping with the property iscalled Gray coding, which will be discussed in more detail.
Signal space concepts are applicable to any modulation wherebits are encoded as one of several possible analog signals,including the amplitude, phase, and frequency modulations asdiscussed later.
Mobile communications - Chapter 3: Physical-layer transmissions Section 3.1: Digital modulations 51
Digital modulation techniquesSignal Space Analysis
Receiver Structure and Sufficient StatisticsError Probability Analysis and the Union Bound
Passband modulation
General principlesAmplitude and phase modulationPulse amplitude modulation (MPAM)Phase shift keying (MPSK)Quadrature amplitude modulation (MQAM)
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General principles
The basic principle of passband digital modulation is toencode an information bit stream into a carrier signal which isthen transmitted over a communications channel.
Demodulation is the process of extracting this information bit
stream from the received signal. Corruption of the transmittedsignal by the channel can lead to bit errors in thedemodulation process.
The goal of modulation is to send bits at a high data rate
while minimizing the probability of data corruption.In general, modulated carrier signals encode information in theamplitude (), frequency (), or phase () of a carriersignal.
Mobile communications - Chapter 3: Physical-layer transmissions Section 3.1: Digital modulations 52
Digital modulation techniquesSignal Space Analysis
Receiver Structure and Sufficient StatisticsError Probability Analysis and the Union Bound
Passband modulation
General principlesAmplitude and phase modulationPulse amplitude modulation (MPAM)Phase shift keying (MPSK)Quadrature amplitude modulation (MQAM)
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General principles (cont.)
Thus, the modulated signal can be represented as
() = ()cos[2 ( + ()) + () + 0] = ()cos[2 + () + 0]
where () = 2 () + () and 0 is the phase offset of the
carrier. This representation combines frequency and phasemodulation into angle modulation.
One can rewrite the right-hand side of (44) in terms of its in-phaseand quadrature components as:
() = ()cos ()cos[2 ] − ()sin ()sin[2 ]= ()cos[2 ] − ()sin[2 ] (44)
where () = ()cos () is called the in-phase component of ()and () = ()sin () is called its quadrature component.
Mobile communications - Chapter 3: Physical-layer transmissions Section 3.1: Digital modulations 53
Digital modulation techniquesSignal Space Analysis
Receiver Structure and Sufficient StatisticsError Probability Analysis and the Union Bound
Passband modulation
General principlesAmplitude and phase modulationPulse amplitude modulation (MPAM)Phase shift keying (MPSK)Quadrature amplitude modulation (MQAM)
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General principles (cont.)
We can write () in its complex baseband representation as
() = Re () 2 (45)
where () = () + ().
This representation is useful since receivers typically processthe in-phase and quadrature signal components separately.
Mobile communications - Chapter 3: Physical-layer transmissions Section 3.1: Digital modulations 54
Digital modulation techniquesSignal Space Analysis
Receiver Structure and Sufficient StatisticsError Probability Analysis and the Union Bound
Passband modulation
General principlesAmplitude and phase modulationPulse amplitude modulation (MPAM)Phase shift keying (MPSK)Quadrature amplitude modulation (MQAM)
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Amplitude and phase modulation
In amplitude and phase modulation the information bit streamis encoded in the amplitude and/or phase of the transmittedsignal.
Specifically, over a time interval of , = log2 bits are
encoded into the amplitude and/or phase of the transmittedsignal (), 0 ≤ < .
The transmitted signal over this period() = ()cos[2 ] − ()sin[2 ] can be written interms of its signal space representation as
() = ,11() + ,22() (46)
where basis functions 1() = ()cos(2 + 0) and2() = −()sin(2 + 0), where () is a shaping pulse.
Mobile communications - Chapter 3: Physical-layer transmissions Section 3.1: Digital modulations 55
Digital modulation techniquesSignal Space Analysis
Receiver Structure and Sufficient StatisticsError Probability Analysis and the Union Bound
Passband modulation
General principlesAmplitude and phase modulationPulse amplitude modulation (MPAM)Phase shift keying (MPSK)Quadrature amplitude modulation (MQAM)
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Amplitude and phase modulation (cont.)
To send the th message over the time interval [ , ( + 1) ),we set () = ,1() and () = ,2(). These in-phaseand quadrature signal components are baseband signals withspectral characteristics determined by the pulse shape ().
In particular, their bandwidth equals the bandwidth of g(t),and the transmitted signal () is a passband signal withcenter frequency fc and passband bandwidth 2.
In practice we take = / where depends on the
pulse shape: for rectangular pulses = .5 and for raisedcosine pulses .5 ≤ ≤ 1.
Thus, for rectangular pulses the bandwidth of () is .5/ and the bandwidth of () is 1/ .
Mobile communications - Chapter 3: Physical-layer transmissions Section 3.1: Digital modulations 56
Digital modulation techniquesSignal Space Analysis
Receiver Structure and Sufficient StatisticsError Probability Analysis and the Union Bound
Passband modulation
General principlesAmplitude and phase modulationPulse amplitude modulation (MPAM)Phase shift keying (MPSK)Quadrature amplitude modulation (MQAM)
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Amplitude and phase modulation (cont.)
Since the pulse shape () is fixed, the signal constellation foramplitude and phase modulation is defined based on theconstellation point: (,1, ,2) ∈ ℝ2, = 1,..., .
The complex baseband representation of () is
() = Re
() 0 2
(47)
where:
() = () + () = (,1 + ,2) ().
The constellation point s = (,1, ,2) is called the symbolassociated with the log2 bits and is called the symbol time and the bit rate for thismodulation is bits per symbol or = log2 / bits persecond.
Mobile communications - Chapter 3: Physical-layer transmissions Section 3.1: Digital modulations 57
Digital modulation techniques
Signal Space AnalysisReceiver Structure and Sufficient Statistics
Error Probability Analysis and the Union BoundPassband modulation
General principles
Amplitude and phase modulationPulse amplitude modulation (MPAM)Phase shift keying (MPSK)Quadrature amplitude modulation (MQAM)
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Amplitude and phase modulation (cont.)
There are three main types of amplitude/phase modulation:
Pulse Amplitude Modulation (MPAM): information encoded inamplitude only.Phase Shift Keying (MPSK): information encoded in phase
only.Quadrature Amplitude Modulation (MQAM): informationencoded in both amplitude and phase.
The number of bits per symbol = log2 , signalconstellation (,1, ,2)
∈ℝ2, = 1,..., , and the choice of
shaping pulse () determines the digital modulation design.The pulse shape () is designed to improve spectral efficiencyand combat inter-symbol-interference (ISI).
Mobile communications - Chapter 3: Physical-layer transmissions Section 3.1: Digital modulations 58
Digital modulation techniques
Signal Space AnalysisReceiver Structure and Sufficient Statistics
Error Probability Analysis and the Union BoundPassband modulation
General principles
Amplitude and phase modulationPulse amplitude modulation (MPAM)Phase shift keying (MPSK)Quadrature amplitude modulation (MQAM)
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Amplitude and phase modulation (cont.)
Amplitude and phase modulation over a given symbol periodcan be generated using the modulator structure shown in thenext Figure.
Note that the basis functions in this figure have an arbitrary
phase 0 associated with the transmit oscillator.Demodulation over each symbol period is performed using thedemodulation structure of Figure xx +1, which is equivalentto the structure of for 1() = ()cos(2 + ) and2() =
−()sin(2 + ).
Typically the receiver includes some additional circuitry forcarrier phase recovery that matches the carrier phase at thereceiver to the carrier phase 0 at the transmitter, which iscalled coherent detection.
Mobile communications - Chapter 3: Physical-layer transmissions Section 3.1: Digital modulations 59
Digital modulation techniques
Signal Space AnalysisReceiver Structure and Sufficient Statistics
Error Probability Analysis and the Union BoundPassband modulation
General principles
Amplitude and phase modulationPulse amplitude modulation (MPAM)Phase shift keying (MPSK)Quadrature amplitude modulation (MQAM)
( )
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Amplitude and phase modulation (cont.)
If − 0 = △ ∕= 0 then the in-phase branch will have anunwanted term associated with the quadrature branch andvice versa, i.e., 1 = ,1 cos(△) + ,2 sin(△) + 1 and2 = ,1 sin(△) + ,2 cos(△) + 2 can result in significantperformance degradation.
The receiver structure also assumes that the sampling functionevery seconds is synchronized to the start of the symbolperiod, which is called synchronization or timing recovery.
Receiver synchronization and carrier phase recovery are
complex receiver operations that can be highly challenging inwireless environments.
We will assume perfect carrier recovery in our discussion of MPAM, MPSK and MQAM, and therefore set = 0 = 0 fortheir analysis.
Mobile communications - Chapter 3: Physical-layer transmissions Section 3.1: Digital modulations 60
Digital modulation techniques
Signal Space AnalysisReceiver Structure and Sufficient Statistics
Error Probability Analysis and the Union BoundPassband modulation
General principles
Amplitude and phase modulationPulse amplitude modulation (MPAM)Phase shift keying (MPSK)Quadrature amplitude modulation (MQAM)
P l li d d l i (MPAM)
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Pulse amplitude modulation (MPAM)
We will start by looking at the simplest form of linearmodulation, one-dimensional MPAM, which has noquadrature component (,2 = 0).
For MPAM all of the information is encoded into the signal
amplitude . The transmitted signal over one symbol time isgiven by
() = Re
() 2
= ()cos(2 ), 0 ≤ ≤ ≫ 1/ ,
(48)
where = (2 − 1 − ), = 1, 2,..., defines the signalconstellation, parameterized by the distance which istypically a function of the signal energy, and () is theshaping pulse.
Mobile communications - Chapter 3: Physical-layer transmissions Section 3.1: Digital modulations 61
Digital modulation techniques
Signal Space AnalysisReceiver Structure and Sufficient Statistics
Error Probability Analysis and the Union BoundPassband modulation
General principles
Amplitude and phase modulationPulse amplitude modulation (MPAM)Phase shift keying (MPSK)Quadrature amplitude modulation (MQAM)
P l li d d l i ( )
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Pulse amplitude modulation (cont.)
π2
ShapingFilter g(t)
ShapingFilter g(t)
s(t)
In−Phase branch
Quadrature Branch
i1
i2s
s i1s g(t)
s g(t)i2
c−sin(2 f t+ )
cos(2 f t+ )cπ φ
0
cos(2 f t+ )cπ φ
0
π φ0
Figure 2: Amplitude and phase modulator.Mobile communications - Chapter 3: Physical-layer transmissions Section 3.1: Digital modulations 62
Digital modulation techniques
Signal Space AnalysisReceiver Structure and Sufficient Statistics
Error Probability Analysis and the Union BoundPassband modulation
General principles
Amplitude and phase modulationPulse amplitude modulation (MPAM)Phase shift keying (MPSK)Quadrature amplitude modulation (MQAM)
P l lit d d l ti ( t )
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Pulse amplitude modulation (cont.)
The minimum distance between constellation points is = , ∣ − ∣= 2. The amplitude of thetransmitted signal takes on M different values, which impliesthat each pulse conveys 2 = bits per symbol time .
Over each symbol period the MPAM signal associated withthe th constellation has energy
=
0
2 () =
0
2
2()cos2(2 ) = 2 . (49)
It is noted that the energy is not the same for each signal(), = 1,..., .
Mobile communications - Chapter 3: Physical-layer transmissions Section 3.1: Digital modulations 63
Digital modulation techniques
Signal Space AnalysisReceiver Structure and Sufficient Statistics
Error Probability Analysis and the Union BoundPassband modulation
General principles
Amplitude and phase modulationPulse amplitude modulation (MPAM)Phase shift keying (MPSK)Quadrature amplitude modulation (MQAM)
P l lit d d l ti ( t )
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Pulse amplitude modulation (cont.)
Assuming equally likely symbols, the average energy is
=1
=1
2 . (50)
i
1
m̂=m
Find i: x Zi
i
T
TIn−Phase branch
π/2
g(T−t)
g(T−t)
cos (2 f t+ )φ
i1 1
2 i2 2
Quadrature branch
s
s
π c
−sin (2 f t+ )cπ φ
r(t)=s (t)+n(t)
r =s +n
r =s +n
Mobile communications - Chapter 3: Physical-layer transmissions Section 3.1: Digital modulations 64
Digital modulation techniques
Signal Space AnalysisReceiver Structure and Sufficient Statistics
Error Probability Analysis and the Union BoundPassband modulation
General principles
Amplitude and phase modulationPulse amplitude modulation (MPAM)Phase shift keying (MPSK)Quadrature amplitude modulation (MQAM)
P l lit d d l ti ( t )
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Pulse amplitude modulation (cont.)
The constellation mapping is usually done by Gray encoding,where the messages associated with signal amplitudes that areadjacent to each other differ by one bit value, as illustrated inthe below figure.With this encoding method, if noise causes the demodulation
process to mistake one symbol for an adjacent one (the mostlikely type of error), this results in only a single bit error in thesequence of K bits. Gray codes can be designed for MPSK andsquare MQAM constellations, but not rectangular MQAM.
M=4, K=2
00 01 11 10
M=8, K=3
000 001 011 010 110 111 101 100
2d
2dMobile communications - Chapter 3: Physical-layer transmissions Section 3.1: Digital modulations 65
Digital modulation techniques
Signal Space AnalysisReceiver Structure and Sufficient Statistics
Error Probability Analysis and the Union BoundPassband modulation
General principles
Amplitude and phase modulationPulse amplitude modulation (MPAM)Phase shift keying (MPSK)Quadrature amplitude modulation (MQAM)
Pulse amplitude modulation (cont )
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Pulse amplitude modulation (cont.)
An example: For () = 2/ , 0 ≤ < a rectangularpulse shape, find the average energy of 4PAM modulation.Solution: For 4PAM, the values are = {3, −,, 3}.Hence, the average is
=2
4 (9 + 1 + 1 + 9) = 52. (51)
The decision regions , = 1,..., associated with thepulse amplitude = (2 − 1 − ) for = 4 and = 8as shown in the next figure. Mathematically, for any , these
decision regions are defined by
=
⎧⎨(−∞, + ) = 1,
[ − , + ) 2 ≤ ≤ − 1
[ −
,∞
) =
(52)
Mobile communications - Chapter 3: Physical-layer transmissions Section 3.1: Digital modulations 66
Digital modulation techniques
Signal Space AnalysisReceiver Structure and Sufficient Statistics
Error Probability Analysis and the Union BoundPassband modulation
General principles
Amplitude and phase modulationPulse amplitude modulation (MPAM)Phase shift keying (MPSK)Quadrature amplitude modulation (MQAM)
Pulse amplitude modulation (cont )
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Pulse amplitude modulation (cont.)
One can see that MPAM has only a single basis function1() = () cos(2 ).
Thus, the coherent demodulator for MPAM reduces to thedemodulator shown in the next figure, where themulti-threshold device maps to a decision region andoutputs the corresponding bit sequence
=
={
1
,..., }
.
Mobile communications - Chapter 3: Physical-layer transmissions Section 3.1: Digital modulations 67
Digital modulation techniques
Signal Space AnalysisReceiver Structure and Sufficient Statistics
Error Probability Analysis and the Union BoundPassband modulation
General principles
Amplitude and phase modulationPulse amplitude modulation (MPAM)Phase shift keying (MPSK)Quadrature amplitude modulation (MQAM)
Pulse amplitude modulation (cont )
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Pulse amplitude modulation (cont.)
2d
2d
A1
A A A2 3 4
Z1
Z Z2
Z3 4
A A A A
Z Z Z ZZ1
Z Z
A1
A2 3
Z2 3 4 5 6 7 8
A A87654
Figure 5: Decision Regions for MPAM.
is (t)+n(t)s
xg (T −t) 0X
cos(2 f t)cπ
^
s
T
Multithreshold Device
2d
4d
−2d
−4d
−(M−2)d
(M−2)d
m=m =b b ...bi 1 2 K
} Zi
Mobile communications - Chapter 3: Physical-layer transmissions Section 3.1: Digital modulations 68
Digital modulation techniques
Signal Space AnalysisReceiver Structure and Sufficient Statistics
Error Probability Analysis and the Union BoundPassband modulation
General principles
Amplitude and phase modulationPulse amplitude modulation (MPAM)Phase shift keying (MPSK)Quadrature amplitude modulation (MQAM)
Phase shift keying (MPSK)
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Phase shift keying (MPSK)
For MPSK modulation, all of the information is encoded inthe phase of the transmitted signal.
Thus, the transmitted signal over one symbol time is given by
() = Re () 2(−1)/ 2 , 0 ≤ ≤ (53)
= ()cos
2 +
2( − 1)
= ()cos 2(
−1)
cos(2 )
− ()sin
2( − 1)
sin(2 ).
Mobile communications - Chapter 3: Physical-layer transmissions Section 3.1: Digital modulations 69
Digital modulation techniques
Signal Space AnalysisReceiver Structure and Sufficient Statistics
Error Probability Analysis and the Union BoundPassband modulation
General principles
Amplitude and phase modulationPulse amplitude modulation (MPAM)Phase shift keying (MPSK)Quadrature amplitude modulation (MQAM)
Phase shift keying (cont )
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Phase shift keying (cont.)
The constellation points or symbols (,1, ,2) are given by
,1 = cos2(−1)
and ,2 = sin
2(−1)
for
= 1,..., . =2(−1) , = 1, 2,..., = 2 are the
different phases in the signal constellation points that conveythe information bits.
The minimum distance between constellation points is = 2 sin(/ ), where is typically a function of thesignal energy.
2PSK is often referred to as binary PSK or BPSK, while 4PSKis often called quadrature phase shift keying (QPSK), and isthe same as MQAM with = 4 which is defined below.
Mobile communications - Chapter 3: Physical-layer transmissions Section 3.1: Digital modulations 70
Digital modulation techniques
Signal Space AnalysisReceiver Structure and Sufficient Statistics
Error Probability Analysis and the Union BoundPassband modulation
General principles
Amplitude and phase modulationPulse amplitude modulation (MPAM)Phase shift keying (MPSK)Quadrature amplitude modulation (MQAM)
Phase shift keying (cont )
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Phase shift keying (cont.)
All possible transmitted signals () have equal energy:
=
02 () = 2. (54)
Note that for () =
2/ , 0 ≤ ≤ , i.e., a rectangularpulse, this signal has constant envelope, unlike the otheramplitude modulation techniques MPAM and MQAM.
However, rectangular pulses are spectrally-inefficient, andmore efficient pulse shapes make MPSK nonconstantenvelope.
Mobile communications - Chapter 3: Physical-layer transmissions Section 3.1: Digital modulations 71
Digital modulation techniques
Signal Space AnalysisReceiver Structure and Sufficient Statistics
Error Probability Analysis and the Union BoundPassband modulation
General principles
Amplitude and phase modulationPulse amplitude modulation (MPAM)Phase shift keying (MPSK)Quadrature amplitude modulation (MQAM)
Phase shift keying (cont )
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Phase shift keying (cont.)
Analogous to MPAM, MPSK constellation mapping is usuallydone by Gray encoding, where the messages associated withsignal phases that are adjacent to each other differ by one bitvalue, as illustrated in the below Figure.With this encoding method, mistaking a symbol for an
adjacent one causes only a single bit error.
=4, K=2
0011
01
10
M=8, K=3
000
001
011
110
100
010
110
101
si1
si2
si1
si2
Figure 7: Gray Encoding for MPSK.Mobile communications - Chapter 3: Physical-layer transmissions Section 3.1: Digital modulations 72
Digital modulation techniques
Signal Space AnalysisReceiver Structure and Sufficient StatisticsError Probability Analysis and the Union Bound
Passband modulation
General principles
Amplitude and phase modulationPulse amplitude modulation (MPAM)Phase shift keying (MPSK)Quadrature amplitude modulation (MQAM)
Phase shift keying: Decision region
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Phase shift keying: Decision region
The decision regions , = 1,..., , associated with MPSKfor = 8 are shown in the next figure.
If we represent r = ∈ ℝ2 in polar coordinates then thesedecision regions for any are defined by
=
: 2( − .5)/ ≤ ≤ 2( + .5)/
. (55)
For the special case of BPSK, the decision regions simplify to 1 = (r : r > 0) and 2 = (r : r
≤0).
Moreover BPSK has only a single basis function1() = () cos(2 ) and, since there is only a single bittransmitted per symbol time , the bit duration = .
Mobile communications - Chapter 3: Physical-layer transmissions Section 3.1: Digital modulations 73
Digital modulation techniques
Signal Space AnalysisReceiver Structure and Sufficient StatisticsError Probability Analysis and the Union Bound
Passband modulation
General principles
Amplitude and phase modulationPulse amplitude modulation (MPAM)Phase shift keying (MPSK)Quadrature amplitude modulation (MQAM)
Phase shift keying: Decision region (cont.)
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Phase shift keying: Decision region (cont.)
Thus, the coherent demodulator for BPSK reduces to thedemodulator shown in the next figure, where the thresholddevice maps to the positive or negative half of the real line,
and outputs the corresponding bit value.We have assumed in this figure that the messagecorresponding to a bit value of 1, 1 = 1, is mapped toconstellation point 1 = and the message corresponding to
a bit value of 0, 2 = 0, is mapped to the constellation point2 = −.
Mobile communications - Chapter 3: Physical-layer transmissions Section 3.1: Digital modulations 74
Digital modulation techniques
Signal Space AnalysisReceiver Structure and Sufficient StatisticsError Probability Analysis and the Union Bound
Passband modulation
General principles
Amplitude and phase modulationPulse amplitude modulation (MPAM)Phase shift keying (MPSK)Quadrature amplitude modulation (MQAM)
Phase shift keying: Decision region (cont.)
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ase s t ey g ec s o eg o (co t )
Z1
Z2
Z3
Z4
Z1
Z2
Z
Z
Z
Z
Z
Z
34
5
6
7
8
Figure 8: Decision Regions for MPSK.
is (t)+n(t)g (T −t)
b 0X
cos(2 f t)cπ
^Tb
Threshold Device
2
m=1 or 0
m=1^
m̂=0
}
}r 1
Z :r>0
Z :r<0
Figure 9: Coherent Demodulator for BPSK.Mobile communications - Chapter 3: Physical-layer transmissions Section 3.1: Digital modulations 75
Digital modulation techniques
Signal Space AnalysisReceiver Structure and Sufficient StatisticsError Probability Analysis and the Union Bound
Passband modulation
General principles
Amplitude and phase modulationPulse amplitude modulation (MPAM)Phase shift keying (MPSK)Quadrature amplitude modulation (MQAM)
Quadrature amplitude modulation (MQAM)
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Q p ( Q )
For MQAM, the information bits are encoded in both theamplitude and phase of the transmitted signal.
Thus, whereas both MPAM and MPSK have one degree of freedom in which to encode the information bits (amplitude orphase), MQAM has two degrees of freedom.
As a result, MQAM is more spectrally-efficient than MPAMand MPSK, in that it can encode the most number of bits per
symbol for a given average energy.
Mobile communications - Chapter 3: Physical-layer transmissions Section 3.1: Digital modulations 76
Digital modulation techniques
Signal Space AnalysisReceiver Structure and Sufficient StatisticsError Probability Analysis and the Union Bound
Passband modulation
General principles
Amplitude and phase modulationPulse amplitude modulation (MPAM)Phase shift keying (MPSK)Quadrature amplitude modulation (MQAM)
Quadrature amplitude modulation (cont.)
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Q p ( )
The transmitted signal is given by() = Re
() 2
(56)
= cos()() cos(2 ) − sin()()sin(2 ).
where 0≤
≤
.
The energy in () is
=
0
2 () = 2 . (57)
that is the same as for MPAM.
The distance between any pair of symbols in the signalconstellation is
, = ∥s − s∥ =
(,1 − ,1)2 + (,2 − ,2)2. (58)
Mobile communications - Chapter 3: Physical-layer transmissions Section 3.1: Digital modulations 77
Digital modulation techniques
Signal Space AnalysisReceiver Structure and Sufficient StatisticsError Probability Analysis and the Union Bound
Passband modulation
General principles
Amplitude and phase modulationPulse amplitude modulation (MPAM)Phase shift keying (MPSK)Quadrature amplitude modulation (MQAM)
Quadrature amplitude modulation (cont.)
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p ( )
For square signal constellations, where ,1 and ,2 takevalues on (2 − 1 − ), = 1, 2,..., = 2, the minimumdistance between signal points reduces to = 2, the
same as for MPAM.In fact, MQAM with square constellations of size 2 isequivalent to MPAM modulation with constellations of size on each of the in-phase and quadrature signal components.
Common square constellations are 4QAM and 16QAM, whichare shown in the below figure.
Mobile communications - Chapter 3: Physical-layer transmissions Section 3.1: Digital modulations 78
Digital modulation techniques
Signal Space AnalysisReceiver Structure and Sufficient StatisticsError Probability Analysis and the Union Bound
Passband modulation
General principles
Amplitude and phase modulationPulse amplitude modulation (MPAM)Phase shift keying (MPSK)Quadrature amplitude modulation (MQAM)
Quadrature amplitude modulation: constellation and
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decision regions
4−QAM 16−QAM
Figure 10: 4QAM and 16QAMConstellations.
Z1
Z2
Z3
Z4
Z5
Z6
Z7
Z8
Z9
Z10
Z11
Z12
Z13
Z14
Z15
Z16
Figure 11: Decision Regions forMQAM withM = 16.
Mobile communications - Chapter 3: Physical-layer transmissions Section 3.1: Digital modulations 79
Digital modulation techniques
Signal Space AnalysisReceiver Structure and Sufficient StatisticsError Probability Analysis and the Union Bound
Passband modulation
General principles
Amplitude and phase modulationPulse amplitude modulation (MPAM)Phase shift keying (MPSK)Quadrature amplitude modulation (MQAM)
Quadrature amplitude modulation: constellation and
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decision regions
These square constellations have = 22 = 2 constellationpoints, which are used to send 2 bits/symbol, or bits perdimension.
It can be shown that the average power of a square signalconstellation with bits per dimension, , is proportional to4/3, and it follows that the average power for one more bitper dimension +1 ≈ 4 .
Thus, for square constellations it takes approximately 6 dBmore power to send an additional 1 bit/dimension or 2bits/symbol while maintaining the same minimum distancebetween constellation points.
Mobile communications - Chapter 3: Physical-layer transmissions Section 3.1: Digital modulations 80