63RVWJUDGXDWH6HPLQDULQ5DGLR&RPPXQLFDWLRQV S-72.333 Post-graduate Course in Radio Communications 2001-2002 Fitting Signals into Given Spectrum Modulation Methods Lars Maura 41747e Lars.maura@hut.fi 63RVWJUDGXDWH6HPLQDULQ5DGLR&RPPXQLFDWLRQV Abstract Modulation is the process where the message information is embedded into the radio carrier. Message information can be transferred in the amplitude, frequency or the phase component of the carrier signal. Modulation methods are categorised according to which component is used for transmitting the information. To achieve high spectral efficiency, modulation schemes need to have high bandwidth efficiency. Three properties need to be satisfied, when digital modulation techniques are chosen for wireless systems. First, compact power density spectrum with a narrow main lobe and fast roll-off of side-lobes is required to minimise the channel interference. Secondly a good error rate performance in all environments is required. Finally a constant envelope is important in mobile applications, where battery power is a limited sourceand amplifiers are typically non-linear. In this study, different modulation methods and the bit error performance with different modulation methods and signal sets are evaluated. One important factor in bit error performance is the shape of the pulse. To prevent intersymbol interference the selected pulse shape has to satisfy the Nyquist criterion. The ideal Nyquist pulse, however, has slow time decay. Therefore other pulses that satisfy the criterion has to be constructed. Different modulation methods are evaluated. The signal constellation is an important factor when error probability is calculated. In coherent demodulation of two equally likely signals transmitted on AWGN channel the error probability depends only on the Euclidean distance between the two signals. Any digital modulation aims at realising the best possible trade-off in a given situation among the bit error probability, the bandwidth efficiency, the signal to noise ratio and the complexity of the equipment. In the end the performance of these modulation methods’ are compared. The power density function is not in the scope of this study. The background material consists of three books. All of them descibes digital modulation methods and could be used as such. The most part in this study is refers to St über [1], but the presentation of Nyquist criterion is mainly based on Lee [2] and in the evaluation of error performance I used Benedetto [3]. Lars.maura@hut.fi 2(39) 63RVWJUDGXDWH6HPLQDULQ5DGLR&RPPXQLFDWLRQV Table of Contents Abstract............................................................................................................................... 3 Table of Contents................................................................................................................ 5 Abbreviations ...................................................................................................................... 7 1 Digital Modulation ........................................................................................................ 9 2 Nyquist Pulse Shaping............................................................................................... 11 3 Error Probability Evaluation ....................................................................................... 17 3.1.1 Symbol Error Probability for Binary Signals............................................... 18 3.1.2 Symbol Error Probability for Rectangular Signal Sets ............................... 21 4 Digital Modulation Schemes ...................................................................................... 24 4.1 Quadrature Amplitude Modulation ...................................................................... 24 4.2 Phase Shift Keying ............................................................................................. 25 4.2.1 Offset Quadrature Phase Shift Keying....................................................... 27 4.2.2 ’π/4’-DQPSK .............................................................................................. 29 4.3 Orthogonal Modulation ....................................................................................... 30 4.4 Orthogonal Frequency Division Multiplexing....................................................... 31 4.4.1 Multiresolution Modulation......................................................................... 31 4.4.2 FFT-based OFDM System ........................................................................ 33 4.5 Continuous Phase Modulation ............................................................................ 33 4.5.1 Full Response CPM .................................................................................. 34 4.5.2 Minimum Shift Keying................................................................................ 35 4.5.3 Partial Response CPM .............................................................................. 37 5 Digital Modulation Trade-Offs .................................................................................... 38 Litterature.......................................................................................................................... 41 Lars.maura@hut.fi 3(39) 63RVWJUDGXDWH6HPLQDULQ5DGLR&RPPXQLFDWLRQV Abbreviations AWGN BER FFT ISI ML LAN PDS Additive White Gaussian Noise Bit Error Rate Fast Fourier Transform Intersymbol Interference Maximum Likelihood Local Area Network Power Density Spectrum Modulation methods: π/4-DQPSK π/4-Differential QPSK CPM Continuous Phase Modulation CPFSK Continuous Phase Frequency Shift Keying DCPSK Differentially Coherent Phase Shift Keying FSK Frequency Shift Keying GMSK Gaussian Minimum Shift Keying MRM Multiresolution Modulation MSK Minimum Shift Keying OFDM Orthogonal Frequency Division Multiplexing OQPSK Offset QPSK PAM Pulse Amplitude Modulation PSK Phase Shift Keying QAM Quadrature Amplitude Modulation QPSK Quadrature Phase Shift Keying Lars.maura@hut.fi 4(39) 63RVWJUDGXDWH6HPLQDULQ5DGLR&RPPXQLFDWLRQV 1 Digital Modulation Modulation is the process where the message information is embedded into the radio carrier. Message information can be transferred in 1. amplitude, 2. frequency or 3. the phase 1 3 2 of the carrier or a combination of these in either analog or digital form. In digital cellular systems digital modulation is used because of its bandwidth efficiency. To achieve high spectral efficiency, modulation schemes need to have high bandwidth efficiency, measured in units of bits per second Hertz of bandwidth (bits/s/Hz). When digital modulation techniques are chosen for wireless systems following three properties need to be satisfied: Compact Power Density Spectrum: To minimise the effect of adjacent channel interference, the power radiated into the adjacent band should be 60 to 80 dB below that in the desired band. Hence, modulation techniques with a narrow main lobe and fast roll-off of side-lobes are needed. Good Bit Error Rate Performance: A low bit error probability must be achieved in the presence of fading, Doppler spread, intersymbol interference, adjacent and cochannel interference and thermal noise. In this presentation only intersymbol interference and noise are considered. Envelope Properties: Portable and mobile applications typically employ non-linear power amplifiers to minimise battery drain. Non-linear amplification may degrade the bit error rate (BER) performance of modulation schemes that transmit information in the amplitude of the carrier. Also, spectral shaping is usually performed prior to upconversion and non-linear amplification. To prevent the regrowth of spectral sidelobes during non-linear amplification, relatively constant envelope modulation schemes are preferred. Two of the more widely used digital modulation techniques for cellular mobile radio are π/4-DQPSK and GMSK. In both modulation methods the information is carried in the phase component of the carrier signal. Lars.maura@hut.fi 5(39) 63RVWJUDGXDWH6HPLQDULQ5DGLR&RPPXQLFDWLRQV 2 Nyquist Pulse Shaping Example: If the channel is an ideal bandlimited channel B ( jω ) = 1 , when ω < W and B ( jω ) = 0 , when ω ≥ W , then the ideally bandlimited pulse can be used which in time domain is a sinc pulse as shown below. Now consider two successive symbols with values a 0 = 1 and a1 = 2 . The contribution of these two symbols to the signal is shown below If the channel is ideally bandlimited, then the receiver only needs to sample at 0 and T . Neighboring symbols do not interfere with one another at the proper sampling time, so there is no intersymbol interference (ISI). Consider a modulation scheme where the complex envelope has the form ~ s (t ) = A∑ x n p (t − nT ) n Where p(t ) is a shaping pulse, {x n } is the complex data symbol sequence, and T is the baud period. Now suppose the complex envelope is sampled every T seconds to yield the sample sequence {y n }, yk = ~ s (kT + t 0 ) = A∑ x n p (kT + t 0 − nT ) n Where t 0 is a timing offset assumed to lie in the interval [0, T ) . When t 0 = 0 and p m = p(mT ) is the sampled pulse Lars.maura@hut.fi 6(39) 63RVWJUDGXDWH6HPLQDULQ5DGLR&RPPXQLFDWLRQV y k = A∑ x n p k −n = Ax k p 0 + A∑ x n p k −n n n≠k The first term is equal to the data symbol transmitted at the k th baud epoch, scaled by the factor p 0 . The second term is the contribution of all other data symbols on the sample y k . This term is called intersymbol interference (ISI). To avoid the appearance of ISI, the sampled pulse response {p k } must satisfy the condition p k = δ k 0 p0 Therefore, to avoid ISI the pulse p(t ) must have equally spaced zero crossings at intervals of T seconds. This requirement is known as the (first) Nyquist criterion. An equivalent requirement in the frequency domain is PΣ ( f ) =ˆ 1 ∞ n P f + = p 0 ∑ T n = −∞ T This allows us to design pulses in frequency domain that will yield to zero ISI. First consider the pulse P( f ) = T ⋅ rect ( fT ) , Figure 1 Pulse rect(fT) This pulse yields a flat folded spectrum. In the time domain p(t) = sinc(t/T) This pulse achives the Nyquist criterion because it has equally spaced zero crossings at T second intervals. Furthermore, from the requirement of a flat folded spectrum, it achieves zero ISI while occupying the smallest possible bandwidth, hence, it is called an ideal Nyquist pulse. However, the problem with this pulse is that the roll-off of side-lobes is slow. Better roll-off factors are given by raised cosine and root raised cosine pulses which also achieves Nyquist criterion, see figure 2. Raised cosine pulses are given by Lars.maura@hut.fi 7(39) 63RVWJUDGXDWH6HPLQDULQ5DGLR&RPPXQLFDWLRQV sin (πt T ) cos(απt T ) p (t ) = 2 πt T 1 − (2αt T ) where α is the so called roll-off factor. For α = 0, the pulse is identical to the ideally bandlimited pulse. For other values of α, the energy rolls off more gradually with increasing frequency. The pulse for α = 0 is the pulse with the smallest bandwidth that has zero crossings at multiples of π W ; larger values of α require excess bandwidth varying from 0% to 100% as α varies from 0 to 1. In the time domain, the tails of the pulses are infinite in extent. However, as α increases, the size of the tails diminishes. Figure 2 Raised cosine pulses with different roll-off factors There are an infinite number of pulses that satisfy the Nyquist criterion and hence have zero crossings at multiples of π W . Some of these are shown in figure 3. Figure 3 The Fourier transform of some pulses that satisfy the Nyquist criterion Lars.maura@hut.fi 8(39) 63RVWJUDGXDWH6HPLQDULQ5DGLR&RPPXQLFDWLRQV 3 Error Probability Evaluation It is assumed that the analog channel connecting the modulator output to the demodulator input is an additive white Gaussian noise (AWGN channel with an infinite bandwidth. The demodulator is a maximum likelihood (ML) demodulator and operates according to minimum distance rule. Figure 4 Geometry of the minimum distance rule The signal in figure 4 is a complex signal with three possible symbols. When symbol sI is received, the receiver observes signal r. While the channel adds noise to the transmitted signal, the observed signal is r = sI + n ≠ si as in figure 4. The minimum distance detector chooses the nearest value of the possible signal set. For correct detection, the received signal has to be observed in the correct decision area. Noise is assumed to be zero-mean Gaussian noise with variance N0/2. Having a random signal, i.e. all symbols are equally likely, the symbol error probability is expressed as P(e ) = 1 − P(c ) = 1 − 1 M ∑ P(c | s ), M j =1 j ( ) where P c s j is the probability of a correct decision given that the signal vector s j , corresponding to the symbol m j , was transmitted. Lars.maura@hut.fi 9(39) 63RVWJUDGXDWH6HPLQDULQ5DGLR&RPPXQLFDWLRQV 3.1.1 Symbol Error Probability for Binary Signals Figure 5 Detection decision regions for binary signals For a binary signal in figure 5 b), the symbol error probability can be determined as follows. Signal s1 is detected with error, if noise element causes the detection to recognise a value less than 0. This happens when the additive noise equals n < − d / 2 . Now we can write the symbol error probability as d P(e ) = P n < − 2 Using the definition of error function P(ξ > x ) = 1 x−m erfc , 2 2σ and remembering that noise is zero-mean with variance N 0 / 2 , symbol error probability can be written P(e ) = Lars.maura@hut.fi d 1 erfc 2 N 2 0 . 10(39) 63RVWJUDGXDWH6HPLQDULQ5DGLR&RPPXQLFDWLRQV Figure 6 Error probability for antipodal and orthogonal binary signals This means, that coherent demodulation of two equally likely signals transmitted on the AWGN channel, the error probability depends only on the Euclidean distance between the two signals. I.e. the selection of the set of symbols has an impact on error probability. Comparing antipodal signals to orthogonal signals in figure 6 shows, that there is a 3 dB penalty in the signal energy to be paid with orthogonal signals with respect to antipodal signals which are shown in figure 5. 3.1.2 Symbol Error Probability for Rectangular Signal Sets The binary representation can be applied to signal sets that have a “rectangular” configuration. This means the cases where the decision regions are 2D-hyperplanes. Figure 7 Received samples perturbed by additive Gaussian noise form a Gaussian cloud around each of the points in the signal constellation Lars.maura@hut.fi 11(39) 63RVWJUDGXDWH6HPLQDULQ5DGLR&RPPXQLFDWLRQV Figure 8 2D signal set with 16 signals, a 16-QAM signal constellation By studying the different decision regions in the signal set in figure 8, we can see that there are only three different types of decision areas. First we need to define the probabilities for correct decisions. p1 =ˆ P(c s1 ) p 2 =ˆ P(c s 2 ) p3 =ˆ P(c s3 ) When different noise-components are independent of each other, we can define by using the results of binary case s −s s −s p1 = P n1 < 1 2 ⋅ P n2 > 1 5 2 2 d d = P n1 < ⋅ P n2 < 2 2 = (1 − p ) 2 where p is the symbol error probability for binary signals with Euclidean distance d between the different symbols. With similar calculation we can obtain p2 = (1 − 2 p )(1 − p ) p3 = (1 − 2 p ) 2 , where p =ˆ d 1 erfc 2 N 2 0 Finally we can obtain the total symbol error probability for signal set in figure 8 P ( e ) = 4 p1 + 8 p2 + 4 p3 = 1− Lars.maura@hut.fi 1 2 (2 − 3 p) 4 12(39) 63RVWJUDGXDWH6HPLQDULQ5DGLR&RPPXQLFDWLRQV 4 Digital Modulation Schemes 4.1 Quadrature Amplitude Modulation When using quadrature amplitude modulation (QAM) the data information is transmitted in the amplitude component of the signal. The quadrature representation is a special case of pulse amplitude modulation (PAM). In QAM, two PAM-signals are combined in, and the combination of these determines the transferred signal. With QAM, the complex envelope is ~ s (t ) = A∑ b(t − nT , x n ) n where b(t , x n ) = x n ha (t ) ha ( t ) is the amplitude shaping pulse and xn = xI ,n + jxQ , n is the complex data symbol that is transmitted at epoch n. It is apparent that with the amplitude and the phase of a QAM signal depend on the complex symbol. QAM has the advantage of high bandwidth efficiency, but amplifier nonlinearities will degrade its performance due to the non-constant envelope. Figure 9 Complex signal-space diagram for square QAM constellation A variety of QAM signal constellations may be constructed. Square constellations can be constructed when M is a power of 4, as shown in figure 9. When M is not a power of 4, the signal constellation is not a square. Usually, the constellation is given the shape of a Lars.maura@hut.fi 13(39) 63RVWJUDGXDWH6HPLQDULQ5DGLR&RPPXQLFDWLRQV cross to minimise the average energy in the constellation for a given minimum Euclidean distance between signal vectors. Error probability for 16-QAM was calculated in previous chapter. 4.2 Phase Shift Keying In PSK modulation the information is signalled in the phase-component. The complex envelope is ~ s (t ) = A∑ b(t − nT , x n ) n where b(t , x n ) = ha (t )e jθ The carrier phase takes on values θn = 2π xn + θ 0 M Figure 10 Complex signal-space diagram QPSK, OQPSK and π/4-DQPSK The source binary symbols are Gray-coded. As a consequence, adjacent phase signals differ by only one binary digit. 4.2.1 Offset Quadrature Phase Shift Keying QPSK or 4-PSK is equivalent to 4-QAM. The QPSK signal can have either ±90° or ±180° phase shifts from one baud interval to the next. With offset QPSK (OQPSK) signals the possibility of ±180° phase shifts is eliminated. In fact the phase can change by only ±90° every Tb seconds. This corresponds to the bit rate of the signal. Lars.maura@hut.fi 14(39) 63RVWJUDGXDWH6HPLQDULQ5DGLR&RPPXQLFDWLRQV Figure 11 In-phase and quadrature baseband components in QPSK, OQPSK and MSK signals With OQPSK two bits are transferred every baud epoch as in QPSK, but the quadrature component is delayed by half of the baud rate. With this shift, the two separate components never change at the same time. The difference between QPSK and OQPSK is shown in figure 9. The in-phase components are the same, but the quadrature component is shifted by half of a symbol in OQPSK. Note from figure 10 that the phase trajectories do not pass through the origin. This property reduces the peak-to-average ratio of the complex envelope, making the OQPSK signal less sensitive to amplifier non-linearities than the QPSK signal. What is gained from OQPSK with respect to QPSK: Both methods have same error performance, since signal constellation is equal. The gain of choosing OQPSK is on power density spectrum. In OQPSK the ±180° phase shifts are eliminated and hence the pds is more compact. 4.2.2 ’π/4’-DQPSK QPSK transmits 2 bits/baud by transmitting sinusoidal pulses having one of 4 absolute phases. π/4-DQPSK also transmits 2 bits/baud, but information is encoded into the Lars.maura@hut.fi 15(39) 63RVWJUDGXDWH6HPLQDULQ5DGLR&RPPXQLFDWLRQV differential carrier phase and sinusoidal pulses having one of 8 absolute carrier phases are transmitted at each baud epoch. The phase differences are ±π/4 and ±3π/4. The absolute carrier phase during the even and odd baud intervals belongs to the sets {0, π/2, π, 3π/2} and {π/4, 3π/4, 5π/4, 7π/4}. With π/4-DQPSK the amplitude shaping pulse is often chosen to be the root raised cosine pulse. The signal space diagram is shown in figure 10, where the dotted lines show allowable phase transitions. Note that the phase trajectories do not pass through the origin. Like in OQPSK, this property reduces the peak-to-average ratio of the complex envelope, making the π/4-DQPSK signal less sensitive to amplifier non-linearities. The error performance is equal to QPSK, since signal constellation during one symbol is same (or shifted by π/4). 4.3 Orthogonal Modulation Orthogonal modulation schemes transmit information by using a set of waveforms, {sm (t )}mM=−01 that are orthogonal in time. FSK modulation technique provides simple means of generating an orthogonal signal set. Orthogonal M-ary frequency shift keying (MFSK) modulation uses a set of M waveforms that have different frequencies. For coherent demodulation orthogonality is met when the correlation coefficients of the real signal is zero. This condition is fulfilled when the frequency separation between adjacent signals is such that m , m any integer . 2 Thus the minimum frequency separation for orthogonality with coherent detection is such that 2 f d T = 0,5 . 2 fdT = The demodulation of of these types of signals increases the complexity in the receiver. The need for a bank of perfectly coherent oscillators renders it rather impractical. The bit error performance is though different from amplitude and phase modulation techniques. There exists an improvement in performance when M is increased, which is exactly the opposite behaviour of PAM and PSK signals. However, this improvement is obtained at the expense of a larger bandwidth. Increasing M requires more frequencies and therefore more bandwidth. For incoherent demodulation the orthogonality condition need to be fulfilled independently of the phases of the signals. The condition is fulfilled when the frequency separation between adjacent signals is Lars.maura@hut.fi 16(39) 63RVWJUDGXDWH6HPLQDULQ5DGLR&RPPXQLFDWLRQV 2 fdT = m , m any integer which is twice as much frequency separation as of coherent demodulation. The performance is somewhat inferior to the coherent case, but this is traded off by the easier implementation. 4.4 Orthogonal Frequency Division Multiplexing Orthogonal Frequency division multiplexing (OFDM) is a modulation technique that has been suggested for use in cellular radio, digital audio broadcasting, digital video broadcasting and wireless LAN systems. OFDM is a block modulation scheme where data symbols are transmitted in parallel by employing a (large) number of orthogonal subcarriers. 4.4.1 Multiresolution Modulation Multiresolution modulation (MRM) refers to a class of modulation techniques where multiple classes of bit streams are transmitted simultaneously that differ in their rates and error probabilities. Figure 12 16-QAM embedded MRM signal constellation, defining two priority classes Figure 12 shows and example of a 16-QAM MRM signal constellation, that can be used to transmit two diferent classes of bit streams, called low priority (LP) and high priority (HP). Two HP bits are used to select the quadrant of the transmitted signal point, while two LP bits are used to select the signal point within the selected quadrant. In order to control the relative error probability between the two priorities, a parameter λ = d l d h is used. In general, λ should be less than 0,5, since the MRM constellation becomes symmetric 16QAM at this point. As λ becomes smaller, more power is allocated to the HP bits and they are received with a smaller error probability. Lars.maura@hut.fi 17(39) 63RVWJUDGXDWH6HPLQDULQ5DGLR&RPPXQLFDWLRQV 4.4.2 FFT-based OFDM System A key advantage of using OFDMis that the modulation and demodulation can be achieved in the discrete-domain by using a discrete Fourier tranform. The fast Fourier transform (FFT) algorithm efficiently implements the discrete Fourier transform. When FFT is used, the rectangular shaping pulses turn into non-causal pulses in figure 13. Figure 13 Time domain OFDM amplitude shaping pulse Another key advantage of OFDM is the ease by which the effects of ISI can be mitigated. This can be done, by using a cyclic guard interval. The guard is appended to the generated signal in the transmitter. On the receiver it is assumed that the first sample is corrupted by ISI and therefore replaces the ISI-component with the guard. 4.5 Continuous Phase Modulation Continuous Phase modulation (CPM) refers to a broad class of frequency modulation techniques where the carrier phase varies in a continuous manner. CPM schemes are attractive because they have constant envelope and excellent spectral characteristics, i.e. narrow main lobe and fast roll-off of side lobes. The complex envelope of a general CPM waveform has the form ~ s (t ) = Ae j (φ (t )+θ 0 ) where φ (t ) is called the excess phase and defined as t ∞ φ (t ) = 2π ∫ ∑ hk x k h f (τ − kT )dτ 0 k =0 h f (t ) is the frequency shaping function, that is zero for t < 0 and t > LT . A full response CPM has L = 1 , while partial response CPM has L > 1 . The phase is continuous in CPM signals so long as the frequency shaping function does not contain impulses, which accounts for all practical cases. hk is the modulation index. Lars.maura@hut.fi 18(39) 63RVWJUDGXDWH6HPLQDULQ5DGLR&RPPXQLFDWLRQV 4.5.1 Full Response CPM Continuous phase frequency shift keying (CPFSK) is a special type of full response CPM obtained by using the rectangular frequency shaping function with L = 1 . h f (t ) = 1 u LT (t ) 2 LT Figure 14 Phase tree of binary CPFSK with modulation index h . CPM signals can be visualised by sketching the evolution of the excess phase Φ(t) for all possible data sequences. This plot is called a phase tree and a typical phase tree is shown in figure 14 for binary CPFSK. In each baud interval, the phase increases by πh if the data symbol is +1 and decreases by πh if the data symbol is -1. 4.5.2 Minimum Shift Keying Minimum shift keying (MSK) is a special case of CPFSK, with modulation index h = 1 2 and number of levels M = 2 . The MSK signal can be described in terms of the phase tree in figure 14 with h = 1 2 . At the end of each symbol interval the excess phase φ (t ) takes on values that are integer multiplies of π 2 and a phase trellis may be plotted. Figure 15 Phase trellis diagram for MSK. Lars.maura@hut.fi 19(39) 63RVWJUDGXDWH6HPLQDULQ5DGLR&RPPXQLFDWLRQV Consider the MSK band-pass waveform in the interval [nT , (n + 1)T ] , given by x π n −1 πn s (t ) = A cos 2π f c + n t + ∑ x k − xn . 4T 2 k =0 2 Observe that the MSK signal has one of two possible frequencies f L = fc − 1 4T and fU = f c + 1 4T The difference between these frequencies is ∆f = f U − f L = 1 2T . This is the minimum frequency separation to ensure orthogonality between two co-phased sinusoids of duration T and, hence, the name minimum shift keying. By viewing figure 15 this type of modulation can be thought of as a special case of OQPSK in which the rectangular waveform is replaced by a sinusoidal pulse, which is shown in figure 11. Figure 16 Performance of different CPFSK signals Figure 16 shows performances of different CPFSK signals compared to MSK. By increasing the number of levels, the bandwidth efficiency is increased clearly. 4.5.3 Partial Response CPM Partial response CPM signals have a frequency shaping pulse hf(t) with duration LT where L > 1. Partial response signals have better spectral characteristics than full response CPM signals, i.e., a narrower main lobe and faster roll-off of side lobes. Lars.maura@hut.fi 20(39) 63RVWJUDGXDWH6HPLQDULQ5DGLR&RPPXQLFDWLRQV 5 Digital Modulation Trade-Offs Any digital modulation aims at realising the best possible trade-off in a given situation among the bit error probability Pb(e), the bandwidth efficiency Rs/W, the ratio εb/N0 and the complexity of the equipment. Following results are taken from Benedetto [3]. Figure 17 Comparison of different modulation methods on the bandwidth-efficiency plane for -5. a bit error probability Pb(e) = 10 A comparison of different modulation methods is illustrated in figure 17 where a bit error probability Pb(e) =10-5 has been fixed. The Shannon capacity bound shows the maximum bandwidth efficiency, which can teoretically be achieved. The graph shows the fact that amplitude modulation (ASK), and phase modulation (CPSK and DCPSK) systems are bandwidth-efficient signalling techniques, since they cover the region of the plane where Rs/W > 1. In this region, the system bandwidth is limited and it can be traded for power (i.e. εb/N0). In fact, for a fixed bandwidth, the bandwidth efficiency can be increased with an increase in the number of levels M. The price paid to achieve the same Pb(e) is an increase in εb/N0. On the other hand, FSK signals make an inefficient use of bandwidth, since they cover the region of the plane where Rs/W < 1. But these systems trade bandwidth for a reduction of the εb/N0 required to achieve the same Pb(e). Lars.maura@hut.fi 21(39) 63RVWJUDGXDWH6HPLQDULQ5DGLR&RPPXQLFDWLRQV Litterature [1] Stüber, G. Principles of Mobile Communication. Second edition. Norwell, Massachusetts, USA. Kluwer Academic Publishers. 2001. p. 751. [2] Lee, E.A. Messerschmitt, D.G. Digital Communication. Second edition. Norwell, Massachusetts, USA. Kluwer Academic Publishers. 1994. p. 893. [3] Benedetto, S. Biglieri, E. Castellani, V. Digital Transmission Theory. Englewood Cliffs, New Jersey, USA. Prentice-Hall, Inc. 1987. p. 639. Lars.maura@hut.fi 22(39)