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Reprint from<br />

PROCEEDINGS<br />

of the IEEE 69<br />

November l981<br />

pp. 1419--1450<br />

<strong>HELMUT</strong> <strong>SCHEUERMANN</strong><br />

<strong>AND</strong> <strong>HElNZ</strong> <strong>GOCKLER</strong>


PROCEEDINGS OF THE IEEE, VOL. 69, NO. 11, KWEMBER 1981<br />

<strong>HELMUT</strong> <strong>SCHEUERMANN</strong> <strong>AND</strong> HEINZ aCKLER<br />

Abstract-With this survey, an attempt is made to describe the pat<br />

majority of all known methods of digital transmultiplexing (Le., conversion)<br />

of time-division-multiplex (TDM) to frequency-divisionmultiplex<br />

(FDM) signals, and vice versa. To this end, the individual<br />

transmultiplexer approaches are classified into four categories according<br />

to the undedying algorithm: Bandpass filter bank, low-pass filter<br />

bank, Weaver structure method, and multistage modulation method.<br />

Finally, the overall performance of the various transmultiplexer approaches<br />

are compared with each other by means of different criteria<br />

[l], such as stability un<strong>der</strong> looped conditions, absolute value of the<br />

group delay, computational and control complexity, modularity, potential<br />

of intelligible crosstalk, absence of an additional analog frequency<br />

conversion, and the impact of out+£-band signaling. For a more profound<br />

un<strong>der</strong>standing of the individual digital transmultiplexer approaches,<br />

the main chapter is preceded by an introductory discussion<br />

on analog and digital generation of single-sideband signals. In this<br />

context, the associated problems of sample rate alteration and multirate<br />

filtering arising f~om digital signal processing are dealt with.<br />

Manuscript received February 8, 1980; revised July 30, 1981. This<br />

work was supported in part by the German Fe<strong>der</strong>al Ministry of Research<br />

and Technology.<br />

The authors are with the Advanced Development Department, AEG-<br />

Telefunken Kommunikationstechnik, P.O.B. 1120, D-71 50 Backnang,<br />

Germany.<br />

I. INTRODUCTION<br />

A<br />

NALOG TRANSMISSION and switching facilities for<br />

telephony signals are nowadays to a growing extent<br />

being expanded and replaced by digital facilities.<br />

Thereby the conventional multiple utilization of transmission<br />

paths. by frequency-division-multiplex (FDM) is being substituted<br />

by time-division-multiplex (TDM) techniques. The<br />

chief advantages of digital TDM transmission as compared with<br />

analog FDM transmission are as follows:<br />

1) no generation of additive noise on the transmission<br />

path;<br />

2) within certain limits, no occurrence of interference<br />

through crosstalk;<br />

3) possibility for concentration of switching and transmission<br />

facilities.<br />

The widespread use and high investment outlays of the<br />

installed facilities will require that analog and digital technologies<br />

coexist well into the foreseeable future. This will lead to<br />

an increasing extent to interfaces between analog and digital<br />

sections of the toll communication network. Interconnection


PROCEEDINGS OF THE IEEE, VOL. 69, NO. 11, NOVEMBER 1981<br />

FDM:<br />

FDM<br />

Frequency Division<br />

Multiplex<br />

SG : Supergroup<br />

PDM : Time Divi<br />

Multiplex<br />

sion<br />

Fig. 1. Block diagram of a 60-channel transmultiplexer. (a) TDM-FDM<br />

direction. (b) FDM-TDM direction.<br />

at these places could be made, in principle, using the available<br />

FDM and TDM terminal-station equipment. In doing so, the<br />

process goes-for instance, when converting from the analog<br />

to the digital signal representation-from the particular FDMcarrier<br />

hierarchy stage down to the voice frequency level and<br />

proceeds from there to the corresponding TDM hierarchy stage.<br />

Better system performance and a more economical solution<br />

may be achieved with an interfacing facility specially designed<br />

for this purpose. For such facility, the designation "transmultiplexer"<br />

has been coined.<br />

Signal processing in a transmultiplexer can be done either in<br />

the analog or in the digital way. As compared with analog<br />

technology, digital technology offers the advantages of being<br />

suited for integration, and of the absence of circuit adjustment<br />

and variation of equipment performance with time and temperature,<br />

etc.<br />

A great number of publications on digitally implemented<br />

transmultiplexers appeared over the last years [ 1 ]-[7].<br />

With<br />

the increasing number of transmultiplexing methods' being<br />

disclosed, it becomes ever niore difficult to maintain an overview<br />

and, for given conditions, to choose a suitable approach.<br />

It is therefore the aim of this contribution to describe the fundamental<br />

algorithms in a tutorial manner, to point out the<br />

common features of the individual known transmultiplexer<br />

approaches and to classify these methods according to the<br />

inherent digital signal processing procedures. To this end, the<br />

functions of individual subassemblies of a transmultiplexer are<br />

explained in the next section. For a deeper un<strong>der</strong>standing of<br />

digital transmultiplexer algorithms, the possibilities of analog<br />

single-sideband modulation are recalled and, in addition, extended<br />

to digital signal processing in the subsequent sections.<br />

Particularly, the questions of sample rate alteration and multirate<br />

filtering (interpolation, decimation) are treated in detail.<br />

In the main section, the individual known transmultiplexer approaches<br />

are classified into four categories according to the<br />

un<strong>der</strong>lying algorithm: Bandpass filter-bank method, low-pass<br />

fiiter-bank method, Weaver structure method, and multistage<br />

modulation methods. Finally, in the concluding sections, the<br />

various transmultiplexing methods described in this paper are<br />

compared with each other on the basis of a set of criteria<br />

essentially introduced by Fettweis [ 1 1.<br />

In its basic function, a transmultiplexer represents a singlesideband<br />

modulator. As an example for the European format,<br />

Fig. 1 shows the functional block diagram of a 60channel<br />

transrnultiplexer for the TDM-FDM-direction (Fig. l(a)) and<br />

for the FDM-TDM-direction (Fig. l(b)): The data streams of<br />

two PCM TDM systems, each of them comprising 30 telephone<br />

channels corresponding to the lowest European TDM hierarchical<br />

level (PCM 30), are simultaneously translated to the<br />

FDM supergroup (SG) level in the frequency range from 3 12<br />

kHz to 552 kHz, and vice versa [ 11, [2]. In contrast to that,<br />

in North America and Japan the lowest hierarchy of the TDM<br />

system is made up of only 24 telephone channels. Un<strong>der</strong> these<br />

constraints, a transmultiplexer is generally applied to the conversion<br />

of one 24channel PCM TDM data stream to two<br />

(primary) groups of the FDM hierarchy, each of them comprising<br />

12 channels in the frequency band ranging from 60 to<br />

108 kHz, and vice versa [ l], [2]. Moreover, in Japan some<br />

attempts have been made to realize a 120-channel transmultiplexer,<br />

corresponding to an interface between five 24-channel<br />

PCM TDM formats and two FDM supergroups [ l], [8], [9].<br />

Subsequently, however, the more general discussion will predominantly<br />

be based on the 60channel approach. Nevertheless,<br />

North American and Japanese 24-channel transmultiplexers<br />

(which can usually be adapted to another number of<br />

channels without difficulty) will be consi<strong>der</strong>ed in the main<br />

chapter as well. On the contrary, facilities, such as those required<br />

for signaling, dialing pulses conversion, and supervision<br />

will only be treated marginally, since they have no bearing on<br />

the un<strong>der</strong>standing of the basic principles of operation. The<br />

interested rea<strong>der</strong> is referred to [75], [76].<br />

In the European approach, the two PCM TDM bit streams<br />

(PCM 30), each with a transmission speed of 2.048 Mbitls, are<br />

applied to a receiver R (Fig. l(a)). Here, the two TDM signals


<strong>SCHEUERMANN</strong> <strong>AND</strong> <strong>GOCKLER</strong>: DIGITAL TRANSMULTIPLEXING METHODS 1421<br />

TABLE I<br />

equipment are compiled in the CCITT Recommendation<br />

SOME SPECIFICATIONS FOR 60-CHAXNEL TRANSMULTIPLEXERS ACCORDING G.792. In addition, some general consi<strong>der</strong>ations on trans-<br />

TO CCIn RECOMMENDATION G. 792 <strong>AND</strong> G. 793<br />

multiplexers can be taken from the CCITT Recommendation<br />

Magnitude rcsponsc *<br />

G.791, whereas the particular specifications of a 60channel<br />

transmultiplexer, such as pilots, signaling, etc., can be found in<br />

6WHz to 2LOOHz -0.6dB 5 a 50.6dB<br />

the CCITT Recommendation G.793. From these recommenda-<br />

Maximum allowancc at thr band edges<br />

tions, the most important requirements for a 60channel trans-<br />

300 Hz -0.6dB r a C 1.7dB multiplexer are given in Table I. It must be noted that these<br />

3400 Hz -0.6dB 5 o S 2.LdB<br />

data are, in general, to be measured at the analog (FDM) ports,<br />

the digital (TDM) ports being looped. As a consequence, the<br />

Group delay * (absolute value) T C 3ms<br />

actual constraints to be imposed on any individual filter of a<br />

transmultiplexer may be much more stringent. Furthermore,<br />

Distortion<br />

1000 Hz to 2600Hz AT 4 0Sms<br />

the individual filter specifications are generally different for<br />

the various transmultiplexing methods to be described in the<br />

sequel.<br />

600 Hz to l000 Hz AT a 1.5n-s<br />

504 Hz to 600Hz, 2600Hz to 28WHz AT C 2ms<br />

Minimum crosstalk attenuation bctwccn any two channcls*<br />

Intclligiblc crosstalk 65 dB<br />

Unintelligible crosstalk 58dB<br />

Maximum idle channcls noisc with all channcls loadad<br />

cxccpt thc one measured. rrtcrcncrd to peak signal<br />

point *<br />

- 8OdB<br />

Maximum in - band r ms nonlinear distortion, rrtcrcncrd<br />

to peak signal point * -40dB<br />

Out -of - band signalling at 3825Hz<br />

Ptlot frtqumcics at 3 920Hz<br />

From the theory of analog signal processing, three basic<br />

methods are known for producing a single-sideband signal.<br />

These methods are described at length in an overview paper of<br />

Kurth [ 121, for which reason the principles will only briefly<br />

be touched upon here. All three methods use for frequency<br />

translation a type of doublesideband amplitude modulation.<br />

The differences lie in the sequential or<strong>der</strong> of modulation and<br />

sideband suppression, as well as in the method of sideband<br />

suppression itself. Mathematically, the single-sideband signal<br />

may be expressed by means of analytical signals<br />

y,(t) = x(t) cos 2rfCt - 2(t) sin 2nfct<br />

where<br />

y,(t) = x(t) cos 2n fc t + 20) sin 2nfc t<br />

(la)<br />

*Measurement of the multiplexed analog signal, the digital ports being<br />

looped.<br />

are synchronized, and the particular signal levels are adjusted<br />

so as to enable a subsequent digital processing. This is followed,<br />

for each of the branches, by a serial-parallel (SIP) converter,<br />

which converts the interleaved TDM signals to parallel<br />

form. The samples, in Europe encoded according to the A-law<br />

[10], are converted in the expan<strong>der</strong> (EX) to linearly encoded<br />

samples. Subsequently, the FDM signal is digitally generated<br />

by means of a bank of single-sideband modulators (SSB-MOD).<br />

A digital-to-analog (D/A) converter, followed by an analog<br />

filter for smoothing the resulting staircase function, produces<br />

the desired FDM signal at the supergroup level.<br />

If we consi<strong>der</strong> the operations of Fig. l (a) in reverse sequence,<br />

we obtain the FDM-TDM conversion shown in Fig. l(b). In<br />

general, the frequency- to time-division-multiplex conversion<br />

may be <strong>der</strong>ived from the TDM to FDM conversion by transposition<br />

[ 1 1 l. For this reason, we can limit ourselves in the<br />

following to the various methods of producing singlesideband<br />

signals; thus, only the subassembly SSB-MOD will be treated<br />

in detail. Suffice to say that a North American or Japanese<br />

24-channel PCM TDM to FDM group-band translator (with a<br />

bit rate of 1.544 Mbit/s and inherent p-law companding [10])<br />

is made up of the same building blocks as a 60channel transmultiplexer<br />

according to Fig. 1.<br />

The remaining questions to be consi<strong>der</strong>ed in this section are<br />

primarily concerned with allowed signal irnpairnients-noise,<br />

crosstalk, phase, and frequency distortion, and nonlinear distortion.<br />

The requirements common to all transmultiplexing<br />

represents the Hilbert transform of the input signal x(t) and<br />

fc the carrier frequency. Equation (la) denotes the upper<br />

sideband and (lb) the lower one.<br />

A. Hartley S Method [13]<br />

The immediate implementation of (1) leads to the Hartley's<br />

method. The input signal is modulated onto the carrier<br />

cos 2rfct and the Hilbert transform of the input signal onto<br />

the orthogonal camer sin 21Tfct. After that, the two branch<br />

signals are subtracted from or added to each other, depending<br />

on whether the translated spectrum so produced is to be noninverted<br />

or inverted.<br />

Fig. 2(a) depicts the principle of implementation of this<br />

method and Fig. 2(b) the associated frequency spectra, from<br />

which the operating principle becomes clear. The unwanted<br />

sideband is cancelled by compensation.<br />

A practical implementation of this method is shown in Fig. 3.<br />

In this case, two signals, shifted in phase through all-pass networks<br />

by n/2 with respect to each other, are <strong>der</strong>ived from the<br />

input signal.<br />

B. Weover S Method (2 41<br />

The baseband signal is first translated by means of an auxiliary<br />

carrier (Fig. 4(a)), whose frequency normally Lies in the<br />

center of the usable band (Fig. 4(b)). Figs. 4(c) and (d)<br />

depict the corresponding frequency spectra for in phase and<br />

quadrature signals upon this translation. The low-pass filters<br />

that follow (LP in Figs. 4(a), (e) suppress the spectral compo-


PROCEEDINGS OF THE IEEE, VOL. 69, NO. 11, NOVEMBER 1981<br />

I cos ZTtf,t<br />

(b)<br />

Fig. 2. Singlesideband modulation according to Hartley's method.<br />

f<br />

cos 2KfCt<br />

l<br />

sin ZTCfCt<br />

Fig. 3. Modified SSB-MOD according to Hartley.<br />

nents for f > If0 I (Figs. 4(f), (g)). This is subsequently followed<br />

in each branch by a translation into the ultimate frequency<br />

band (Figs. 4(h), (i)). Through addition of the two<br />

signals X gi(t) and X 3q (t) (Fig. 4(a)), the frequency components<br />

within the useable frequency band are compensated in<br />

such a way that the desired single-sideband signal is produced<br />

(Fig. 46)).<br />

C. Filtering Method<br />

The oldest and in analog signal processing normally used<br />

method is the double-sideband amplitude modulation with<br />

subsequent suppression of the unwanted sideband (Fig. 5). As<br />

filter, either a low-pass or a high-pass filter may basically be<br />

used, depending on whether the noninverted or inverted signal<br />

Fig. 4. Single-sideband modulation according to Weaver's method.<br />

spectrum is desired. In general, however, modulation products<br />

of nonideal modulators have to be filtered out, so that a bandpass<br />

filter must be used.<br />

IV. DIGITAL SINGLE-SIDEB<strong>AND</strong> MODULATION<br />

The principles of singlesideband modulation outlined for<br />

analog systems in the preceding section can also be used with<br />

digital signal processing. The frequency spectra are now<br />

periodic with the sampling frequency fAY (Fig. 6(a)).<br />

For estimation of the total amount of digital circuitry, the<br />

following consi<strong>der</strong>ations concerning implementation are made.


<strong>SCHEUERMANN</strong> <strong>AND</strong> <strong>GOCKLER</strong>: DIGITAL TRANSMULTZPLEXING METHODS 1423<br />

Fig. 7. Digital FDM signal.<br />

The amount of circuitry, particularly the number of arithmetic<br />

operations, that would arise if such a transmultiplexer were to<br />

be implemented, is so overwhelming that any further consi<strong>der</strong>ation<br />

is superfluous [ 151.<br />

If efforts to process the digital signals at lower sampling rates<br />

should prove to be successful, drastic savings could be achieved<br />

for the following reasons:<br />

2 Lowpass attenuation 1<br />

Highpass attenuation<br />

X (11 : Premodulation 1 baseband spectrum 1<br />

YE If) : Two sidcband amplitude modulation<br />

Yu(f):<br />

Single sideband spectrum (noninverted position1<br />

Y, If): Single sideband spectrum {inverted position)<br />

Fig. 5. Single-sideband modulation according to filtering method.<br />

1) the amount of arithmetic operationsltime is smaller;<br />

2) the degree of the necessary filters is reduced since the<br />

relative width of the transition band is expanded.<br />

If these consi<strong>der</strong>ations are pursued consequently, the minimum<br />

expenditure will be reached if each channel signal is<br />

processed just with the lowest possible sampling frequency according<br />

to the Sampling Theorem [ 161. In or<strong>der</strong> to be able to<br />

produce the FDM signal, the sampling frequency must subsequently<br />

be increased, requiring special interpolators. These<br />

interpolating networks wiU be treated in more detail in the<br />

next section.<br />

If the sampling rate of a sequence is to be increased, additional<br />

sampling values must be inserted. If the sampling rate is<br />

to be increased by an integer factor M, the new sampling interval<br />

becomes<br />

is =<br />

(c)<br />

Fig. 6. Digital singlesideband modulation.<br />

= sampling frequency<br />

If it is desired to form the FDM signal (Fig. 7) of, say, a 60-<br />

channel transmultiplexer, a bank of 60 singlesideband modulators<br />

would be required. If the signal bandwidth of a single<br />

channel is assumed to be BK = 4 kHz, the FDM signal needs a<br />

bandwidth of (cf., Fig. 7)<br />

To be able to perform analog filtering after the D/A converter<br />

(Fig. l), an unconstrained transition band has to be provided.<br />

Approximately fSp = 16 kHz are assumed for this band, yielding<br />

an analog filter of tractable or<strong>der</strong>. Since, according to the<br />

Sampling Theorem the sampling frequency has to be at least<br />

double the maximum signal frequency, the sampling frequency<br />

is (cf., Fig. 7)<br />

where To is the reciprocal of the original sampling frequency.<br />

Each Mth sample of the new sequence is taken over from the<br />

sequence to be interpolated; M - 1 new samples are inserted<br />

inbetween. Two methods for solving the interpolation problem<br />

are outlined in the following (a more detailed treatment<br />

can be found in [92]).<br />

A. Interpolation by Low-Pass Filtering<br />

The time-continuous signal ?(t) is assumed to have the<br />

frequency spectrum X(w) (Fig. 8(a)), which shall be band<br />

lifited according to<br />

2(0)=0, for 101 > ug.<br />

The signal i(t) is sampled with the sampling frequency<br />

fSo = l/To assuming the Sampling Theorem to be met. Due to<br />

the sampling process the spectrum of i(t) is periodically repeated<br />

on the frequency axis (Fig. 8(b)), yielding<br />

Starting with the sequence {~(VT~)} the sequence<br />

(xH(vTo/~)) is to be approximated by interpolation. This<br />

sequence could be obtained by sampling the time-continuous<br />

signal x(t) with sampling frequency fSH = M/To increased by


PROCEEDINGS OF THE IEEE, VOL. 69, NO. 11, NOVEMBER 1981<br />

Fig. 8. Frequency spectra resulting from increasing the sampling<br />

frequency by a factor of M.<br />

*<br />

0 T 2T t<br />

y(VT)* x(VMT-iT) M c HI<br />

150<br />

Fig. 9. Generation of the sequence {JJ(VT)} from .M sequences with<br />

sampling interval MT (example M = 8).<br />

Fig. 10. Polyphase network for sampling rate increase.<br />

the factor M compared with the sampling process of (3). As<br />

corresponding spectrum we get<br />

M +-<br />

In accordance with the increased sampling frequency the<br />

period of the frequency spectrum is increased by a factor of<br />

M (Fig. 8(d)). Digital interpolation can be interpreted as a<br />

low-pass filtering process where the signal is to be amplified by<br />

XH(u) = - C X(W + MiuSO). (4) a factor of M (Fig. 8(c)). The unwanted spectral components<br />

To i=--<br />

(cf., Figs. 8(b) and (d)) are suppressed; in this way, the spec-


<strong>SCHEUERMANN</strong> <strong>AND</strong> <strong>GOCKLER</strong>: DIGITAL TRANSMULTIPLEXING METHODS<br />

-,j<br />

-815 G<br />

-l<br />

-r<br />

L----<br />

I------,<br />

I----- @<br />

-wn 1<br />

.-.-.<br />

L.. -. .... .,<br />

L ----. _ 4<br />

I : . . ; r -+<br />

1<br />

Fig. 11. Phase cancellation process in a polyphase network for interpolation<br />

(M = 5).<br />

trum XH(w) is approximated. An exact and detailed description<br />

of this process can be found in [17], [181, [92].<br />

B. Interpolation by Phase Compensation<br />

For a simple explanation of the phase cancellation process<br />

M - l sequences {X~(VMT)) are <strong>der</strong>ived from the sequence<br />

{X~(VMT)} with the sampling interval To = MT in such a way<br />

that the sequences result from each other by successive phase<br />

shifts corresponding to the time interval T (Fig. 9).<br />

All these subsequences are interleaved to produce the interpolated<br />

output sequence ~(vT)), sampled at the M times<br />

higher rate M/To = l/T. The corresponding network structure<br />

is shown in Fig. 10, where the summing point represents the<br />

interleaving process. As mentioned in the preceding section,<br />

the desired interpolation values to be inserted can only be<br />

produced if the polyphase network as a whole (Fig. 10)<br />

exhibits a low-pass characteristic corresponding to Fig. 8(c),<br />

[ 191, [ 201. From Fig. 9 it is obvious that the signal sequences<br />

in the individual branches of the polyphase network (Fig. 10)<br />

can be processed at the lower input sampling rate l/MT=<br />

l . Furthermore, it will be shown that any rational<br />

(low-pass) transfer function for decimation or interpolation<br />

can be processed at the lower input sampling rate l/(MT) =<br />

tation according to Fig. 10.<br />

If each branch filter is provided with the all-pass characteristic<br />

H? = eioi shown in Fig. 11, the following output spectrum<br />

is obtained (a = 27~Tf):<br />

Range<br />

(b)<br />

Fig. 12. (a) Decomposition of branch allpass networks. (b) Polyphase<br />

structure for interpolation.<br />

since<br />

j(anp)i = (summation orthogonality of<br />

2 trigonometric functions)<br />

i=O<br />

This represents ideal low-pass filtering according to Fig. 8.<br />

The representation of Fig. 11 permits a different <strong>der</strong>ivation of<br />

the low rate signal processing in the polyphase network: The<br />

phase characteristics of the branch filters can be decomposed<br />

in a linear component Gli and in a component periodic<br />

with 1/MT (Fig. 12(a)). The linear component can be<br />

realized by delays; solely the periodic component has to be<br />

realized by all-pass networks H ~(z~) (Fig. 12(b)). Note that a<br />

reference filter in the zeroth branch of the polyphase network<br />

(Fig. 12(b)), a prerequisite for realizability, is omitted for<br />

convenience.<br />

C. Digital Signal Interpolation in Conjunction<br />

With Filtering [l 91<br />

Each sequence f~(v)) whose unilateral z-transform


1426 PROCEEDINGS OF THE IEEE, VOL. 69, NO. 11, NOVEMBER 1981<br />

exists, can be expressed by N interleaving sequences<br />

In it, the expression<br />

N-l<br />

Y(z) = C z-" y(zN, n). (6<br />

n =O<br />

where<br />

and<br />

h (0) = lim H(z)<br />

Z-+ m<br />

(1 lb)<br />

R, = h (z - z,,)[H(z) - h(O)]. (I lc)<br />

m<br />

Z'zmm<br />

y(zN, n) = 2 ~ (VN + n) z - ~ (7) For the <strong>der</strong>ivation of the branch filters H,(z~) from the polyv=o<br />

nomial form according to (9), a method can be found in [l 91.<br />

represents the z-transform of the subsequences. This process is However, a general closed form solution cannot be given. For<br />

visualized by writing the terms of the sequence as follows: this reason, the form c according to (l l) is used in the follow-<br />

~(vT)) = ~ (0)<br />

Y (NI<br />

Y(2W<br />

Y (3N)<br />

N sibseqgences<br />

with sampling ~(vN))<br />

interval N T<br />

z-transforms of<br />

subsequences<br />

y(zN><br />

This results in the following. The fdtering process of a se- ing. Here, one obt@ns after a tedious but straightforward<br />

quence with the sampling interval T can be reduced to fdtering calculation<br />

of N sequences having a sampling interval of N - T (Fig. 13).<br />

Evidently, the transfer function of the polyphase network is M R, 2;l<br />

H, (zN) = h(0) + C<br />

(12)<br />

(Fig. 13)<br />

m = I P - 2 m<br />

Starting with (g), the question arises how to get the transfer<br />

functions of the individual branch filters Hn(zN) in or<strong>der</strong> to<br />

realize a given transfer function H(z). For this purpose H(z)<br />

may be expressed in one of the following three equivalent<br />

forms which can, if necessary, be transformed from each other<br />

l211<br />

a) Polynomial Form<br />

uk'<br />

k=O<br />

H(z)= where K


<strong>SCHEUERMANN</strong> <strong>AND</strong> <strong>GOCKLER</strong>: DIGITAL TRANSMULTIPLEXMG METHODS 1427<br />

For better un<strong>der</strong>standing of this method, we set out from<br />

the model that each branch with the bandpass filter transfer<br />

function H,(z) with complex coefficients3 (Figs. 14(a), (c),<br />

(d), (e)) is replaced by an interpolating filter for generation<br />

of the high sampling rate fS = 1/T, followed by a SSB-MOD.<br />

Moreover, by means of these interpolating filters analytic<br />

baseband signals, i.e. signals with suppressed power spectrum<br />

in the frequency interval (-fS, O), have to be <strong>der</strong>ived from the<br />

real-valued input sequences {x,(vNT)}. Hence, as outlined in<br />

the preceding section, the individual bandpass filters may be<br />

composed of a polyphase network with complex coefficients<br />

and a SSB-MOD (Fig. 14(h)). Thus the following formula<br />

applies:<br />

Fig. 13. Filtering by polyphase network.<br />

analysis and synthesis [26]-[29], as well as for spectral an&-<br />

sis [221, [3O], [31]. Clearly, the algorithms then are adapted<br />

to the specific problems to be solved. Note, however, that we<br />

Limit ourselves to transmultiplexing applications. To this end,<br />

in this section, the transmultiplexing algorithms are classified<br />

into four groups. These are: bandpass filter-bank, low-pass<br />

filter-bank, Weaver structure, and multistage modulation<br />

methods.<br />

A. Bandpass Filter-Bank Method<br />

The frequency spectrum of' the TDM input sequence<br />

{x,(uNT)} (cf., Fig. 14(b)) exhibits the following characteristics:<br />

assuming a complex-valued output sequence G~(T)). Thereby<br />

the polyphase network realizes the frequency response<br />

~ ~ ( ein i all ~ branches ) according to Fig. 14(a). The subsequent<br />

single-sideband modulator causes the corresponding<br />

frequency translation along the frequency axis. From (8)<br />

f 0110 ws<br />

According to the modulation theorem of the z-transform the<br />

ideal complex single-sideband modulation is represented by<br />

substitution of the variable<br />

&(z) is thus obtained from H;(Z) by<br />

2) Frequency response has Hermitian symmetry, ie.,<br />

~,(~iznTfN) = X,*(e-i2"TfN) (15)<br />

(* denotes "conjugate complex").<br />

Starting with a TDM-sequence according to (14) and (IS)<br />

the corresponding FDM signal may be gained by suitable filtering<br />

in a bandpass filter bank (Fig. 14(a)). Such a bank consists<br />

of N bandpass filters, whereby the passband range of the<br />

individual bandpass filters is shifted by the frequency l/(NT)<br />

with respect to each other (Figs. 14(c), (d), (e)). The output<br />

signals of the bandpass filter bank are combined by an ad<strong>der</strong>,<br />

thus forming the FDM signal. For all channels with<br />

r E [N/2, N - l], the resulting spectra are in the inverted<br />

position. If these signals are subjected beforehand to a doublesideband<br />

amplitude modulation with fs/2 = 1/(2T) as carrier<br />

frequency, the desired position of the frequency spectrum<br />

will be obtained. This modulation process is particularly<br />

simple, since it can be performed by multiplication with the<br />

sequence<br />

The FDM signal then exhibits the correct frequency position<br />

for all channels. In the sequel, this inversion process will no<br />

longer be mentioned explicitly.<br />

2 represents the set of integer numbers.<br />

According to (16) the real single-sideband signal is obtained<br />

by<br />

For better un<strong>der</strong>standing, the complex SSB-MOD is depicted<br />

symbolically in Fig. 14(i). Using (17) and (18), there follows:<br />

since e-jZar = 1 because of r €N.<br />

Since the same transfer function &(z) (Fig. 14(h)) is generated<br />

in each filter branch r (Fig. 14(a)), the following relation<br />

holds:<br />

Inserting equations (19) and (20) into (16), we obtain for the<br />

3Complex signals and transfer functions with complex-valued coefficients<br />

are indicated by boldface letters and un<strong>der</strong>lined in the figures.


PROCEEDINGS OF THE IEEE, VOL. 69, NO. 11, NOVEMBER 1981<br />

(€9<br />

Fig. 14. Bandpass fdter-bank method.<br />

real-valued output signe<br />

Interchanging the sequential or<strong>der</strong> of summation and rearranging<br />

yields<br />

The term<br />

represents the inverse discrete Fourier transform (IDFT) for<br />

N points at the I/(NT) sampling rate. We thus.obtain from<br />

(21)<br />

N-l<br />

Y(z) = C z-" 2 Re L~n(zN) - IDFT { xr(P) )l (22)<br />

n=O<br />

from which the block diagram in Fig. 15 can be <strong>der</strong>ived. The<br />

filters H,(z~) with complex coefficients process complexvalued<br />

input signals. From the output signal, only the real<br />

part is needed.<br />

The transmultiplexers described by Terrell and Rayner [32],<br />

Maruta and Tomozawa [8], [g], [33], [34] as well as by<br />

Takahata et al. 1351 work in accordance with the bandpass<br />

filter-bank method treated above.<br />

If the number of channels is specifically fixed to


<strong>SCHEUERMANN</strong> <strong>AND</strong> <strong>GOCKLER</strong>: DIGITAL TRANSMULTIPLEXING METHODS<br />

(i)<br />

Fig. 14. (Continued).<br />

TDM - signal<br />

sampling rate<br />

R, = real part<br />

I, = imaginary part<br />

1<br />

m<br />

Fig. 15. Block diagram of transmultiplexer according to the bandpass<br />

filter-bank method (see (22)).<br />

FDM- signal<br />

where<br />

the described transmultiplexer method may be decomposed<br />

into subunits consisting of transmultiplexer~, each of them<br />

processing $I input signals. The total number of subunit transmultiplexers<br />

is then<br />

N N N N<br />

+p"-


PROCEEDINGS OF THE IEEE, VOL. 69, NO. 11, NOVEMBER 1981<br />

,<br />

spectral inversion<br />

2 point lDFT<br />

Fig. 16. Transmultiplexer for N = 2 channels according to the bandpass<br />

ffiter-bank method.<br />

Using (23), s becomes<br />

The simplest transmultiplexer is obtained for p = 2. From (21)<br />

results<br />

Since in this particular case (N = 2), no imaginary parts occur<br />

in the discrete Fourier transform, we obtain the block diagram<br />

shown in Fig. 16. Hence, H,(Z~) and H~ (z2) represent filters<br />

with real coefficients.<br />

If N is chosen such that<br />

the entire transmultiplexer may be constructed from stages<br />

according to Fig. 16. By combining the processors of all subunits<br />

to an overall processor, we obtain a "Hadamard processor."<br />

Within this processor only trivial multiplications with<br />

plus or minus one have to be carried out. A transmultiplexer<br />

according to this principle has been proposed by Qaasen and<br />

Mecklenbrauker [3 6 1.<br />

Furthermore, there exist other methods mechanizing a bandpass<br />

filter-bank in the frequency domain. They are based on<br />

fast convolution techniques applying fast Fourier transforms<br />

(FFT) [37], [38] or number theoretic transforms (NTT) [39],<br />

[40]. However, these methods seem to be less suitable due to<br />

their inherent time delay, caused by block processing of the<br />

incoming sequences. A transmultiplexing algorithm in which<br />

the bandpass filter-bank is implemented via fast convolution<br />

techniques is presented by Constantinides and Valenzuela<br />

[41]. Sophisticated simplifications were made to reduce the<br />

computational load, for instance, by taking FIR filters. To<br />

meet the specifications (60-dB minimum stopband attenuation,<br />

passband gain accuracy k0.5 dB), which do not comply with<br />

the CCITT Recommendations according to Table I, a linear<br />

phase FIR filter degree of about 1760 is needed for a 60-<br />

channel transmultiplexer. In conjunction with the minimum<br />

block length this leads to a (looped) group delay of greater<br />

than 3 ms (cf., Table 11). Moreover, it is conjectured that even<br />

with the application of minimum phase FIR filters a group<br />

delay of less than 3 ms cannot be reached.<br />

Most recently, a modulator-free and multiplier-free transmultiplexer<br />

approach was proposed by Kurth et al. [81 I, [821.<br />

It resumes the most obvious idea of directly selecting the<br />

desired frequency band, for instance of the periodic input<br />

spectrum of the TDM signal (TDM-to-FDM), at' the group or<br />

supergroup level by means of a single filter per channel-a<br />

method which has so far been abandoned due to its extremely<br />

high computational load (cf., [ 15, ch. 41 ). The per-channel<br />

processor uses minimum-phase FIR filters which also perform<br />

interpolation (TDM-to-FDM) and decimation (FDM-to-TDM).<br />

Hardware efficiency, which can hardly be compared with that<br />

of other approaches, is obtained by implementing the FIR filters<br />

in a logarithmic mode, wherein multiplication becomes<br />

addition. Lookup tables, in form of memoxy, perform conversion<br />

between the logarithmic and linear formats.<br />

A similar transmultiplexer with conventional digital filters<br />

processing complex (analytic) instead of real signals was proposed<br />

by Del Re [83]. Before feeding the input sequences to<br />

the complex filter-bank on a per-channel basis, the analytic<br />

signals are generated by means of a phasesplitting network<br />

(Hilbert filter).<br />

B. Low-Pass Filter-Ban k Method<br />

If one succeeds in obtaining real signals at the output of the<br />

Fourier processor, processing of "complex" signals in the poly- .<br />

phase network can be avoided. The output signals of a Fourier<br />

processor are real if the complex input signals exhibit<br />

Hermitian symmetry. Assuming a 2Wpoint DFT processor,<br />

the following relation must hold for the complex input signals:<br />

For a 2N-point inverse discrete Fourier transform, the following<br />

holds:<br />

Using (26), equation (27) may be factored into<br />

Applying the variable transformation<br />

to the second term of (28) yields<br />

Thus there results from (28), if in its first term r is replaced


<strong>SCHEUERMANN</strong> <strong>AND</strong> <strong>GOCKLER</strong>: DIGITAL TRANSMULTIPLEXING METHODS<br />

TABLE I1<br />

COMPARISON OF THE ~NDIVIDUAL TRANSMULTIPLEXER APPROACHES<br />

1) GROUP DELAY MEASURED AT THE ANALOG PORTS, THE DIGITAL<br />

PORTS BEING LOOPED 2) PELLONI'S FILTER BANK (POLYPHASE NETWORK)<br />

Transmult~plexer<br />

approach<br />

Tcrrell W75 [32]<br />

Maruta 1976 [33]<br />

lakahata 1978<br />

[3L,35]<br />

:loam 1978 [36]<br />

Aoyama 1980 [ 8,9 1<br />

Constantinides 1980 [L11<br />

hdul. scheme,<br />

40 of chan~ls:<br />

jingle -way IS)<br />

'WO-way IT)<br />

bltiple-way (M1<br />

M 12 (2LI<br />

M M)<br />

M 12 (24<br />

Group<br />

delay '1<br />

?<br />

2.3ms<br />

> 3rns ?<br />

?<br />

2.3ms<br />

-3ms<br />

Operation<br />

rate lchmtl<br />

[l/sI<br />

Degree<br />

of<br />

modularity<br />

IOW<br />

l ow<br />

low<br />

~ d i u m<br />

low<br />

low<br />

Analog<br />

frequency<br />

cowersion<br />

Yes<br />

M<br />

no ISG: yes)<br />

Yes<br />

no<br />

Yes<br />

Rocessing<br />

of<br />

out - of -band<br />

- signalling<br />

separate ?<br />

inherent ?<br />

scparate ?<br />

-<br />

inherent<br />

separate ?<br />

Bellanqzr l97L [L2,LL,69]<br />

Tomlinson l976 [L81<br />

Drogespt R78 [L61<br />

Rdste [L71<br />

Vary 1978 [22.30]<br />

Pelloni 1979 1231<br />

Narasimha 1979 [SO]<br />

2.5ms<br />

c 3ms?<br />

-3ms<br />

Not S<br />


PROCEEDINGS OF THE IEEE, VOL. 69, NO. 11, NOVEMBER 1981<br />

('J)<br />

Fig. 17. Generation of an FDM signal according to the low-pass filterbank<br />

method.<br />

Fig. 18 depicts the block diagram of the transmultiplexer<br />

operating according to this method.<br />

A comparison of Fig. 15 with Fig. 18 shows that there are N<br />

complex bandpass filters required in the bandpass filter-bank<br />

method and 2N low-pass filters in the low-pass filter-bank<br />

method. The number of filters is the same, since a complex<br />

filter can be constructed from two real filters. As the sampling<br />

rate in the low-pass filter-bank method is by a factor of two<br />

lower and the absolute widths of the filter transition bands are<br />

the same, the amount of circuitry for the low-pass filters is<br />

smaller than that for the bandpass filters. On the other hand,<br />

the number of arithmetic operations in the Fourier processor<br />

remains about the same, because a 2N-point IDFT at half the<br />

sampling rate requires about the same amount of circuitry as<br />

an N-point IDFT at double sampling frequency.<br />

A consi<strong>der</strong>able part of the circuitry to be expended on the<br />

low-pass filter-bank method is required for the generation of<br />

the complex singlesideband signals. Here, the Hartley method<br />

proves to be the most favorable, for it needs about 4 poles and<br />

4 zeros for a phase splitting network. In contrast, the Weaver<br />

method requires about 8 poles [3].<br />

In 1974, Bellanger and Daguet [42] first proposed a transmultiplexer<br />

according to the above mentioned low-pass filterbank<br />

method. Further modifications of the DFT-algorithm<br />

lead to a special inverse discrete Fourier transform (102 DFT).<br />

Moreover, filters generating complex-valued signals can completely<br />

be omitted. Thus a further reduction of the number of<br />

arithmetic operations is accomplished. This highly efficient<br />

type of transmultiplexer was presented by Bonnerot et al.<br />

[43] -[45], by Drageset et al. [46], R&te et al. 1471, and by<br />

Pelloni [23].<br />

Still another transmultiplexer, proposed by Tomlinson and<br />

method. In this approach polyphase filtering is accomplished<br />

by a single time-multiplexed filter. This filter is mechanized as<br />

a so called time-varying filter where the coefficients are<br />

periodically interchanged at a rate corresponding to the low<br />

sampling frequency. Thus the effective operation rate complies<br />

with the high sampling rate. At first sight, the transmultiplexer<br />

of Tondinson and Wong [481 seems to be of lower<br />

computational complexity than the Bellanger and Daguet [42]<br />

approach. Yet the computational load of the polyphase filters,<br />

operating at the low sampling rate, is about the same as that of


<strong>SCHEUERMANN</strong> <strong>AND</strong> <strong>GOCKLER</strong>: DIGITAL TRANSMULTIPLEXING METHODS<br />

TDM-signal<br />

FDM -signal<br />

SS0 : single-sideband modulator (Hartley - or Weava- method]<br />

sanp(ing rate<br />

V' W 1<br />

- 1 1 1<br />

J, I<br />

NT 2NT T<br />

Fig. 18. Block diagram of transmultiplexer according to the low-pass<br />

filter-bank method.<br />

the time-varying filter operating at the high sampling rate.<br />

Thereby the necessary control circuitry is not consi<strong>der</strong>ed.<br />

Finally in 1979, Narasimha and Peterson [50] presented a<br />

transmultiplexer using an N-point discrete cosine transform<br />

(DCT). In contrast to other low-pais filter-bank methods, with<br />

this approach no premodulation is required to generate complex-valued<br />

signals. This means that the individual filters of the<br />

filter bank to be <strong>der</strong>ived from a low-pass prototype filter<br />

exhibit Hermitian symmetry according to (15) corresponding<br />

to real coefficients. Thus, in or<strong>der</strong> to obtain the desired passband<br />

frequency position of the individual bandpass filters of<br />

the filter bank, the low-pass transfer function has to be<br />

shifted by<br />

instead of<br />

Summation of the individual channel signals yields the output<br />

signal<br />

. [H,(~N, in[r+llZl ) + H, (p, -in [r +l12 l )l. (34)<br />

By inspection and employing trigonometric identities we get<br />

after interchanging the sequential or<strong>der</strong> of summation<br />

. cos [d2r + 1) 5<br />

l<br />

- x,.(z~). (35)<br />

r=o<br />

n<br />

Here, the second term represents the DCT.<br />

substitution<br />

Applying the<br />

as it is the case with the other low-pass filter-bank methods. findy we obtain<br />

In conjunction with Hermitian symmetry and the Modulation<br />

Theorem of z-transform we get N-l N-l<br />

Y(z) = C z-"G,(z~) cos<br />

= 3 [ ~ ( ~ ~ 1 i IN) ~ + [ H(ze-jn ~ + ~ lr+llZ / ~ 1 IN)]. (32) n =O r=0<br />

Comparing this solution with (31), here only an N-point DCT<br />

~pplyin~ the polyphase principle for interpolation we <strong>der</strong>ive processor instead of a 2N-point DFT processor is needed. The<br />

with (8)<br />

branch filters of the polyphase network are modified according<br />

to (36). With the application of linear phase FIR filters<br />

significant simplifications of hardware are possible, as it is<br />

reported in [ 501. A somewhat different implementation of<br />

the Narasimha and Peterson approach was proposed by<br />

Marshd [80]. Here the DCT is performed in an other way<br />

and the filters of the polyphase network are specifically<br />

matched single-input-double-output filters of the recursive<br />

(33) type.


PROCEEDINGS OF THE IEEE, VOL. 69, NO. 11, NOVEMBER 1981<br />

H, = rcurs.~ lwrpols<br />

H2= transversal lowpau<br />

1 voice -band spectrum<br />

I ,<br />

flkHz<br />

('J)<br />

Fig. 19. Block diagram of the transmultiplexer according to Freeny<br />

etal. 1151.<br />

C. Weaver-Structure Method<br />

A direct method for the generation of an FDM signal is the<br />

Weaver SSB-MOD bank according to Section 111-B. By ingenious<br />

partitioning of filters into recursive and transversal lowpass<br />

filters, operating at different sampling rates, the amount<br />

of circuitry can be kept low. Fig. 19 shows a transmultiplexer<br />

according to Freeny et al. [15], [51] which operates in compliance<br />

with this method.<br />

The TDM signals are being furnished at a sampling frequency<br />

of fsl = 8 kHz and modulated onto an auxiliary carrier with a<br />

frequency of fs1/4, so that the voice signal occupies the frequency<br />

range -2 < f/kHz < t 2. The modulation is very<br />

simple, since the sampled carrier is given by the sequence<br />

{. . - 0, 1, 0, - 1, 0 . . .). In the next step, the sampling fre-<br />

quency is doubled. The filter HI represents a recursive lowpass<br />

filter with a cutoff frequency of 2 kHz (Fig. 19(b)). At<br />

the output of filter HI, the sampling frequency is increased by<br />

a factor of M. This signal is processed by the following transversal<br />

low-pass filter H*. After that, the resulting spectra are<br />

shifted to the desired frequency bands by modulation. The<br />

FDM signal is obtained by summation of the individual signals.<br />

The purpose of the two low-pass filters is twofold: They are<br />

necessary for the operation of the Weaver modulator, and they<br />

serve at the same time as interpolation filters as described in<br />

Section V-A.<br />

Almost one year before the publication of the above Freeny<br />

papers, Kurth [52], as well, proposed a sophisticated transmultiplexer<br />

scheme based on the Weaver modulation. While feed-<br />

ing the Weaver modulator by highly oversampled, ingeniously<br />

interpolated, and spectray inverted voice-band sequences, he<br />

uses high-pass instead of low-pass filters in the Weaver modulator.<br />

However, the main drawback of this proposal is that, in<br />

contrast to the Freeny approach [l 53, the Weaver modulator<br />

operates at the high sampling rate throughout. Therefore, the<br />

resulting operation rate is far too high for a practical implementation<br />

(cf., Section IV). According to the proposal of<br />

Kurth an exploratory TDM/FDM single-sideband generator<br />

was presented by Kao [53].<br />

An extension of the approach reported by Freeny et al. [l51<br />

was-even earlier in time than [52] but not recognized in its<br />

far-reaching importance in those days-described by Darlington<br />

[ 161. To thls end, the low-pass filter cascade<br />

In this expression, [HR (z)]-l represents the recursive part and<br />

Hr(z) the transversal part of the transfer function H(z). As<br />

outlined in Section V-C, the transfer function H(z) can be split<br />

into parallel branches according to (8)


<strong>SCHEUERMANN</strong> <strong>AND</strong> <strong>GOCKLER</strong>: DIGITAL TRANSMULTIPLEXING METHODS<br />

As can be seen from (13), the recursive part can be put as a<br />

factor in front of the summation, since it is common to all<br />

additive terms. Thus using (38), equation (39) becomes<br />

N-l<br />

H(z) = [ H~(z~)I-' - C Z-'HTr(zN). (40)<br />

r=O<br />

According to (40), the transmultiplexer of Fig. 19 is modified<br />

such that the structure depicted in Fig. 20 results. The modulators<br />

at the input are now replaced by rotating switches.<br />

The part of the transmultiplexer in Fig. 20 bounded by the<br />

dashed Line can be simplified further. To this end, the FDM<br />

L__-- - --J<br />

Fig. 20. To the <strong>der</strong>ivation of Darlington's transmultiplexer [ 161.<br />

Furthermore, the following expressions hold:<br />

Yini(z)=.fhi(zN) N-l C Z-'H~(~)<br />

r=o<br />

N-1<br />

Yqi(z) = kqi(zN) C z-~H~~(z~).<br />

r=o<br />

(44)<br />

(45)<br />

Inserting (44) and (45) into (42) and (43), respectively, we<br />

signal is expressed in terms of symbols used in Fig. 20 Yj&) = ihi(zN) C {z' 3 [e+i(2nlwir<br />

r=o<br />

N-l<br />

According to the Modulation Theorem of z-transform, we ob-<br />

N-l<br />

yqi(z) = iqi(p) {z-r -L [e+f(2n~~)ir<br />

tain for Yini and Yqi r=o 2i<br />

cos X = + (eix -t e-ix)


PROCEEDINGS OF THE IEEE, VOL. 69, NO. 11, NOVEMBER 1981<br />

1<br />

sampling f rcqucncy 8 kHz 1 8 N kHz<br />

Fig. 21. Transmultiplexer according to Darlington [ 161.<br />

and<br />

the summed signal at point 1 is<br />

and by inserting (46) and (47) into (411, there results<br />

Y(Z) = k*i . z-~<br />

i=o {<br />

N-l<br />

rq<br />

cos (: i$<br />

HTr(zN)<br />

An interchange of summation and rearrangement of factors<br />

leads to<br />

where fo = fs/4.<br />

The spectrum at this point is given by<br />

+Xz(f- fo)+Xz(f +fob<br />

In the subsequent low-pass filtering, frequencies higher than<br />

l fo l are suppressed, so that the signal at point 2 becomes<br />

At point 3, we obtain<br />

From (44) the transmultiplexer according to Darlington [l 61<br />

with a cosine and a sine processor can be <strong>der</strong>ived, the block<br />

diagram of which is shown in Fig. 21.<br />

Note: If the sampling rate is reduced by a factor of two at<br />

the output ports of Ihe recursive filters HR(zN), and, in addition,<br />

the cosine-sine processor is provided with the conjugate<br />

complex input signals, a W-point DFT results as can easily be<br />

shown. The transmultiplexer of Fig. 21 then merges into that<br />

of Fig. 18.<br />

A modified version of the transmultiplexer of Fig. 21 was<br />

proposed by Singh et al. [54]. By suitably processing the<br />

branch signals of the Weaver modulator, they achieve the conversion<br />

of two TDM signals using only one modulator (Fig.<br />

22(a)). The sum of the two signals to be processed is applied<br />

to the upper branch, whereas the difference of these signals is<br />

fed into the lower branch.<br />

According to the Modulation Theorem, the z-transform of<br />

Ydf)=4[~1(f-fo -fc)+X1(f-fo +fc)<br />

+Xz(f-fo -fc)+Xz(f-fo +fc)l. (50)<br />

Using similar calculations, the signal at point 3' of the quadrature<br />

branch is obtained<br />

Y3r(z) = - 3xl (ze -jzrrfalfs<br />

-i~nfclfs)<br />

+ $xl (ze -iznfO Ifs .e +iznfclfs)<br />

+ ~ .~~(~~-i2nf~ Ifs .e-iznfc/fs)<br />

- (,,-iZnfo Ifs +iZnfclfs<br />

2 2 'e 1


(b)<br />

Fig. 22. 'Modification of the Weaver modulato: according to Singh<br />

et al. [54].<br />

Using (50) and (51), there results at the output<br />

This process is depicted in Fig. 22(b). Now only N/2 recursive<br />

low-pass filters are needed instead of N recursive low-pass<br />

filters. The same applies to the transversal filter bank at the<br />

output (Fig. 21). The N-point sine and cosine processor is<br />

reduced to one with N/2 points. However, processing of the<br />

signals must now be done at double speed, because the sampling<br />

frequency is increased by a factor of 2 to 16 kHz. Therefore<br />

a reduction of the necessary amount of circuitry and<br />

arithmetic operations cannot be expected.<br />

Similar signal processing is also possible using a HartIey<br />

modulator. With this method, two channel signals may likewise<br />

be converted using one modulator only [4].<br />

Recently, an alternative approach to the Weaverstructure<br />

method was published by Peled and Winograd [55]. The<br />

complex input signals are generated by Weaver modulators.<br />

In contrast to the transmultiplexers described so far in this<br />

section, linear-phase transversal filters are used exclusively<br />

both for band limiting and interpolation. By suitable grouping<br />

and utilization of symmetries, a consi<strong>der</strong>able reduction of the<br />

number of arithmetic operations is achieved. The resulting<br />

signal processor is specifically tailored for a TDM/FDM conversion<br />

of 12 channels. To realize a 60-channel transmultiplexer,<br />

five such transmultiplexers have to be connected by<br />

using an analog interface.<br />

D. Multistage Modulation Methods<br />

With muitistage modulation methods, both the sampling<br />

rate and the spectral position of the signals to be processed are<br />

changed step by step. Various intermediate FDM signals are<br />

composed which comprise an increasing number of channels<br />

from stage to stage. In the last stage the FDMsupergroup<br />

signal is formed.<br />

A transmultiplexer operating according to this principle was<br />

published by Tsuda et al. 1561, [58]. The principle is explained<br />

by way of an eight-channel transmultiplexer shown in<br />

Fig. 23(a). For convenience, complex signals are used throughout;<br />

all spectra-apart from those of the real input sequences<br />

{xi(v8T) l i = 0, 1, 2, - .., 7)-are spectra of complex sequences.<br />

The symbols used for multiplication, addition and<br />

interpolation of complex sequences in Fig. 23(a) are explained<br />

in the time domain in Fig. 23(b). The spectra depicted in Fig.<br />

24 serve as illustration for the signal processing in the trmsmultiplexer;<br />

the notation used refers to Fig. 23(a).<br />

The TDM signals Xi(z) (Fig. 24(a)) are fed in at a sampling<br />

rate of fsl = fs/8 =-8 kHz and modulated on a carrier at a<br />

frequency of fsj /(4) (Fig. 24(b)). This is the same process<br />

as in the Weaver-structure method described in Section VI-C.<br />

After the subsequent low-pass filtering with the filter characteristic<br />

Ho(eln) (Fig. 24(c)) the spectra Xi2, i = 0, 1, 2, . - - ,7,<br />

as shown in Fig. 24(d), result. By inserting a zero between<br />

every two successive samples, the sampling frequency is increased<br />

by a factor of two, whereby, as outlined Section<br />

V-A, Ell serves as interpolation filter pair (Fig. 24(e), (f)).<br />

Thereafter, by a modulation process, the spectrum of every<br />

even-numbered branch is shifted to the left by Af = 1/(32T),<br />

and that of every odd-numbered branch to the right by<br />

Af = 1/(32T). Fig. 24(g) shows the spectra Xi4 for i = 0,<br />

2,4, 6, and Fig. 24(h) those for i = l, 3, 5, 7. Finally, the<br />

first stage FDM signals Xis/(i = 0, 1, 2, 3) are obtained by<br />

addition of the signals Xi4 and X(i+1)4 for i = 0, 2, 4, 6<br />

(Fig. 24(i)).<br />

In the following stage the signals are processed in the same<br />

way (increase of the sampling frequency by a factor of two,<br />

"left7'- and "right"-shifts of the spectra by Af = 1/(16T)).


PROCEEDINGS OF THE IEEE, VOL. 69, NO. 11, NOVEMBER 1981<br />

traquancy danain<br />

B(zl {RcCa~t} &<br />

time domain<br />

{RC~~IVII}<br />

RcIc 1~11)<br />

U<br />

U<br />

(b)<br />

Fig. 23. Eight-channel transmultiplexer according to Tsuda et al. [56].


<strong>SCHEUERMANN</strong> <strong>AND</strong> GoCKLER: DIGITAL TRANSMULTIPLEXING METHODS<br />

Fig. 24. Spectra of transmultiplexer according to Fig. 23.<br />

The corresponding spectra are sketched in Figs. 246), (k), (l),<br />

(m), (n). In the last stage the samphg frequency is increased<br />

once more by a factor of two, however, the modulation<br />

process is chosen such that the spectrum of the branch i = 0 is<br />

shifted along the frequency axis .by Af= 1/(8T), and the<br />

spectrum of the branch i = 1 by Af = 3/(8T) to the right (Figs.<br />

24(0), (p), (q), (I), (S)). The complex FDM signal Y is produced<br />

by addition of Xolo and Xllo (Fig. 24(t)). Its real part<br />

represents the desired FDM signal Y (Fig. 24(u)).<br />

A great advantage of this method is that it only requires a<br />

small number of different filter types. go represents a pair<br />

of identical low-pass filters with a narrow transition band<br />

(Fig. 24(c)). Because these filters operate at the lowest possible<br />

sampling rate, the amount of circuitry, however, remains<br />

relatively low. Furthermore, it can be shown for i > 0 (i Em<br />

that all filters _Hi exhibit the same relative width of the transition<br />

band. Thus for every &(i > 0) just one filter type can<br />

be used; the frequency response is selected merely by changing


PROCEEDINGS OF THE IEEE, VOL. 69, NO. 11, NOVEMBER 1981<br />

R = ZR -f-<br />

fs<br />

fs = output sampling rate<br />

Fig. 24. (Continued).<br />

Fig. 25. Transrnultiplexer subunit for 12 charineis according to Fettweis [59].<br />

the sampling frequency. In addition, the expenditure for the<br />

interpolation filters is reduced to a great extent, since nonrecursive<br />

"half-band" filters [57! are used. In [58] an efficient<br />

experimental realization of such a 60-channel transmultiplexer<br />

isdescribed in detail, and experimental results are given.<br />

Recently, a further transmultiplexer design based on the<br />

multistage principle of Tsuda et al. was published by Constantinides<br />

and Valenzuela [73]. Here, for any two intermediate<br />

FDM-signals complex modulation, interpolation and<br />

filtering are performed by using only one type of a two branch<br />

polyphase network, each combined with four operations for<br />

spectral inversion, and a band multiplexer using an FIR filter.<br />

h alternative transmultiplexer approach, based likewise on<br />

the multistage modulation principle, is proposed by Fettweis<br />

[59]. By appropriate selection of the basic sampling rate and<br />

by ingenious arrangement of the various carrier frequencies, it<br />

is accomplished that every modulation process is reduced to a<br />

multiplication with a sequence of carrier samples only comprising<br />

the trivial values of 0 or + 1.<br />

As a consequence, the modulation processes cannot produce


Fig. 26. Spectral illustration of the transmultiplexer subunit according to Fig. 25.<br />

quantization errors. The principles of such "multiplier-free"<br />

modulation systems are described in detail in 1601. "Mdtiplierfree"<br />

modulation schemes for TDM/FDM conversion are outlined<br />

in [59]. This modulation scheme is particularly favorable<br />

for the conversion of two 2048 Mbit/s PCM TDM bit<br />

streams (PCM30) to a supergroup of the FDM hierarchy (60<br />

channels in the frequency band from 312 kHz to 552 kHz),<br />

since with this approach an additional analog frequency<br />

translation of the FDM signal can be avoided. The principle of<br />

the Fettweis approach will therefore be treated for a 60-<br />

channel transmdtiplexer.<br />

The 60 TDM voice signals are converted to the FDM format<br />

using five submits, each of them for 12 voice channels (Fig.<br />

25). Subsequently, these five intermediate FDM signals are<br />

combined to a 60-channel FDM supergroup signal (Fig. 27).<br />

The spectra in Figs. 26 and 28 serve as illustration; the notation<br />

of Fig. 25 is related to Fig. 26 and the notation of Fig. 27<br />

corresponds to Fig. 28.<br />

The TDM input signals Xb(z) are supplied at a sampling<br />

frequency of fso = fs/72 = 8 kHz (Fig. 26(ad). BY inserting<br />

two zero-valued samples between every pair of adjacent<br />

samples of the original sequence and subsequent filtering with<br />

the frequency response H.<br />

(Fig. 26(a2)), the sampling fre-<br />

quency is increased by a factor of three to fS1 = fS/24 = 24<br />

kHz. For details on the selection of fs, = 24 kHz, the rea<strong>der</strong><br />

is referred to the discussion in 1601.<br />

By multiplication of the signals of every second channel by<br />

the sequence ((-l)'), the spectrally inverted signals xAK are<br />

produced for n = l, 3, 5, . - - , 11 (Fig. 26(a4)); another increase<br />

of the sampling frequency by a factor of two to


PROCEEDINGS OF THE IEEE, VOL. 69, NO. 11, NOVEMBER 1981<br />

Fig. 26. (Continued).<br />

fsz = fS/12 =48 kHz follows (Fig. 26(a5)), Fig. 26(a6) fox<br />

n = 0, 2,4, . . . , 10 and Fig. 26(a7) for n = 1, 3,5,. - - , l l).<br />

Furthermore, in the Figs. 26 (a,) and 26 (a7), the carrier fre-<br />

quency fC1 = fs& is shown. After the modulation process,<br />

performed by multiplication with the sequence {ol(v. 12~)) =<br />

the spectra X: are obtained (Fig.<br />

{. . - 1, 0, 1, - 1, 0, . - m),<br />

26(a8) for n = 0, 2, 4, .- - , 10 and Fig. 26(a9) for n =<br />

1, 3, 5, ..., 11). By low-pass filtering (Fig. 26(alo) the upper<br />

sideband is suppressed (Fig. 26(all) for n = 0, 2, 4, ..., 10<br />

and Fig. 26(a13) for n = 1, 3, 5, - . - , 11). After the spectral<br />

inversion of the signals in the channels n = 0, 2,4, ..., 10, the<br />

signals xK and are added, yielding the signals X; for<br />

n = 0, 1,2, . - . , 5 (Fig. 26(al4).<br />

Subsequently the signals X: for n = 1, 2, 3,4 are processed<br />

in the same way as the signals X;, with the only difference<br />

that the sampling rate is twice as high at any point (Fig. 26(b 1)<br />

through (bll). The spectra for X: and X; are depicted in<br />

Fig. 26(b12). The same holds for the signal (Fig. 26(cl)<br />

through (cl2) in the next hierarchy stage.<br />

As shown in Figs. 26(dl) through (dl;), the spectra X; and<br />

X: are processed differently; the filter characteristic Hg appears<br />

only in the channels 0, 1, and 10, 11. Finally, the Figs.<br />

26(e1) through (e4) show, how the signal Yi is generated from<br />

the signals xk3, xi3, and X:$.<br />

The subsequent processing of the subunit signals Yi(i=<br />

0, 1,2,3,4) is shown in Figs. 27 and 28. After having increased<br />

the sampling rate by a factor of three, the signal Y:<br />

already occupies the desired frequency band (Fig. 28(al)-(~3)).<br />

The same holds for the signal Y: (Fig. 28(dl)-(d3)) if it is<br />

spectrally inverted beforehand.<br />

In processing the signal Y4 two spectral inversions have to be<br />

performed (Fig. 28 (bl) through (ba)), one before and one after<br />

the sampling rate increase. Each of the signals Y1 and Y3 is<br />

subjected to a modulation (multiplication by the sequence<br />

(P(v - T)) = 1. - . , - 1, 0, 1, 0, - 1, 0, . . .)) and subsequently<br />

passed through a high-pass filter for sideband suppression (Fig.<br />

28(cl) through (~4) and Fig. 28(el) through (e~). Finally,<br />

the 60channel FDM supergroup signal Y(z) is formed by<br />

adding the five signals Y;, Y:, Y:, Y& and ~ 4 (Fig. 1 28(f)).<br />

~<br />

The transmultiplexer approach by Fettweis is well suited for<br />

the application of wave digital filters [61], [78]. A detailed<br />

discussion on this subject can be found in [591. At present,<br />

this approach is the only transmultiplexer which might possibly<br />

be mechanized by means of sampled-data filters (e.g.,


<strong>SCHEUERMANN</strong> <strong>AND</strong> <strong>GOCKLER</strong>: DIGITAL TRANSMULTPLEXING METHODS<br />

nbn, AAM, nnnn, AAAA<br />

o 16 32 LB 6i 80 96 112 128 IU 160 176 192 f<br />

T<br />

T<br />

I<br />

T<br />

T<br />

nnnn<br />

ILL 160 176 192<br />

f<br />

-<br />

192 f<br />

AA AA, -<br />

160 176 192f<br />

I<br />

I nnnr\, a<br />

0 16 32 6L % 128 1M3 176 l92 f<br />

AA r\nnn,~~nn, nnnn -<br />

0 32 L8 80 96 112 1U 160 192 f<br />

nn M, nmnn~, AAAA, -<br />

0 32 L8 80 96 112 1U 160 192 f<br />

-<br />

9<br />

0 96 192 f<br />

AAAA<br />

nnnn,<br />

0 32 L& 96 lk 160 192 f<br />

nnnh AAAA, -<br />

0 L8 6L 96 128 ILL 192 f<br />

nnnn, AAAA, -<br />

32 L 8 96 1 U 160 192 f<br />

nnnnnnnn,<br />

AAMAAAA,<br />

0 32 6L 96 128 160 192 f<br />

Fig. 26. (Continued).<br />

switched-capacitor filters 1601, [62]-1641, 1791, because it<br />

does not make use of cancellation.<br />

In the previous four sections of this chapter we have discussed<br />

transmultiplexer methods which are based on one of<br />

two fundamental concepts of filter decomposition: 1) parallel<br />

decomposition using a signal processor and 2) serial decomposition<br />

resulting in a tree-like structure. Naturally, it is<br />

possible to compound both principles. Recently such an<br />

approach was disclosed by Molo [74]. This approach starts<br />

from a 2-kHz frequency shifted version of the incoming<br />

TDM-signal xr(zN) as it is shown in Fig. 17(a). Now the<br />

remaining transmultiplexer has to perform a filter bank which<br />

is <strong>der</strong>ived from a low-pass prototype. The basic idea is now to<br />

decompose the filter both in a parallel and in a serial manner.<br />

The manipulation of the parallel part of the filter decomposition<br />

equals the low-pass principle. The treatment of the serial<br />

part resembles the <strong>der</strong>ivation of a radix-2 butterfly in an FFT.<br />

Thus we get a complex 8-point IDFT followed by a tree-like<br />

structure with multipliers and modulators to perform frequency<br />

pre- and post-shifting. Note that the number of TDM<br />

channels to be frequency multiplexed in this approach has to<br />

be a power of two.<br />

VII. COMPARING THE TRANSMULTIPLEXER METHODS<br />

If we want to compare the individual transmultiplexer<br />

methods described so far with each other, we need an appropriate<br />

tool for comparison. Certainly, the most important<br />

features of such a tool are cost and performance. To allow a<br />

more detailed judgment, however, a representative list of<br />

criteria will be set up as a basis for the subsequent comparison.<br />

A. List of Criteria [I]<br />

When comparing digital transmultiplexing methods with<br />

emphasis laid on the inherent algorithms, the subsequent list of<br />

criteria must, to some extent, be incomplete, since not all<br />

aspects of hardware are covered in this paper. Note that the<br />

sequential or<strong>der</strong> of the following criteria is chosen essentially<br />

according to their relative importance in these authors'<br />

opinion.<br />

1) 'Stability Un<strong>der</strong> Looped Conditions (6.51: With the application<br />

of digital transmultiplexers, stability problems may<br />

potentially arise, since these assemblies are installed in the<br />

four-wire branch of an essentially two-wire transmission line<br />

(Fig. 29). Due to the four-wireltwo-wire transitions (hybrids),


PROCEEDINGS OF THE IEEE, VOL. 69, NO. 11, NOVEMBER 1981<br />

*<br />

0 96 192 f<br />

x;k'*)l I I I I<br />

I<br />

nn, I AA, , ,m I AA,<br />

0 b 16<br />

k6,lP)l<br />

A A,<br />

32 6L 80 88 96 10L li2 128 160 176 18L 192 f<br />

I<br />

I<br />

I<br />

\h, , ,AA, I<br />

,<br />

I<br />

-<br />

0 8 16 32 6L 80 88 96 1OL 112 128 160 176 18L 192 f<br />

1x;i<br />

AA, AA AA, M,<br />

0 16 2L L0 L8 56 72 80 96 112 120 136 1U 152 168 176 192 f<br />

P ,m nnM, AA, M, AA,~<br />

I<br />

I<br />

n, nn -m<br />

0 16 2L L0 LB 56 72 80 96 112 120 136 1U 152 l68 ' lj6 192 f<br />

lH2l<br />

IIX:I<br />

L<br />

0 96 192 f<br />

4 \,h,<br />

0 l6 2L . L8<br />

AA, \,h, .m1<br />

72 80 96 112 120 ILL ljg 176 192<br />

L<br />

Fig. 26. (Continued).<br />

transmultiplexers actually operate in a looped arrangement. osciUations will generally disturb not only the telephone<br />

Stability, however, must be guaranteed un<strong>der</strong> any adverse channel un<strong>der</strong> consi<strong>der</strong>ation but also a multiplicity, if not all,<br />

condition, such as strongly unbalanced hybrids which may adjacent channels.<br />

occur in practice. This is particularly crucial, since parasitic One way to avoid these parasitic oscillations un<strong>der</strong> any


<strong>SCHEUERMANN</strong> <strong>AND</strong> <strong>GOCKLER</strong>: DIGITAL TRANSMULTIPLEXING METHODS<br />

Fig. 27. Complete 60-channel transmultiplexer according to Fettweis<br />

[591.<br />

practical circumstances is to use transversal (FIR) filters. Alternatively,<br />

wave digital filters (WDF) may be used when the<br />

exclusive utilization of FIR filters is inefficient. For these<br />

filter classes, potential stability un<strong>der</strong> looped conditions has<br />

been proved by Meerkotter and Fettweis [65]. They showed<br />

that only minor m'easures are required for guaranteeing<br />

absolute stability. Note that their proof is based on the implicit<br />

assumption of a single-way modulation scheme, meaning<br />

that each input signal to the TDM/FDM-translator arrives at<br />

the output by a separate way. Furthermore, this stability<br />

theory can be extended to two-way modulation schemes using<br />

Hartley or Weaver modulators [l 21-[ 141 for processing<br />

complex-valued signals. However, in or<strong>der</strong> to assure absolute<br />

stability in this case, the required computational complexity is<br />

substantially higher than that of single-way modulation<br />

schemes. Initial attempts to apply this theory to transmultiplexing<br />

methods utilizing discrete Fourier-, sine-, cosine-, or<br />

Hadamard-processors, respectively, indicate that, as compared<br />

to a two-way modulation scheme, still much additional circuitry<br />

would be required for guaranteeing absolute stability (if<br />

it could be achieved at all) un<strong>der</strong> looped conditions [ 11.<br />

2) Absolute Value of the Group Delay: As stated in<br />

Table I, the absolute value of the group delay measured at the<br />

analog ports of a transmultiplexer, the digital ports being<br />

looped, may not exceed 3 ms. This criterion is placed just<br />

behind stability, since some, even promising transmultiplexer<br />

approaches do not meet this requirement. This holds true<br />

particularly for some methods applying linear-phase FIR<br />

filters, or block processing, respectively.<br />

3) Computational and Control Complexity: The overall<br />

computational complexity of a digital signal processing algorithm<br />

can be measured by the number of multiplies and/or<br />

adds to be carried out per second. However, these figures are<br />

suitable measures only if the associated wordlengths are taken<br />

into account appropriately. This is, for instance, achieved if<br />

the multiplications and additions are counted at the bit level<br />

[ 151. mus transmultiplexers which make explicit use of<br />

multipliers can be compared with other approaches being<br />

based on the application of the canonical signed-digit (CSD)<br />

code [Ss], [66]. With this code all multiplications are com-<br />

pletely replaced by combined shift/add operations. In contrast<br />

to these ideas, when using higher integrated signal processors,<br />

the computational load may be measured in machine cycles<br />

per second [ 21.<br />

Besides the multiplication and/or addition rate the overall<br />

complexity of the controlunits (timing, logic, etc.) may not be<br />

overlooked. Unfortunately, there does not exist any general<br />

direct relation between the efficiency of a transmultiplexing<br />

method and its control complexity. It is even felt that the<br />

more efficient the algorithm the higher the control complexity.<br />

Hence, concerning the latter, the subsequent comparison must<br />

compulsorily be rather vague.<br />

4) Modularity: A highly modular transmultiplexer implementation<br />

is thought of being composed of a great number of<br />

identical subunits of low complexity. Moreover, the number<br />

of different subunits should be as small as possible. For this<br />

reason, a highly modular transmultiplexer approach has the<br />

potential of good testability, high reliability, and may, in addition,<br />

be suitable for LSI/VLSI-integration. Furthermore, the<br />

overall control complexity is expected to be noticeably smaller,<br />

since identical subunits can, in general, be controlled by identical<br />

pulse trains. Finally, design and manufacturing will greatly<br />

be simplified in contrast to an approach of lower modularity.<br />

5) Intelligible Crosstalk: In a transmultiplexer residual<br />

crosstalk between arbitrary channels may occur within the<br />

limits given in Table I. Clearly, intelligible crosstalk represents<br />

a more severe system degradation than unintelligible crosstalk.<br />

Therefore, different transmultiplexer approaches may also be<br />

compared with each other on the basis of their relative amount<br />

of intelligible and unintelligible crosstalk introduced. According<br />

to Fettweis [I] and own investigations, intelligible crosstalk<br />

can essentially occur only between neighbouring channels,<br />

a single-way modulation scheme being provided. On the contrary,<br />

in a transmultiplexer based on a multiple-way modulation<br />

scheme in combination with a phase-compensation<br />

method for filtering, in at least every second pair of any two<br />

channels intelligible crosstalk is observed.<br />

6) Analog Frequency Conversion: Consi<strong>der</strong>ing the European<br />

60-channel transmultiplexer approach, there are two suitable<br />

rates to be used for sampling the FDM supergroup signal,


PROCEEDINGS OF THE IEEE, VOL. 69, NO. 11, NOVEMBER 1981<br />

~YLK (ejln)l<br />

A [1;2'\- h 4 L<br />

0 2L L2 1M 158 216 23 288 312 360 LOB L% 504 552 576<br />

Wt<br />

, r-f<br />

0 2L R 288 SOL 552 576<br />

Fig. 28. Spectral illustration of the transmultiplexer according to Fig. 27.<br />

512 or 576 kHz, respectively. The first one (generally leading<br />

to slightly more efficient digital transmultiplexing algorithms)<br />

requires an analog frequency translation of the FDM output<br />

signal to the supergroup band (ranging from 3 12 to 552 kHz)<br />

after D/A conversion. Thus additional noise is introduced by<br />

the supplementary analog circuitry [67]. On the contrary,<br />

with a sampling rate of 576 kHz this drawback can be overcome,<br />

since the FDM supergroup signal is obtained directly<br />

in the desired frequency band. Hence, a bandpass filter for<br />

post D/A conversion smoothing is all that is required. Moreover,<br />

it can be shown that this bandpass filter exhibits better<br />

sensitivity properties than the filters needed for the analog<br />

frequency translation with the 5 12-kHz super-group sampling<br />

rate [851.<br />

7) Out-of-Band Signaling and Pilots: Particularly related<br />

to European transmultiplexer approaches using out-of-band<br />

signaling, it is essential to know whether the signaling information<br />

and the pilot tones can be processed in the main unit,


, I ] ,l,2 12 f<br />

0 2L R 120 163 216 &L 288 312 3&l L08 L 56 50L 552 576<br />

Fig. 2 8. (Continued).<br />

un<strong>der</strong> looped conditions has not yet been proved [l]. Some<br />

- ------ other proposals use a two-way (T) modulation scheme. Fundamentally,<br />

the required absolute stability can be guaranteed<br />

Hybrid<br />

Hybrid<br />

\<br />

B. Comparison of the Individual Transmultiplexer Approaches<br />

In this section, the attempt is made to compare the transmultiplexer<br />

methods described so far on the basis of the above<br />

list of criteria. All available data are compiled in Table 11. It<br />

must be noted, however, that some figures are more or less<br />

uncertain as indicated. Moreover, other data are not directly<br />

comparable with each other, since the prescribed specifications<br />

do, in many cases, not comply with the CCITT Recommendations<br />

G. 791 to G. 793, published in 1980. This holds particularly<br />

true for those designs of earlier days. The sequential<br />

or<strong>der</strong> of the columns of Table I1 is chosen according to the<br />

list of criteria of the preceding section.<br />

Besides the number of channels, it can be seen from the<br />

second column of Table I1 that the majority of transmultiplexer<br />

approaches is based on a multiple-way (M) modulation<br />

scheme. As stated above,<br />

for these approaches at the expense of consi<strong>der</strong>able additional<br />

expenditure, the sole application of nonrecursive (FIR) and/or<br />

wave digital (WD) filters provided [ 1 ], [61], [65]. However,<br />

such an attempt has never been reported by Kurth [52] and<br />

+<br />

rc-tc<br />

Kao [53], Freeny et al. [Is], 1511, Singh et al. [54], Tsuda<br />

et al. [58], and Constantinides et al. [73]. This might be attributed<br />

to the high amount of circuitry necessary for an entire<br />

nonrecursive implementation, or to the fact that wave digital<br />

filters [61] could not have or have not been familiar to those<br />

C-<br />

authors. The only approaches published up to now requiring<br />

negligible additional hardware for assuring absolute stability<br />

Fig. 29. Closed loop due to nonideal two--+re/four-wire transitions un<strong>der</strong> looped conditions were proposed by Fettweis [59], [60]<br />

[l],[651.<br />

and most recently by Kurth et al. [8 l], [82].<br />

The next column of Table I1 is related to the absolute value<br />

or, to which extent, additional circuitry, such as a separate<br />

translator, is required.<br />

of the group delay measured at the analog ports of a transmultiplexer,<br />

the digital ports being looped (cf., Table I). As<br />

stated above, the basic group delay may not exceed 3 ms. For<br />

this reason, all those transmultiplexer implementations exclusively<br />

using linear phase FIR filters are generally not applicable.<br />

However, within the great majority of these approaches the<br />

linear phase filters could be replaced by minimum phase filters<br />

at the expense of a generally lower computational efficiency.<br />

This does not hold for the proposal of Constantinides et al.<br />

[41], since fast convolution techniques being based on block<br />

processing are applied for filtering (cf., [23]). Moreover, it<br />

must be noted that substantial delay may arise in transmultiplexer<br />

realizations with an inherent multiple-way modulation<br />

scheme utilizing DFT, DCT, or related signal processors.<br />

From the next column of Table I1 the operation rate per<br />

channel, or the multiplication (M) and addition (A) rates per<br />

channel can be seen, respectively. Here, the algorithms of<br />

Bellanger et al. [42]-[45], and Narasimha et al. [50], [86]<br />

being based on a multiple-way modulation scheme are, by


PROCEEDINGS OF THE IEEE, VOL. 69, NO. 11, NOVEMBER 1981<br />

far, most efficient. According to the subsequent column of<br />

Table I1 referring to the degree of modularity, the control<br />

circuitry required for these approaches is, on the contrary,<br />

expected to be rather complex. This is confirmed by Bellanger<br />

et al. [70] giving a figure for their amount of transmultiplexer<br />

overhead circuitry of up to 30 percent of the total hardware.<br />

Moreover, the transmultiplexer methods with an inherent<br />

multiple-way modulation scheme generally require the longest<br />

words for coefficient representation [70]. Hence, these approaches<br />

and, for instance, the proposal by Fettweis [59]-<br />

necessitating substantially shorter coefficients' wordlengths at<br />

a higher multiplication rate-can only be compared with each<br />

other on the bit level. However, such and other more detailed<br />

discussion of hardware aspects is beyond the scope of this<br />

paper. The interested rea<strong>der</strong> is referred to [70], [71 l.<br />

Conce~ng the degree of modularity, those transmultiplexer<br />

approaches needing only few interconnections between different<br />

modules and which exhibit a regular overall structure are<br />

classified to be highly modular. Hence, all methods applying<br />

a highly meshed signal processor and a filter bank with all<br />

filter coefficients being generally different are of a low degree<br />

of modularity. The poorest specimens of this sort seem to be<br />

the sophisticated transmultiplexer approaches of Peled et al.<br />

[55] and Molo [74]. On the contrary, a bank of Weaver<br />

modulators [ 1 S], [S l] -[53], and some multistage modulation<br />

methods [36], [56], [59], [73] exhibit a mo<strong>der</strong>ate or even<br />

higher degree of modularity. It is felt, that the approach of<br />

Kurth et al. [81], [82] shows the highest degree of modularity<br />

compared with all other methods of Table 11. Here, even the<br />

implementation of channel filters is highly modular.<br />

Finally, the last two columns of Table I1 are essentially selfevident.<br />

Suffice to say that a 12 (24)-channel transmultiplexer<br />

directly generating the FDM signals in the desired group band<br />

frequency range actually requires an additional (analog) group<br />

band to supergroup (SG) convertor, if it is to be used at the<br />

supergroup level. Furthermore, separate processing of outof-band<br />

signaling pulses is necessary for all North American<br />

transmultiplexer systems, since these are designed for in-band<br />

signaling. Although being based on the same 24-channel PCM<br />

frame as in North America, Japanese domestic FDM systems<br />

apply out-of-band signaling (cf., [8, table 111).<br />

VIII. CONCLUSION<br />

With this report an attempt was made to present a comprehensive<br />

survey of the currently known digital transmultiplexer<br />

methods. In or<strong>der</strong> to cope with this task, the necessary theoretical<br />

background, such as analog and digital modulation<br />

techniques, and the complex of sample rate alteration (i.e.,<br />

decimation and interpolation), is contained. Within the main<br />

section of this paper, the various transmultiplexing methods<br />

were classified into four categories: bandpass fdter-bank<br />

method, low-pass filter-bank method, Weaver structure method,<br />

and multistage modulation methods. Furthermore, on the<br />

basis of a list of criteria given in the preceding section, the<br />

individual transmultiplexer approaches were compared with<br />

each other.<br />

When concluding, we first pick up again the two most important<br />

items of Table 11: Absolute stability un<strong>der</strong> looped<br />

conditions, and the CCITT Recommendation concerning the<br />

absolute value of the group delay measured at the analog ports<br />

of a transmultiplexer, the digital ports being looped, which<br />

may not exceed 3 ms. Refening to stability in a looped arrangement<br />

(Fig. 29), we follow the <strong>der</strong>ivations of Fettweis<br />

et al. [l], [651 rigorously. (It must be noted, however, that<br />

the resulting conditions for guaranteeing absolute stability<br />

un<strong>der</strong> any adverse circumstances are sufficient but not necessary.)<br />

As a consequence of this assumption, we are forced to<br />

drop almost all, even computationally most efficient transmultiplexer<br />

approaches, such as 1441, [SO], due to potential<br />

stability problems. At present, the only exceptions are the<br />

multistage modulation method proposed by Fettweis [59],<br />

1601 and the per-channel approach by Kurth et al. [811,1821 .<br />

Certainly, the algorithms published by Kurth [S21 and Kao<br />

[53], Freeny et al. [IS], [Sl], Singh et al. [54], Del Re 1831,<br />

Tsuda et al. [56], [58], and Constantinides et al. [73] can<br />

also be used, provided that the implementation of these approaches<br />

is restricted to the sole application of wave digital<br />

andtor nomecursive filters. From these, however, only the<br />

two latter ones deserve further interest, since the other approaches<br />

mentioned here are relatively inefficient (cf., Table<br />

11). Morebver, if the Weaver modulator bank were extended to<br />

60 channels, this gap would still get wi<strong>der</strong> due to the increased<br />

sampling rate alteration ratio.<br />

The following comparison can, thus, be limited to the singleway<br />

modulation schemes of Fettweis [59], [60] and Kurth<br />

et al. 1811, 1821, and the two-way modulation schemes of<br />

Tsuda et al. [%l, 1.581 and Constantinides et al. [73]. The<br />

latter, however, applies recursive interpolators throughout the<br />

whole transmultiplexer. As a consequence, the sole use of<br />

wave digital andtor nonrecursive fdters would lead to a fundamental<br />

alteration of this approach: More or less, it would<br />

result in a new approach. Hence, we preclude this method,<br />

which is nevertheless very interesting due to its low computational<br />

load, from the following final discussion.<br />

Next, if the first most complex filter at the PCM end of the<br />

Tsuda approach were realized as a wave digital filter, the multiplication<br />

rate per channel according to Table I1 would essenti-<br />

ally be retained. However, in or<strong>der</strong> to guarantee absolute<br />

stability un<strong>der</strong> looped conditions, the additional amount of<br />

circuitry required for this two-way modulation scheme is expected<br />

to be substantially higher than that necessary for<br />

Fettweis' single-way scheme [ 11.<br />

Furthermore, in Tsuda's<br />

approach the minimum absolute value of the group delay of<br />

the multistage filter cascade of about 2.6 ms is not very far<br />

removed from the maximum allowable figure of 3 ms. A wi<strong>der</strong><br />

margin can, however, only be gained with the application of<br />

minimum phase FIR instead of linear phase halfband filters at<br />

the expense of a lower computational efficiency (cf., [57]).<br />

Finally, it must be noted that an additional analog frequency<br />

convertor has to be provided. On the other hand, the singleway<br />

modulation scheme of Fettweis is less regular (less modular)<br />

than Tsuda's transmultiplexer approach. Therefore, it<br />

depends essentially on the rea<strong>der</strong>'s particular weighting of the<br />

(optional) criteria discussed in Section VII, which of these two<br />

transmultiplexer approaches is preferable.<br />

Most recently, the discussion on different transmultiplexing<br />

methods has been promoted by the resumption of one of the<br />

first ideas in transmultiplexing history [l51 by Kurth et al.<br />

[8 l], 1821 : The direct extraction of the desired frequency<br />

band from the overall wide-band spectrum by a single interpolation<br />

or decimation filter per channel, respectively. Due to<br />

logarithmic processing this proposal is memory oriented. Since<br />

no multiplication at all must be carried out, the amount of<br />

memory seems to be extremely high: Between any multiply<br />

and add operations of the direct form minimum-phase FIR<br />

filter used, the logarithmic number representation has to be


<strong>SCHEUERMANN</strong> <strong>AND</strong> <strong>GOCKLER</strong>: DIGITAL TRANSMULTIPLEXING METHODS 1449<br />

converted to linear format. From this it follows immediately<br />

that all convertors with the exception of the p-law/logarithmic<br />

look-up table at each filter input are identical. Consequently,<br />

these convertor memories can efficiently be time-multiplexed<br />

within a channel filter and/or across the channels, since very<br />

fast ROM's are readily available. In conclusion, this approach<br />

taking full advantage of today's fast advancing memory technology<br />

seems to be one of the most promising transmultiplexing<br />

methods for the future. This approach is particularly<br />

striking due to its inherent high degree of modularity, requiring<br />

only one type of a direct form FIR interpolation filter with<br />

time-varying coefficients (cf., [921) which, by itself, is highly<br />

regular. With this approach the widespread expectation "the<br />

simpler, the better" seems to be best met.<br />

Nevertheless, in or<strong>der</strong> to stimulate the further discussion on<br />

efficient, absolutely stable, and modular transmultiplexing<br />

methods, the rea<strong>der</strong> is referred to a .forthcoming paper on a<br />

novel 60-channel transmultiplexer approach being based on<br />

a single-way multistage conversion scheme using directional<br />

filters [72], [go]. Furthermore, an extension of the proposal<br />

by Kurth et al. [8 1 ] with reduced computational load is presently<br />

being investigated [91].<br />

The authors are greatly indebted to Prof. Fettweis and Dr. L.<br />

Gazsi, Ruhr Universitat Bochum, to Prof. Schiissler, Dr. U.<br />

Heute and Dr. P. Vary, Universitat Erlangen-Niirnberg, and to<br />

Dr. R. Lagadec and Dr. D. Pelloni, formerly ETH Zurich, for<br />

various stimulating discussions on the topic treated in this<br />

paper. Furthermore, we would like to thank Dr. E. Gleissner<br />

for carefully reading the initial manuscript and providing valuable<br />

constructive criticisms.<br />

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[S51 H. Gockler and H. Scheuermann. unpublished investigations, 1979.<br />

[S61 M. Nararirnha. M. Abell, P. Hanagan, k Maenchen, and J. Montalvo.<br />

"The TM 7400-M2: An improved digital transmultiplexer<br />

with un~versal signalling," in Conf. Rec. ICC (Denver, CO), pp.<br />

7.2.1-7.2.5. 1981.<br />

[87] R. Marula. h Kanemasa, H. Sakaguchi, M. Hibino and N. Kawayachi.<br />

"A 24.channel LSI transmultiplexer," in Con$ Rec. ICC<br />

(Denver. CO), pp. 7.5.1-7.5.5, 1981.<br />

[88] K. Wakabayarhl. T. Aoyama, K Murano, F. Amano, and T.<br />

Tsuda. "TDM-FDM transmultiplexer using a digital signal processor."<br />

In Conl. Rec. ICC(Denver, CO), pp. 7.6.1-7.6.5, 1981.<br />

[89] I. Versvik. "Design of a digital transmultiplexer using standard<br />

TTL-lopc." In Conf. Rec. ICC (Denver, CO), pp. 7.1.1-7.1.6,<br />

1981.<br />

[90] H. Gockler and H. Scheuermann, "A modular approach to a digital<br />

60-channel transmultiplexer using directional filters," IEEE<br />

Trans. Commun. Technol., to be published.<br />

[91] H. Gockler and H. Scheuermann, "A per-channel transmultiplexer<br />

applying 1IR filters with logarithmic processing," in preparation.<br />

[92] R. E. Crochiere and L. R. Rabiner, "Interpolation and decimation<br />

of digital signals-A tuto&l review," Proc. IEEE, vol. 69, pp.<br />

300-331, Mar. 1981.


PROCEEDINGS OF THE IEEE, VOL. 70, NO. 7, JULY 1982<br />

Then, the real output signals of the DFT processor can most easily be<br />

<strong>der</strong>ived, if the samples of the complex signals (26) are taken at odd<br />

multiples of vT/2 (instead of integer multiples of vT) leading to a<br />

W-point odd-time inverse discrete Fourier transfo~m (IODFT)~ 1431<br />

Using (26), (27) may b'e factored into<br />

Correction to "A Comprehensive Survey of Digital<br />

Transmultiplexing Methods"<br />

<strong>HELMUT</strong> <strong>SCHEUERMANN</strong> <strong>AND</strong> HEINZ <strong>GOCKLER</strong><br />

In the above-titled survey paper1 the basic <strong>der</strong>ivation of the lowpass<br />

frlter-bank method at the beginning of section VI-B is somewhat<br />

erroneous. The correct <strong>der</strong>ivation is given leading to a minor modification<br />

of Fig. 18.' In addition, two errors are corrected as follows:<br />

B. Low-Pass Filter-Bank Method<br />

If one succeeds in obtaining real signals at the output of the Fourier<br />

processor, processing of "complex" signals in the polyphase network<br />

can be avoided. This is achieved if the complex input signals to a W-<br />

point DFT processor exhibit Herrnitian symmetry<br />

~ppiying the variable transformation K = 2N - r - 1, the second tern<br />

of (28) yields<br />

Thus there results from (28), if in its fust term r is replaced by K<br />

Manuscript received January 20, 1982.<br />

The authors are with AEG-Telefunken Nachrichtentechnik GmbH,<br />

Advanced Development Department, D-7150 Backnang, Germany.<br />

'H, Scheuermann and H. GocMer, Proc. ZEEE, vol. 69, pp. 1419-<br />

1450, NOV. 1981.<br />

a G. Bonnerot and M. Bellanger, "Odd-time odd-frequency discrete<br />

Fourier transform for symmetric real-valued series," Proc. ZEEE, vol.<br />

64, pp. 392-393, Mar. 1976.


PROCEEDINGS OF THE IEEE, VOL.,70, NO. 7, JULY 1982<br />

From this, the z-transform of the transmultiplexer output sequence is<br />

obtained in the natural sequential or<strong>der</strong> of summation<br />

and, accordingly, by interchanging the summation or<strong>der</strong><br />

As a consequence, the IDFT processor in Fig. lgl must be replaced by<br />

a 2N-point IODFT processor.<br />

Finally, two errors are indicated: The fust sentence of the last paragraph<br />

of p. 1432 should read: "Still another transmultiplexer, proposed<br />

by Tomlinson and Wong [48], [49], works according to the low-pass<br />

filter-bank method." Second, the author of 1631 is A. Fettweis.

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