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Sec. 3–6 Intersymbol Interference 185<br />

TABLE 3–6<br />

Code Type<br />

SPECTRAL EFFICIENCIES OF LINE CODES<br />

First Null Bandwidth<br />

(Hz)<br />

Spectral Efficiency<br />

h = RB [(bits/s)/Hz]<br />

Unipolar NRZ R 1<br />

Polar NRZ R 1<br />

1<br />

Unipolar RZ<br />

2R<br />

2<br />

Bipolar RZ R 1<br />

1<br />

Manchester NRZ<br />

2R<br />

2<br />

Multilevel polar NRZ R <br />

All of these binary line codes have h ≤ 1. Multilevel signaling can be used to achieve<br />

much greater spectral efficiency, but multilevel circuits are more costly. In practice, multilevel<br />

polar NRZ signaling is used in the T1G digital telephone lines, as described in Sec. 3–9.<br />

3–6 INTERSYMBOL INTERFERENCE<br />

The absolute bandwidth of rectangular multilevel pulses is infinity. If these pulses are filtered<br />

improperly as they pass through a communication system, they will spread in time, and the<br />

pulse for each symbol may be smeared into adjacent time slots and cause intersymbol interference<br />

(ISI), as illustrated in Fig. 3–23. Now, how can we restrict the bandwidth and still not<br />

introduce ISI? Of course, with a restricted bandwidth, the pulses would have rounded tops<br />

(instead of flat ones). This problem was first studied by Nyquist [1928]. He discovered three<br />

different methods for pulse shaping that could be used to eliminate ISI. Each of these methods<br />

will be studied in the sections that follow.<br />

Input waveform, w in (t)<br />

1 0 0 0<br />

Individual pulse response<br />

Received waveform, w out (t)<br />

(sum of pulse responses)<br />

0<br />

t<br />

0<br />

t<br />

0<br />

t<br />

1 0 1 1<br />

T s<br />

T s T s<br />

Intersymbol interference<br />

0 t 0 t 0<br />

t<br />

Sampling points<br />

(transmitter clock)<br />

Sampling points<br />

(receiver clock)<br />

Sampling points<br />

(receiver clock)<br />

Figure 3–23<br />

Examples of ISI on received pulses in a binary communication system.

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