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Simulink Tutorial on Digital Modulation Methods - Cengage Learning

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590 CHAPTER 13. SIMULINK TUTORIAL ON DIGITAL MODULATION<br />

2. The maximum horiz<strong>on</strong>tal eye opening of T is obtained <strong>on</strong>ly for α = 1. The<br />

horiz<strong>on</strong>tal eye opening is determined by the transiti<strong>on</strong>s +1 →−1 and −1 →+1.<br />

Since for α = 1 the impulse resp<strong>on</strong>se satisfies<br />

⎧<br />

� � ⎪⎨<br />

1, n = 0<br />

nT<br />

1<br />

g =<br />

2<br />

2 , n =±1<br />

⎪⎩<br />

0, otherwise<br />

the respective lines in the eye pattern are zero at T/2.<br />

3. The bandwidth increases with increasing α. In the time domain the impulse<br />

resp<strong>on</strong>se is infinite in durati<strong>on</strong>. However, it decreases faster as α decreases.<br />

Now we examine square-root raised-cosine pulses with various roll-off factors (see<br />

Figure 13.18). Choose<br />

from the Pulse Shape menu.<br />

Pulse Shape > Root-RC<br />

Figure 13.18: Impulse resp<strong>on</strong>se and Fourier transform of a square-root raised-cosine<br />

pulse (α = 0.5)<br />

TUTORIAL PROBLEM<br />

Problem 13.5 [Square-Root RC Pulse]<br />

1. Are the zero ISI c<strong>on</strong>diti<strong>on</strong> and the maximum horiz<strong>on</strong>tal eye-opening c<strong>on</strong>diti<strong>on</strong><br />

met ?<br />

2. For which rolloff factor are square-root raised-cosine pulses and raised-cosine<br />

pulses identical?<br />

© 2013 <strong>Cengage</strong> <strong>Learning</strong>. All Rights Reserved. May not be scanned, copied or duplicated, or posted to a publicly accessible website, in whole or in part.

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