Exercise 1.10Z: Gaussian Band-Pass

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Gaussian bandpass channel

For this exercise we assume:

  • Binary phase modulation (BPSK) is used for modulation.
  • Demodulation is frequency and phase synchronous.


For carrier frequency modulated transmission, the channel frequency response  $H_{\rm K}(f)$  must always be assumed to be a bandpass. The channel parameters are, for example, the center frequency  $f_{\rm M}$  and the bandwidth  $\Delta f_{\rm K}$, where the center frequency  $f_{\rm M}$  often coincides with the carrier frequency  $f_{\rm T}$. 

In this exercise, in particular, we will assume a Gaussian bandpass according to the diagram. For its frequency response holds:

$$H_{\rm K}(f) = {\rm exp} \left [ - \pi \cdot \left ( \frac {f - f_{\rm M} }{\Delta f_{\rm K}}\right )^2 \right ] +{\rm exp} \left [ - \pi \cdot \left ( \frac {f + f_{\rm M} }{\Delta f_{\rm K}}\right )^2 \right ]$$

For a simpler description, one often uses the equivalent TP frequency response  $H_{\rm K,TP}(f)$. This results from  $H_{\rm K}(f)$  by

  • truncating the components at negative frequencies,
  • shifting the spectrum by  $f_{\rm T}$  to the left.


In the considered example with  $f_{\rm T} = f_{\rm M}$  for the equivalent TP frequency response results:

$$ H_{\rm K,\hspace{0.04cm} TP}(f) = {\rm e}^ { - \pi \hspace{0.04cm}\cdot \hspace{0.04cm}\left ( {f }/{\Delta f_{\rm K}}\right )^2 }.$$

The corresponding time function (Fourier inverse transform) is:

$$ h_{\rm K,\hspace{0.04cm} TP}(t) = \Delta f_{\rm K} \cdot {\rm e}^ { - \pi \hspace{0.04cm}\cdot \hspace{0.04cm}\left ( {\Delta f_{\rm K}} \cdot t \right )^2 }.$$

However, the frequency response is also suitable for describing a phase-synchronous BPSK system in the low-pass range

$$H_{\rm MKD}(f) = {1}/{2} \cdot \left [ H_{\rm K}(f-f_{\rm T}) + H_{\rm K}(f+f_{\rm T})\right ] ,$$

where "MKD" stands for modulator – channel (Kanal) – demodulator. Often - but not always -  $H_{\rm MKD}(f)$  and  $H_{\rm K,TP}(f)$  are identical.



Notes:


Questions

1

Give the impulse response  $h_{\rm K}(t)$  of the Gaussian bandpass channel. What is the (normalized) value for time  $t = 0$?

$ h_{\rm K}(t)/\Delta f_{\rm K} \ = \ $

2

Which statements are valid under the condition  $f_{\rm T} = f_{\rm M}$?

$H_{\rm K,TP}(f)$  and  $H_{\rm MKD}(f)$  coincide completely.
$H_{\rm K,TP}(f)$  and  $H_{\rm MKD}(f)$  are the same for low frequencies.
The time function  $h_{\rm K,TP}(t)$  is real.
The time function  $h_{\rm MKD}(t)$  is real.

3

Which statements are true under the condition $f_{\rm T} \neq f_{\rm M}$?

$H_{\rm K,TP}(f)$  and  $H_{\rm MKD}(f)$  coincide completely.
$H_{\rm K,TP}(f)$  and  $H_{\rm MKD}(f)$  are the same for low frequencies.
The time function  $h_{\rm K,TP}(t)$  is real.
The time function  $h_{\rm MKD}(t)$  is real.

4

What should be true with respect to a smaller bit error probability?

$f_{\rm M} = f_{\rm T}$,
$f_{\rm M} \neq f_{\rm T}$.


Solution

(1)  For the bandpass frequency response $H_{\rm K}(f)$ we can write:

$$H_{\rm K}(f) = H_{\rm K,\hspace{0.04cm} TP}(f) \star \big [ \delta (f - f_{\rm M}) + \delta (f + f_{\rm M}) \big ] .$$
  • The Fourier inverse transform of the bracket expression yields a cosine function of frequency $f_{\rm M}$ with amplitude $2$.
  • Thus, according to the convolution theorem:
$$h_{\rm K}(t) = 2 \cdot \Delta f_{\rm K} \cdot {\rm exp} \left [ - \pi \cdot \left ( {\Delta f_{\rm K}} \cdot t \right )^2 \right ] \cdot \cos(2 \pi f_{\rm M} t ) \hspace{0.3cm} \Rightarrow \hspace{0.3cm}h_{\rm K}(t = 0)/\Delta f_{\rm K} \hspace{0.1cm}\underline {= 2}.$$
  • This means: The TP impulse response $h_{\rm K,\hspace{0.04cm}TP}(t)$ is identical in shape to the envelope of the bp impulse response $h_{\rm K}(t)$, but twice as large.


(2)  Statements 2, 3 and 4 are correct:

  • The first statement is false because $H_{\rm MKD}(f)$ also has components around $\pm 2f_{\rm T}$.
  • The time function $h_{\rm K,\hspace{0.04cm}TP}(t)$ is real according to the given equation.
  • The same is true for $h_{\rm MKD}(t)$ also considering the $\pm 2f_{\rm T}$ components, since $H_{\rm MKD}(f)$ is an even function with respect to $f = 0$.
  • The diagram shows $H_{\rm MKD}(f)$, which also has components around $\pm 2f_{\rm T}$. At low frequencies, $H_{\rm K,\hspace{0.04cm}TP}(f)$ is identical to $H_{\rm MKD}(f)$.


Resulting baseband frequency response for $f_{\rm M} = f_{\rm T}$

(3)  Only solution 4 is correct:

  • Here $H_{\rm K,\hspace{0.04cm}TP}(f)$ and $H_{\rm MKD}(f)$ differ even at the low frequencies.
  • $H_{\rm K,\hspace{0.04cm}TP}(f)$ is a Gaussian function with the maximum at $f_{ε} = f_{\rm M} - f_{\rm T}$.
  • Because of this asymmetry, $h_{\rm K,\hspace{0.04cm}TP}(t)$ is complex.
  • In contrast, $H_{\rm MKD}(f)$ is still an even function with respect to $f = 0$ with real impulse response $h_{\rm MKD}(t)$.
  • $H_{\rm MKD}(f)$ is composed of two Gaussian functions at $± f_ε$.


Resulting baseband frequency response for $f_{\rm M} \ne f_{\rm T}$

(4)  Correct is of course the first answer.