Aufgaben:Exercise 2.5: Scatter Function

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Delay-Doppler profile

For the mobile radio channel as a time-variant system, there are a total of four system functions that are linked with each other via the Fourier transform.  With the nomenclature from our tutorial, these are:

• the time-variant impulse response  $h(\tau, \hspace{0.05cm}t)$, which we also denote here as  $\eta_{\rm VZ}(\tau,\hspace{0.05cm} t)$,
• the delay-Doppler function  $\eta_{\rm VD}(\tau,\hspace{0.05cm} f_{\rm D})$,
• the frequency-Doppler function  $\eta_{\rm FD}(f, \hspace{0.05cm}f_{\rm D})$,
• the time-variant transfer function  $\eta_{\rm FZ}(f,\hspace{0.05cm}t)$  or  $H(f, \hspace{0.05cm}t)$.

The four possible system functions are uniformly denoted by  $\boldsymbol{\eta}_{12}$ .

• The first subindex is either a  $\boldsymbol{\rm V}$  $($because of German  $\rm V\hspace{-0.05cm}$erzögerung   ⇒   delay time  $\tau)$  or  a  $\boldsymbol{\rm F}$  $($frequency  $f)$.
  

• Either a  $\boldsymbol{\rm Z}$  $($because of German  $\rm Z\hspace{-0.05cm}$eit   ⇒   time  $t)$  or a  $\boldsymbol{\rm D}$  $($Doppler frequency  $f_{\rm D})$  is possible as the second subindex.

The delay–Doppler function  $\eta_{\rm VD}(\tau,\hspace{0.05cm} f_{\rm D})$  is shown in the plot:

$$\eta_{\rm VD}(\tau, f_{\rm D}) \hspace{-0.1cm} \ = \ \hspace{-0.1cm} \frac{1}{\sqrt{2}} \cdot \delta (\tau) \cdot \delta (f_{\rm D} - 100\,{\rm Hz})-$$

$$\hspace{1.75cm} \ - \ \hspace{-0.1cm} \frac{1}{2} \cdot \delta (\tau- 1\,{\rm \mu s}) \cdot \delta (f_{\rm D} - 50\,{\rm Hz})-\frac{1}{2} \cdot \delta (\tau- 1\,{\rm \mu s}) \cdot \delta (f_{\rm D} + 50\,{\rm Hz})\hspace{0.05cm}.$$

In the literature,  $\eta_{\rm VD}(\tau, \hspace{0.05cm}f_{\rm D})$  is often also called  scatter function  and denoted with  $s(\tau, \hspace{0.05cm}f_{\rm D})$ .

In this task, the associated delay–time function  $\eta_{\rm VZ}(\tau, \hspace{0.05cm}t)$  and the frequency–Doppler function  $\eta_{\rm FD}(f, \hspace{0.05cm}f_{\rm D})$  are to be determined.

Notes:

• This exercise should clarify the subject matter of the chapter  The GWSSUS Channel Model.
• The relationship between the individual system functions is given in the  graph on the first page  of this chapter.
• Note that the magnitude function  $|\eta_{\rm VD}(\tau, \hspace{0.05cm} f_{\rm D})|$  is shown above, so negative weights of the Dirac functions cannot be recognized.

Questionnaire

1 At which values of  $\tau$  there are the components of 2D impulse response  $\eta_{\rm VZ}(\tau, \hspace{0.05cm}t)$ ?

	$\tau = 0$,
	$\tau = 1 \ \rm µ s$,
	other $\tau$–values.

2 Calculate  $|\eta_{\rm VZ}(\tau = 0,\hspace{0.05cm}t)|$.  Which of the following statements are true?

	$|\eta_{\rm VZ}(\tau = 0,\hspace{0.05cm} t)|$  is independent of  $t$.
	$\eta_{\rm VZ}(\tau = 0, \hspace{0.05cm}t) = A \cdot \cos {(2\pi f_0 t)}$.
	$\eta_{\rm VZ}(\tau = 0, \hspace{0.05cm}t) = A \cdot \sin {(2\pi f_0 t)}$.

3 Calculate  $|\eta_{\rm VZ}(\tau = 1 \ {\rm µ s},\hspace{0.05cm} t)|$.  Which of the following statements are true?

	$|\eta_{\rm VZ}(\tau = 1 \ {\rm µ s},\hspace{0.05cm} t)|$  is independent of  $t$.
	$\eta_{\rm VZ}(\tau = 1 \ {\rm µ s}, \hspace{0.05cm}t) = A \cdot \cos {(2\pi f_0 t)}$.
	$\eta_{\rm VZ}(\tau = 1 \ {\rm µ s}, \hspace{0.05cm}t) = A \cdot \sin {(2\pi f_0 t)}$.

4 Consider the frequency–Doppler representation  $\eta_{\rm FD}(f, \hspace{0.05cm}f_{\rm D})$.  For which values of  $f_{\rm D}$ is this function not equal to zero?

	$f_{\rm D} = 0$,
	$f_{\rm D} = ± 50 \ \rm Hz$,
	$f_{\rm D} = ± 100 \ \rm Hz$.

5 Which of the following statements are true for  $\eta_{\rm FD}(f,\hspace{0.05cm} f_{\rm D})$?

	$|\eta_{\rm FD}(f,\hspace{0.05cm} f_{\rm D} = 100 \ \rm Hz)|$  is independent of $f_{\rm D}$.
	$\eta_{\rm FD}(f, \hspace{0.05cm} f_{\rm D} = 50 \ {\rm Hz}) = A \cdot \cos {(2\pi t_0 f)}$.
	$\eta_{\rm FD}(f, \hspace{0.05cm}f_{\rm D} = 50 \ {\rm Hz}) = A \cdot \sin {(2\pi t_0 f)}$.

6 How do you get the time-variant transfer function  $\eta_{\rm FZ}(f, \hspace{0.05cm}t)$?

	By Fourier transformation of  $\eta_{\rm VD}(\tau,\hspace{0.05cm} f_{\rm D})$  with respect to  $\tau$.
	By Fourier transformation of  $\eta_{\rm VZ}(\tau, \hspace{0.05cm}t)$  with respect to  $\tau$.
	By inverse Fourier transformation of  $\eta_{\rm FD}(f,\hspace{0.05cm} f_{\rm D})$  with respect to $f_{\rm D}$.

Solution

Solution

(1)  The time-variant impulse response  $h(\tau, \hspace{0.05cm} t) = \eta_{\rm VZ}(\tau, \hspace{0.05cm} t)$  is the inverse Fourier transform of the delay–Doppler function  $\eta_{\rm VD}(\tau,\hspace{0.05cm} f_{\rm D}) = s(\tau, \hspace{0.05cm} f_{\rm D})$:

$$\eta_{\rm VZ}(\tau, \hspace{0.05cm} t)\hspace{0.2cm} \stackrel{t, \hspace{0.02cm}f_{\rm D}}{\circ\!\!-\!\!\!-\!\!\!-\!\!\bullet} \hspace{0.2cm} \eta_{\rm VD}(\tau, f_{\rm D})\hspace{0.05cm}.$$

• Accordingly,  $\eta_{\rm VZ}(\tau,\hspace{0.05cm} t)=0$  for the values of  $\tau$  that make  $\eta_{\rm VD}(\tau, f_{\rm D})=0$.
• Correct are therefore the solutions 1 and 2: 
  Only for  $\tau = 0$  and  $\tau = 1 \ \ \rm \mu s$  does the time-variant impulse response have non-zero values.

(2)  For the delay  $\tau = 0$, the scatter function  $\eta_{\rm VD}$  consists of a single Dirac at $f_{\rm D} = 100 \ \rm Hz$.

• According to the second Fourier integral, the desired time-domain function satisfies:

$$\eta_{\rm VZ}(\tau = 0, t) \hspace{-0.1cm} \ = \ \hspace{-0.1cm} \frac{1}{\sqrt{2}} \cdot \int\limits_{-\infty}^{+\infty} \delta (f_{\rm D} - 100\,{\rm Hz}) \cdot {\rm e}^{{\rm j}\hspace{0.05cm}\cdot\hspace{0.05cm} 2 \pi f_{\rm D} t}\hspace{0.15cm}{\rm d}f_{\rm D} =\frac{1}{\sqrt{2}} \cdot {\rm e}^{ {\rm j}\hspace{0.05cm}\cdot \hspace{0.05cm}2 \pi t \hspace{0.05cm}\cdot \hspace{0.05cm}100\,{\rm Hz}} .$$

• Correct is solution 1.

(3)  For the delay  $\tau = 1 \ \ \rm µ s$  the delay–Doppler function consists of two Dirac functions at  $±50 \ \rm Hz$, each with weight  $-0.5$.

• The time function is  $\eta_{\rm VZ}(\tau = 1\,{\rm \mu s}, t) = - \cos( 2 \pi t \cdot 50\,{\rm Hz})\hspace{0.05cm}.$

• This function can be represented with  $A = -1$  and  $f_0 = 50 \ \rm Hz$  according to solution 2.

(4)  The three Dirac functions  $\eta_{\rm VD}(\tau, \hspace{0.05cm}f_{\rm D})$  are at the Doppler frequencies  $+100 \ \rm Hz$, $+50 \ \rm Hz$  and  $-50 \ \rm Hz$.

• For all other Doppler frequencies, we must have  $\eta_{\rm FD}(f, \hspace{0.05cm}f_{\rm D}) \equiv 0$.
• Solution 2 is correct.

(5)  If you look at the scatter function  $\eta_{\rm VD}(\tau, \hspace{0.05cm}f_{\rm D})$  in the direction of the  $\tau$–axis, there is one Dirac function at each of the Doppler frequencies  $100 \ \rm Hz$  and  $±50 \ \rm Hz$.

• Here, depending on $f$,  complex exponential oscillations with constant magnitude result in each case  (from which it follows that solution 1 is correct):

$$|\eta_{\rm FD}(f, \hspace{0.05cm}f_{\rm D} = 100\,{\rm Hz})| \hspace{-0.1cm} \ = \ \hspace{-0.1cm} {1}/{\sqrt{2}} = {\rm const.}$$

$$| \eta_{\rm FD}(f, \hspace{0.05cm}f_{\rm D}= \pm 50\,{\rm Hz})| \hspace{-0.1cm} \ = \ \hspace{-0.1cm} 0.5 = {\rm const.}$$

Relationships between all system functions

(6)  As can be seen from the given graph, solutions 2 and 3 are correct.

• The graph shows all system functions.
• The Fourier correspondences (shown in green) illustrate the relationships between these system functions.

Note:

Compare the time-variant transfer function  $|\eta_{\rm FZ}(f, \hspace{0.05cm} t)|$  in the bottom right figure with the corresponding graph in  Exercise 2.4:

• The respective magnitude functions differ significantly, although  $|\eta_{\rm VZ}(\tau, t)|$  is the same in both cases.
• In Exercise 2.4, a cosine was implicitly assumed for  $\eta_{\rm VZ}(\tau = 1 \ {\rm µ s}, t)$;  here we have a negative cosine function.
• The (not explicitly) specified delay–Doppler function for Exercise 2.4 was

$$\eta_{\rm VD}(\tau, f_{\rm D}) \hspace{-0.1cm} \ = \ \hspace{-0.1cm} \frac{1}{\sqrt{2}} \cdot \delta (\tau) \cdot \delta (f_{\rm D} - 100\,{\rm Hz})+$$

$$\hspace{2cm}+\hspace{0.22cm}\frac{1}{2} \cdot \delta (\tau- 1\,{\rm \mu s}) \cdot \delta (f_{\rm D} - 50\,{\rm Hz})+ $$

$$\hspace{2cm}+\hspace{0.22cm} \frac{1}{2} \cdot \delta (\tau- 1\,{\rm \mu s}) \cdot \delta (f_{\rm D} + 50\,{\rm Hz})\hspace{0.05cm}.$$

• Comparison with the equation in this task shows that only the signs of the Diracs have changed at  $\tau = 1 \ \rm µ s$.