A signal x(t) is bandlimited to B Hz

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SUMMARY

A signal x(t) that is bandlimited to B Hz implies that its n-th power, denoted as x^{n}(t), is bandlimited to nB Hz. The Fourier transform of a band-limited signal is represented by a Heaviside step function, X(f) = c(f) θ(B - |f|). The convolution of two band-limited signals A(f) and B(f) results in another band-limited signal, with the convolution's band limit determined by the individual band limits B_{1} and B_{2}. Mathematical induction can be employed to rigorously prove the band limit of the n-th power of the signal.

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  • Familiarity with convolution operations in signal processing
  • Basic principles of mathematical induction
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A singal x(t) is bandlimited to B Hz. Show that that the signal [tex]x^{n}(t)[/tex] is bandlimited to nB Hz.

I have no idee on how to address this problem. Can get some help?
 
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A band-limited signal has a Fourier component containing a heaviside step function:

[tex] X(f) = c(f) \theta(B - |f|)[/tex]

The Fourier transform of a product of two functions is their convolution:

[tex] \begin{array}{l}<br /> \mathrm{F.T.}[a(t) b(t)](f) = \int_{-\infty}^{\infty}{a(t) \, b(t) \, e^{-2\pi j f t} \, dt} \\ \\<br /> <br /> = \int_{-\infty}^{\infty}{dt \, e^{-2\pi j f t} \, \int_{-\infty}^{\infty}{A(f_{1}) \, e^{2\pi j f_{1} t} \, df_{1}} \, \int_{-\infty}^{\infty}{B(f_{2}) \, e^{2\pi j f_{2} t} \, df_{2}}} \\ \\<br /> <br /> = \int_{-\infty}^{\infty}{\int_{-\infty}^{\infty}{df_{1} \, df_{2} \, A(f_{1}) \, B(f_{2}) \, \int_{-\infty}^{\infty}{dt \, e^{2\pi j (f_{1} + f_{2} - f) t} \, dt}}} \\ \\<br /> <br /> = \int_{-\infty}^{\infty}{\int_{-\infty}^{\infty}{df_{1} \, df_{2} \, A(f_{1}) \, B(f_{2}) \, \delta(f_{1} + f_{2} - f)} \\ \\<br /> <br /> = \int_{-\infty}^{\infty}{A(f') \, B(f - f') \, df'}<br /> \end{array}[/tex]

Take the signals [itex]A(f)[/itex] and [itex]B(f)[/itex] to be band-limited with band limits [itex]B_{1}[/itex] and [itex]B_{2}[/itex], respectively. Then, their convolution is:

[tex] A \ast B(f) = \int_{-\infty}^{\infty}{A(f') \, \theta(B_{1} - |f'|) \, B(f - f') \, \theta(B_{2} - |f - f'|) \, df'}[/tex]

The integrand is non-zero only when:

[tex] \left\{\begin{array}{lcl}<br /> B_{1} - |f'| & \ge & 0 \\<br /> <br /> B_{2} - |f - f'| & \ge & 0<br /> \end{array}\right.[/tex]

These conditions limit the domain of integration with respect to [itex]f'[/itex]. But, they also give some necessary conditions on the possible values of [itex]f[/itex] when the above conditions are not contradictory. This makes the convolution also band limited. What is the band limit on the convolution in terms of [itex]B_{1}[/itex] and [itex]B_{2}[/itex]?

Then, use Mathematical Induction to prove the band limit of the [itex]n[/itex]-th power.
 

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