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The Fourier Transform and its applications goals: present the Fourier ...

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Proof:<br />

1) for <strong>the</strong> Cosine back-trafo:<br />

define an even function for all x : f 1� x �= f �∣x∣�={<br />

Its FT is<br />

FT � f 1 � x ��=F 1 �s�=CT �e 1 � x��<br />

� CT� f 1� x��<br />

−i ST � �o1 �x ��=CT<br />

� f � x��=F C �s�<br />

,<br />

=0<br />

which is also even, being a pure cosine transform:<br />

F 1 �−s�=F 1 �s� , resp. E 1 �s�=F 1 �s � , O 1 �s�=0<br />

Its back-transform reproduces f 1 � x � :<br />

f 1� x �=FT �i � F 1 �s��=CT � E 1�s��<br />

� CT� F 1 �s��<br />

�i ST �O 1 �s��<br />

� =0<br />

� �<br />

=0<br />

ST�F 2 �s��<br />

<strong>The</strong> <strong>Fourier</strong> <strong>Transform</strong> <strong>and</strong> <strong>its</strong> Applications, Jürgen Stutzki, Sommersemester 2007<br />

f � x � , x�0<br />

f �−x � , x�0 , i.e. e 1 � x �= f 1 � x� , o 1 �x �=0 .<br />

=CT �CT � f �∣x∣���<br />

<strong>and</strong> for<br />

x�0 , where f �x � is defined: f � x �= f 1 � x �=CT �CT � f � x �� �=CT � F C � s� � q.e.d.<br />

2) similarly for <strong>the</strong> Sine backtrafo, but with <strong>the</strong> odd function f 2 �x �={ f � x � , x�0<br />

− f �−x � , x�0 :<br />

FT � f 2� x��=F 2�s�=CT � �e 2� x��<br />

=0<br />

−i ST ��o 2� x ��<br />

ST � f 2�x�� =−i ST � f �x ��=−i F S�s� , <strong>and</strong><br />

f 2�x�=FT �i � F 2�s��=CT � E2�s�� �i ST �O 2�s�� =i �−i�ST � F s�s��=ST �ST � f �∣x∣�� �<br />

q.e.d.<br />

Page 24

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