<?xml version="1.0" encoding="utf-8"?>
<!DOCTYPE document PUBLIC "-//CNX//DTD CNXML 0.5 plus MathML//EN" "http://cnx.rice.edu/cnxml/0.5/DTD/cnxml_mathml.dtd">
<document xmlns="http://cnx.rice.edu/cnxml" xmlns:m="http://www.w3.org/1998/Math/MathML" xmlns:md="http://cnx.rice.edu/mdml/0.4" xmlns:bib="http://bibtexml.sf.net/" id="m0525">

  <name>Discrete-Time Fourier Transform Pair</name>

  <metadata>
  <md:version>2.5</md:version>
  <md:created>2000/08/09</md:created>
  <md:revised>2003/07/24 10:53:30 GMT-5</md:revised>
  <md:authorlist>
      <md:author id="dhj">
      <md:firstname>Don</md:firstname>
      
      <md:surname>Johnson</md:surname>
      <md:email>dhj@rice.edu</md:email>
    </md:author>
  </md:authorlist>

  <md:maintainerlist>
    <md:maintainer id="prash">
      <md:firstname>Prashant</md:firstname>
      
      <md:surname>Singh</md:surname>
      <md:email>prash@ece.rice.edu</md:email>
    </md:maintainer>
    <md:maintainer id="richb">
      <md:firstname>Richard</md:firstname>
      <md:othername>G.</md:othername>
      <md:surname>Baraniuk</md:surname>
      <md:email>richb@rice.edu</md:email>
    </md:maintainer>
    <md:maintainer id="mariyah">
      <md:firstname>Mariyah</md:firstname>
      
      <md:surname>Poonawala</md:surname>
      <md:email>mariyah@rice.edu</md:email>
    </md:maintainer>
  </md:maintainerlist>
  
  <md:keywordlist>
    <md:keyword>analog</md:keyword>
    <md:keyword>digital</md:keyword>
    <md:keyword>discrete-time</md:keyword>
    <md:keyword>Fourier Transform</md:keyword>
    <md:keyword>frequency</md:keyword>
    <md:keyword>Nyquist</md:keyword>
  </md:keywordlist>

  <md:abstract>Computing discrete-time frequencies by the use of Fourier transforms.
</md:abstract>
</metadata>

  <content>

    <para id="p1">
      When we obtain the discrete-time signal via sampling an analog
      signal, the Nyquist frequency corresponds to the discrete-time
      frequency
      <m:math>
	<m:apply>
	  <m:divide/>
	  <m:cn>1</m:cn>
	  <m:cn>2</m:cn>
	</m:apply>
      </m:math>
      .  To show this, note that a sinusoid at the Nyquist frequency
      <m:math>
	<m:apply>
	  <m:divide/>
	  <m:cn>1</m:cn>
	  <m:apply>
	    <m:times/>
	    <m:cn>2</m:cn>
	    <m:ci><m:msub>
		<m:mi>T</m:mi>
		<m:mi>s</m:mi>
	      </m:msub></m:ci>
	  </m:apply>
	</m:apply>
      </m:math> 
      has a sampled waveform that equals

      <equation id="eqn0002">
	<name>Sinusoid at Nyquist Frequency 1/2T</name>
	<m:math>
	  <m:apply>
	    <m:eq/>
	    <m:apply>
	      <m:cos/>
	      <m:apply>
		<m:times/>
		<m:cn>2</m:cn>
		<m:pi/>
		<m:apply>
		  <m:divide/>
		  <m:cn>1</m:cn>
		  <m:apply>
		    <m:times/>
		    <m:cn>2</m:cn>
		    <m:ci><m:msub>
			<m:mi>T</m:mi>
			<m:mi>s</m:mi>
		      </m:msub></m:ci>
		  </m:apply>
		</m:apply>
		<m:ci>n</m:ci>
		<m:ci><m:msub>
		    <m:mi>T</m:mi>
		    <m:mi>s</m:mi>
		  </m:msub></m:ci>
	      </m:apply>
	    </m:apply>
	    <m:apply>
	      <m:cos/>
	      <m:apply>
		<m:times/>
		<m:pi/>
		<m:ci>n</m:ci>
	      </m:apply>
	    </m:apply>
	    <m:apply>
	      <m:power/>
	      <m:apply>
		<m:minus/>
		<m:cn>1</m:cn>
	      </m:apply>
	      <m:ci>n</m:ci>
	    </m:apply>
	  </m:apply>
	</m:math>
      </equation>
    </para>

    <para id="p2">
      The exponential in the DTFT at frequency 
      <m:math>
	<m:apply>
	  <m:divide/>
	  <m:cn>1</m:cn>
	  <m:cn>2</m:cn>
	</m:apply>
      </m:math> 
      equals 
      <m:math>
	<m:apply>
	  <m:eq/>
	  <m:apply>
	    <m:exp/>
	    <m:apply>
	      <m:divide/>
	      <m:apply>
		<m:minus/>
		<m:apply>
		  <m:times/>
		  <m:imaginaryi/>
		  <m:cn>2</m:cn>
		  <m:pi/>
		  <m:ci>n</m:ci>
		</m:apply>
	      </m:apply>
	      <m:cn>2</m:cn>
	    </m:apply>
	  </m:apply>
	  <m:apply>
	    <m:exp/>
	    <m:apply>
	      <m:minus/>
	      <m:apply>
		<m:times/>
		<m:imaginaryi/>
		<m:pi/>
		<m:ci>n</m:ci>
	      </m:apply>
	    </m:apply>
	  </m:apply>
	  <m:apply>
	    <m:power/>
	    <m:apply>
	      <m:minus/>
	      <m:cn>1</m:cn>
	    </m:apply>
	    <m:ci>n</m:ci>
	  </m:apply>
	</m:apply>
      </m:math>
      , meaning that the correspondence between analog and
      discrete-time frequency is established:

      <equation id="eqn0003">
	<name>Analog, Discrete-Time Frequency Relationship</name>
	<m:math>
	  <m:apply>
	    <m:eq/>
	    <m:ci>
	    <m:msub>
		<m:mi>f</m:mi>
		<m:mi>D</m:mi>
	      </m:msub>
	    </m:ci>
	    <m:apply>
	      <m:times/>
	      <m:ci>
		<m:msub>
		  <m:mi>f</m:mi>
		  <m:mi>A</m:mi>
		</m:msub>
	      </m:ci>
	      <m:ci>
		<m:msub>
		  <m:mi>T</m:mi>
		  <m:mi>s</m:mi>
		</m:msub>
	      </m:ci>
	    </m:apply>
	  </m:apply>    
	</m:math> 
      </equation>
    </para>

    <para id="p3">
      where 
      <m:math>
	<m:ci>
	  <m:msub>
	    <m:mi>f</m:mi>
	    <m:mi>D</m:mi>
	  </m:msub>
	</m:ci>
      </m:math> 
      and 
      <m:math>
	<m:ci>
	  <m:msub>
	    <m:mi>f</m:mi>
	    <m:mi>A</m:mi>
	  </m:msub>
	</m:ci>
      </m:math> represent discrete-time and analog frequency
      variables, respectively.  The <cnxn document="m0050" target="alias" strength="8">aliasing figure</cnxn> provides
      another way of deriving this result.  As the duration of each
      pulse in the periodic sampling signal
      <m:math>
	<m:apply>
	  <m:ci type="fn">
	    <m:msub>
	      <m:mi>p</m:mi>
	      <m:msub>
		<m:mi>T</m:mi>
		<m:mi>s</m:mi>
	      </m:msub>
	    </m:msub>
	  </m:ci>
	  <m:ci>t</m:ci>
	</m:apply>
      </m:math> narrows, the amplitudes of the signal's spectral
      repetitions, which are governed by the <cnxn document="m0050" target="pulse" strength="8">Fourier series coefficients</cnxn>
      of
      <m:math>
	<m:apply>
	  <m:ci type="fn">
	    <m:msub>
	      <m:mi>p</m:mi>
	      <m:msub>
		<m:mi>T</m:mi>
		<m:mi>s</m:mi>
	      </m:msub>
	    </m:msub>
	  </m:ci>
	  <m:ci>t</m:ci>
	</m:apply>
      </m:math>
      , become increasingly equal.  
      <note type="footnote">
	Examination of the <cnxn document="m0050" target="pulse" strength="8">periodic pulse signal</cnxn> reveals that as
      <m:math>
	<m:ci>Δ</m:ci>
      </m:math> 
      decreases, the value of
      <m:math>
	<m:ci>
	  <m:msub>
	    <m:mi>c</m:mi>
	    <m:mn>0</m:mn>
	  </m:msub>
	</m:ci>
      </m:math>
      , the largest Fourier coefficient, decreases to zero: 
      <m:math>
	<m:apply>
	  <m:eq/>
	  <m:apply>
	    <m:abs/>
	    <m:ci>
	      <m:msub>
		<m:mi>c</m:mi>
		<m:mn>0</m:mn>
	      </m:msub>
	    </m:ci>
	  </m:apply>
	  <m:apply>
	    <m:divide/>
	    <m:apply>
	      <m:times/>
	      <m:ci>A</m:ci>
	      <m:ci>Δ</m:ci>
	    </m:apply>
	    <m:ci>T</m:ci>
	  </m:apply>
	</m:apply>
      </m:math>
      .  Thus, to maintain a mathematically viable Sampling Theorem,
      the amplitude
      <m:math>
	<m:ci>A</m:ci>
      </m:math> 
      must increase as 
      <m:math>
	<m:apply>
	  <m:divide/>
	  <m:cn>1</m:cn>
	  <m:ci>Δ</m:ci>
	</m:apply>
      </m:math>
      , becoming infinitely large as the pulse duration decreases.
      Practical systems use a small value of
      <m:math>
	<m:ci>Δ</m:ci>
      </m:math>
      , say 
      <m:math>
	<m:apply>
	  <m:times/>
	  <m:cn>0.1</m:cn>
	  <m:ci><m:msub>
	      <m:mi>T</m:mi>
	      <m:mi>s</m:mi>
	    </m:msub></m:ci>
	</m:apply>
      </m:math> and use amplifiers to rescale the signal.
      </note>

      Thus, the sampled signal's spectrum becomes periodic with period
      <m:math>
	<m:apply>
	  <m:divide/>
	  <m:cn>1</m:cn>
	  <m:apply>
	    <m:times/>
	    <m:ci><m:msub>
		<m:mi>T</m:mi>
		<m:mi>s</m:mi>
	      </m:msub></m:ci>
	  </m:apply>
	</m:apply>
      </m:math>
      . Thus, the Nyquist frequency 
      <m:math>
	<m:apply>
	  <m:divide/>
	  <m:cn>1</m:cn>
	  <m:apply>
	    <m:times/>
	    <m:cn>2</m:cn>
	    <m:ci><m:msub>
		<m:mi>T</m:mi>
		<m:mi>s</m:mi>
	      </m:msub></m:ci>
	  </m:apply>
	</m:apply>
      </m:math>
      corresponds to the frequency 
      <m:math>
	<m:apply>
	  <m:divide/>
	  <m:cn>1</m:cn>
	  <m:cn>2</m:cn>
	</m:apply>
      </m:math>
      .
    </para>

    <para id="p4">
      The inverse discrete-time Fourier transform is easily derived
      from the following relationship:

    <equation id="eqn0012">
	<m:math>
	  <m:apply>
	    <m:eq/>
	    <m:apply>
	      <m:int/>
	      <m:uplimit>
		<m:apply>
		  <m:divide/>
		  <m:cn>1</m:cn>
		  <m:cn>2</m:cn>
		</m:apply>
	      </m:uplimit>
	      <m:lowlimit>
		<m:apply>
		  <m:minus/>
		  <m:apply>
		    <m:divide/>
		    <m:cn>1</m:cn>
		    <m:cn>2</m:cn>
		  </m:apply>
		</m:apply>
	      </m:lowlimit>
	      <m:bvar><m:ci>f</m:ci></m:bvar>
	      <m:apply>
		<m:times/>
		<m:apply>
		  <m:exp/>
		  <m:apply>
		    <m:minus/>
		    <m:apply>
		      <m:times/>
		      <m:imaginaryi/>
		      <m:cn>2</m:cn>
		      <m:pi/>
		      <m:ci>f</m:ci>
		      <m:ci>m</m:ci>
		    </m:apply>
		  </m:apply>
		</m:apply>
		<m:apply>
		  <m:exp/>
		  <m:apply>
		    <m:plus/>
		    <m:apply>
		      <m:times/>
		      <m:imaginaryi/>
		      <m:pi/>
		      <m:ci>f</m:ci>
		      <m:ci>n</m:ci>
		    </m:apply>
		  </m:apply>
		</m:apply>
	      </m:apply>
	    </m:apply>
	    <m:piecewise>
	      <m:piece>
		<m:cn>1</m:cn>
		<m:apply>
		  <m:eq/>
		  <m:ci>m</m:ci>
		  <m:ci>n</m:ci>
		</m:apply>
	      </m:piece>
	      <m:piece>
		<m:cn>0</m:cn>
		<m:apply>
		  <m:neq/>
		  <m:ci>m</m:ci>
		  <m:ci>n</m:ci>
		</m:apply>
	      </m:piece>
	    </m:piecewise>
	  </m:apply>
	</m:math>
      </equation>
    </para>

    <para id="p5">
      Therefore, we find that

      <equation id="eqn0013">
	<m:math>
	  <m:apply>
	    <m:eq/>
	    <m:apply>
	      <m:int/>
	      <m:bvar><m:ci>f</m:ci></m:bvar>
	      <m:lowlimit>
		<m:apply>
		  <m:minus/>
		  <m:apply>
		    <m:divide/>
		    <m:cn>1</m:cn>
		    <m:cn>2</m:cn>
		  </m:apply>
		</m:apply>
	      </m:lowlimit>
	      <m:uplimit>
		<m:apply>
		  <m:divide/>
		  <m:cn>1</m:cn>
		  <m:cn>2</m:cn>
		</m:apply>
	      </m:uplimit>
	      <m:apply>
		<m:times/>
		<m:apply>
		  <m:ci type="fn">S</m:ci>
		  <m:apply>
		    <m:exp/>
		    <m:apply>
		      <m:times/>
		      <m:imaginaryi/>
		      <m:cn>2</m:cn>
		      <m:pi/>
		      <m:ci>f</m:ci>
		    </m:apply>
		  </m:apply>
		</m:apply>
		<m:apply>
		  <m:exp/>
		  <m:apply>
		    <m:plus/>
		    <m:apply>
		      <m:times/>
		      <m:imaginaryi/>
		      <m:cn>2</m:cn>
		      <m:pi/>
		      <m:ci>f</m:ci>
		      <m:ci>n</m:ci>
		    </m:apply>
		  </m:apply>
		</m:apply>
	      </m:apply>
	    </m:apply>
	    <m:apply>
	      <m:int/>
	      <m:bvar><m:ci>f</m:ci></m:bvar>
	      <m:lowlimit>
		<m:apply>
		  <m:minus/>
		  <m:apply>
		    <m:divide/>
		    <m:cn>1</m:cn>
		    <m:cn>2</m:cn>
		  </m:apply>
		</m:apply>
	      </m:lowlimit>
	      <m:uplimit>
		<m:apply>
		  <m:divide/>
		  <m:cn>1</m:cn>
		  <m:cn>2</m:cn>
		</m:apply>
	      </m:uplimit>
	      <m:apply>
		<m:sum/>
		<m:bvar><m:ci>m</m:ci></m:bvar>
		<m:domainofapplication><m:ci>m</m:ci></m:domainofapplication>
		<m:apply>
		  <m:times/>
		  <m:apply>
		    <m:ci type="fn">s</m:ci>
		    <m:ci>m</m:ci>
		  </m:apply>
		  <m:apply>
		    <m:exp/>
		    <m:apply>
		      <m:minus/>
		      <m:apply>
			<m:times/>
			<m:imaginaryi/>
			<m:cn>2</m:cn>
			<m:pi/>
			<m:ci>f</m:ci>
			<m:ci>m</m:ci>
		      </m:apply>
		    </m:apply>
		  </m:apply>
		  <m:apply>
		    <m:exp/>
		    <m:apply>
		      <m:plus/>
		      <m:apply>
			<m:times/>
			<m:imaginaryi/>
			<m:cn>2</m:cn>
			<m:pi/>
			<m:ci>f</m:ci>
			<m:ci>n</m:ci>
		      </m:apply>
		    </m:apply>
		  </m:apply>
		</m:apply>
	      </m:apply>
	    </m:apply>
	    <m:apply>
	      <m:sum/>
	      <m:bvar><m:ci>m</m:ci></m:bvar>
	      <m:domainofapplication><m:ci>m</m:ci></m:domainofapplication>
	      <m:apply>
		<m:times/>
		<m:apply>
		  <m:ci type="fn">s</m:ci>
		  <m:ci>m</m:ci>
		</m:apply>
		<m:apply>
		  <m:int/>
		  <m:bvar><m:ci>f</m:ci></m:bvar>
		  <m:lowlimit>
		    <m:apply>
		      <m:minus/>
		      <m:apply>
			<m:divide/>
			<m:cn>1</m:cn>
			<m:cn>2</m:cn>
		      </m:apply>
		    </m:apply>
		  </m:lowlimit>
		  <m:uplimit>
		    <m:apply>
		      <m:divide/>
		      <m:cn>1</m:cn>
		      <m:cn>2</m:cn>
		    </m:apply>
		  </m:uplimit>
		  <m:apply>
		    <m:exp/>
		    <m:apply>
		      <m:times/>
		      <m:apply>
			<m:minus/>
			<m:apply>
			  <m:times/>
			  <m:imaginaryi/>
			  <m:cn>2</m:cn>
			  <m:pi/>
			  <m:ci>f</m:ci>
			</m:apply>
		      </m:apply>
		      <m:apply>
			<m:minus/>
			<m:ci>m</m:ci>
			<m:ci>n</m:ci>
		      </m:apply>
		    </m:apply>
		  </m:apply>
		</m:apply>
	      </m:apply>
	    </m:apply>
	    <m:apply>
	      <m:ci type="fn">s</m:ci>
	      <m:ci>n</m:ci>
	    </m:apply>
	  </m:apply>
	</m:math>
      </equation>
    </para>

    <para id="p6">
      The Fourier transform pairs in discrete-time are 

      <equation id="eqn0014a">
	<name>Fourier Transform Pairs in Discrete Time</name>
	<m:math>
	  <m:apply>
	    <m:eq/>
	    <m:apply>
	      <m:ci type="fn">S</m:ci>
	      <m:apply>
		<m:exp/>
		<m:apply>
		  <m:times/>
		  <m:imaginaryi/>
		  <m:cn>2</m:cn>
		  <m:pi/>
		  <m:ci>f</m:ci>
		</m:apply>
	      </m:apply>
	    </m:apply>
	    <m:apply>
	      <m:sum/>
	      <m:bvar><m:ci>n</m:ci></m:bvar>
	      <m:domainofapplication><m:ci>n</m:ci></m:domainofapplication>
	      <m:apply>
		<m:times/>
		<m:apply>
		  <m:ci type="fn">s</m:ci>
		  <m:ci>n</m:ci>
		</m:apply>
		<m:apply>
		  <m:exp/>
		  <m:apply>
		    <m:minus/>
		    <m:apply>
		      <m:times/>
		      <m:imaginaryi/>
		      <m:cn>2</m:cn>
		      <m:pi/>
		      <m:ci>f</m:ci>
		      <m:ci>n</m:ci>
		    </m:apply>
		  </m:apply>
		</m:apply>
	      </m:apply>
	    </m:apply>
	  </m:apply>
	</m:math> 
      </equation>

      <equation id="eqn0014b">
	<name>Fourier Transform Pairs in Discrete Time</name>
	<m:math>
	  <m:apply>
	    <m:eq/>
	    <m:apply>
	      <m:ci type="fn">s</m:ci>
	      <m:ci>n</m:ci>
	    </m:apply>
	    <m:apply>
	      <m:int/>
	      <m:bvar><m:ci>f</m:ci></m:bvar>
	      <m:lowlimit>
		<m:apply>
		  <m:minus/>
		  <m:apply>
		    <m:divide/>
		    <m:cn>1</m:cn>
		    <m:cn>2</m:cn>
		  </m:apply>
		</m:apply>
	      </m:lowlimit>
	      <m:uplimit>
		<m:apply>
		  <m:divide/>
		  <m:cn>1</m:cn>
		  <m:cn>2</m:cn>
		</m:apply>
	      </m:uplimit>
	      <m:apply>
	      <m:times/>
		<m:apply>
		  <m:ci type="fn">S</m:ci>
		  <m:apply>
		    <m:exp/>
		    <m:apply>
		      <m:times/>
		      <m:imaginaryi/>
		      <m:cn>2</m:cn>
		      <m:pi/>
		      <m:ci>f</m:ci>
		    </m:apply>
		  </m:apply>
		</m:apply>
		<m:apply>
		  <m:exp/>
		  <m:apply>
		    <m:plus/>
		    <m:apply>
		      <m:times/>
		      <m:imaginaryi/>
		      <m:cn>2</m:cn>
		      <m:pi/>
		      <m:ci>f</m:ci>
		      <m:ci>n</m:ci>
		    </m:apply>
		  </m:apply>
		</m:apply>
	      </m:apply>
	    </m:apply>
	  </m:apply>
	</m:math>
      </equation>
    </para>

  </content>
</document>
