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Update build for AUDIO_COMPONENT_FIX
author Chris Cannam
date Wed, 30 Oct 2019 12:40:34 +0000
parents 2cd0e3b3e1fd
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Chris@42 25 <title>FFTW 3.3.5: 1d Real-odd DFTs (DSTs)</title>
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Chris@42 72 <a name="g_t1d-Real_002dodd-DFTs-_0028DSTs_0029"></a>
Chris@42 73 <div class="header">
Chris@42 74 <p>
Chris@42 75 Next: <a href="1d-Discrete-Hartley-Transforms-_0028DHTs_0029.html#g_t1d-Discrete-Hartley-Transforms-_0028DHTs_0029" accesskey="n" rel="next">1d Discrete Hartley Transforms (DHTs)</a>, Previous: <a href="1d-Real_002deven-DFTs-_0028DCTs_0029.html#g_t1d-Real_002deven-DFTs-_0028DCTs_0029" accesskey="p" rel="prev">1d Real-even DFTs (DCTs)</a>, Up: <a href="What-FFTW-Really-Computes.html#What-FFTW-Really-Computes" accesskey="u" rel="up">What FFTW Really Computes</a> &nbsp; [<a href="index.html#SEC_Contents" title="Table of contents" rel="contents">Contents</a>][<a href="Concept-Index.html#Concept-Index" title="Index" rel="index">Index</a>]</p>
Chris@42 76 </div>
Chris@42 77 <hr>
Chris@42 78 <a name="g_t1d-Real_002dodd-DFTs-_0028DSTs_0029-1"></a>
Chris@42 79 <h4 class="subsection">4.8.4 1d Real-odd DFTs (DSTs)</h4>
Chris@42 80
Chris@42 81 <p>The Real-odd symmetry DFTs in FFTW are exactly equivalent to the unnormalized
Chris@42 82 forward (and backward) DFTs as defined above, where the input array
Chris@42 83 <em>X</em> of length <em>N</em> is purely real and is also <em>odd</em> symmetry. In
Chris@42 84 this case, the output is odd symmetry and purely imaginary.
Chris@42 85 <a name="index-real_002dodd-DFT-1"></a>
Chris@42 86 <a name="index-RODFT-1"></a>
Chris@42 87 </p>
Chris@42 88
Chris@42 89 <a name="index-RODFT00"></a>
Chris@42 90 <p>For the case of <code>RODFT00</code>, this odd symmetry means that
Chris@42 91 <i>X<sub>j</sub> = -X<sub>N-j</sub></i>,where we take <em>X</em> to be periodic so that
Chris@42 92 <i>X<sub>N</sub> = X</i><sub>0</sub>.Because of this redundancy, only the first <em>n</em> real numbers
Chris@42 93 starting at <em>j=1</em> are actually stored (the <em>j=0</em> element is
Chris@42 94 zero), where <em>N = 2(n+1)</em>.
Chris@42 95 </p>
Chris@42 96 <p>The proper definition of odd symmetry for <code>RODFT10</code>,
Chris@42 97 <code>RODFT01</code>, and <code>RODFT11</code> transforms is somewhat more intricate
Chris@42 98 because of the shifts by <em>1/2</em> of the input and/or output, although
Chris@42 99 the corresponding boundary conditions are given in <a href="Real-even_002fodd-DFTs-_0028cosine_002fsine-transforms_0029.html#Real-even_002fodd-DFTs-_0028cosine_002fsine-transforms_0029">Real even/odd DFTs (cosine/sine transforms)</a>. Because of the odd symmetry, however,
Chris@42 100 the cosine terms in the DFT all cancel and the remaining sine terms are
Chris@42 101 written explicitly below. This formulation often leads people to call
Chris@42 102 such a transform a <em>discrete sine transform</em> (DST), although it is
Chris@42 103 really just a special case of the DFT.
Chris@42 104 <a name="index-discrete-sine-transform-2"></a>
Chris@42 105 <a name="index-DST-2"></a>
Chris@42 106 </p>
Chris@42 107
Chris@42 108 <p>In each of the definitions below, we transform a real array <em>X</em> of
Chris@42 109 length <em>n</em> to a real array <em>Y</em> of length <em>n</em>:
Chris@42 110 </p>
Chris@42 111 <a name="RODFT00-_0028DST_002dI_0029"></a>
Chris@42 112 <h4 class="subsubheading">RODFT00 (DST-I)</h4>
Chris@42 113 <a name="index-RODFT00-1"></a>
Chris@42 114 <p>An <code>RODFT00</code> transform (type-I DST) in FFTW is defined by:
Chris@42 115 <center><img src="equation-rodft00.png" align="top">.</center></p>
Chris@42 116 <a name="RODFT10-_0028DST_002dII_0029"></a>
Chris@42 117 <h4 class="subsubheading">RODFT10 (DST-II)</h4>
Chris@42 118 <a name="index-RODFT10"></a>
Chris@42 119 <p>An <code>RODFT10</code> transform (type-II DST) in FFTW is defined by:
Chris@42 120 <center><img src="equation-rodft10.png" align="top">.</center></p>
Chris@42 121 <a name="RODFT01-_0028DST_002dIII_0029"></a>
Chris@42 122 <h4 class="subsubheading">RODFT01 (DST-III)</h4>
Chris@42 123 <a name="index-RODFT01"></a>
Chris@42 124 <p>An <code>RODFT01</code> transform (type-III DST) in FFTW is defined by:
Chris@42 125 <center><img src="equation-rodft01.png" align="top">.</center>In the case of <em>n=1</em>, this reduces to
Chris@42 126 <i>Y</i><sub>0</sub> = <i>X</i><sub>0</sub>.</p>
Chris@42 127 <a name="RODFT11-_0028DST_002dIV_0029"></a>
Chris@42 128 <h4 class="subsubheading">RODFT11 (DST-IV)</h4>
Chris@42 129 <a name="index-RODFT11"></a>
Chris@42 130 <p>An <code>RODFT11</code> transform (type-IV DST) in FFTW is defined by:
Chris@42 131 <center><img src="equation-rodft11.png" align="top">.</center></p>
Chris@42 132 <a name="Inverses-and-Normalization-1"></a>
Chris@42 133 <h4 class="subsubheading">Inverses and Normalization</h4>
Chris@42 134
Chris@42 135 <p>These definitions correspond directly to the unnormalized DFTs used
Chris@42 136 elsewhere in FFTW (hence the factors of <em>2</em> in front of the
Chris@42 137 summations). The unnormalized inverse of <code>RODFT00</code> is
Chris@42 138 <code>RODFT00</code>, of <code>RODFT10</code> is <code>RODFT01</code> and vice versa, and
Chris@42 139 of <code>RODFT11</code> is <code>RODFT11</code>. Each unnormalized inverse results
Chris@42 140 in the original array multiplied by <em>N</em>, where <em>N</em> is the
Chris@42 141 <em>logical</em> DFT size. For <code>RODFT00</code>, <em>N=2(n+1)</em>;
Chris@42 142 otherwise, <em>N=2n</em>.
Chris@42 143 <a name="index-normalization-11"></a>
Chris@42 144 </p>
Chris@42 145
Chris@42 146 <p>In defining the discrete sine transform, some authors also include
Chris@42 147 additional factors of
Chris@42 148 &radic;2(or its inverse) multiplying selected inputs and/or outputs. This is a
Chris@42 149 mostly cosmetic change that makes the transform orthogonal, but
Chris@42 150 sacrifices the direct equivalence to an antisymmetric DFT.
Chris@42 151 </p>
Chris@42 152 <hr>
Chris@42 153 <div class="header">
Chris@42 154 <p>
Chris@42 155 Next: <a href="1d-Discrete-Hartley-Transforms-_0028DHTs_0029.html#g_t1d-Discrete-Hartley-Transforms-_0028DHTs_0029" accesskey="n" rel="next">1d Discrete Hartley Transforms (DHTs)</a>, Previous: <a href="1d-Real_002deven-DFTs-_0028DCTs_0029.html#g_t1d-Real_002deven-DFTs-_0028DCTs_0029" accesskey="p" rel="prev">1d Real-even DFTs (DCTs)</a>, Up: <a href="What-FFTW-Really-Computes.html#What-FFTW-Really-Computes" accesskey="u" rel="up">What FFTW Really Computes</a> &nbsp; [<a href="index.html#SEC_Contents" title="Table of contents" rel="contents">Contents</a>][<a href="Concept-Index.html#Concept-Index" title="Index" rel="index">Index</a>]</p>
Chris@42 156 </div>
Chris@42 157
Chris@42 158
Chris@42 159
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