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Tidy up for ROLI
author | Geogaddi\David <d.m.ronan@qmul.ac.uk> |
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date | Tue, 17 May 2016 18:50:19 +0100 |
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3 <title>1d Real-odd DFTs (DSTs) - FFTW 3.2.1</title> | |
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50 <a name="1d-Real-odd-DFTs-(DSTs)"></a> | |
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55 <hr> | |
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57 | |
58 <h4 class="subsection">4.8.4 1d Real-odd DFTs (DSTs)</h4> | |
59 | |
60 <p>The Real-odd symmetry DFTs in FFTW are exactly equivalent to the unnormalized | |
61 forward (and backward) DFTs as defined above, where the input array | |
62 X of length N is purely real and is also <dfn>odd</dfn> symmetry. In | |
63 this case, the output is odd symmetry and purely imaginary. | |
64 <a name="index-real_002dodd-DFT-302"></a><a name="index-RODFT-303"></a> | |
65 <a name="index-RODFT00-304"></a>For the case of <code>RODFT00</code>, this odd symmetry means that | |
66 <i>X<sub>j</sub> = -X<sub>N-j</sub></i>,where we take X to be periodic so that | |
67 <i>X<sub>N</sub> = X</i><sub>0</sub>. Because of this redundancy, only the first n real numbers | |
68 starting at j=1 are actually stored (the j=0 element is | |
69 zero), where N = 2(n+1). | |
70 | |
71 <p>The proper definition of odd symmetry for <code>RODFT10</code>, | |
72 <code>RODFT01</code>, and <code>RODFT11</code> transforms is somewhat more intricate | |
73 because of the shifts by 1/2 of the input and/or output, although | |
74 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, | |
75 the cosine terms in the DFT all cancel and the remaining sine terms are | |
76 written explicitly below. This formulation often leads people to call | |
77 such a transform a <dfn>discrete sine transform</dfn> (DST), although it is | |
78 really just a special case of the DFT. | |
79 <a name="index-discrete-sine-transform-305"></a><a name="index-DST-306"></a> | |
80 In each of the definitions below, we transform a real array X of | |
81 length n to a real array Y of length n: | |
82 | |
83 <h5 class="subsubheading">RODFT00 (DST-I)</h5> | |
84 | |
85 <p><a name="index-RODFT00-307"></a>An <code>RODFT00</code> transform (type-I DST) in FFTW is defined by: | |
86 <center><img src="equation-rodft00.png" align="top">.</center> | |
87 | |
88 <h5 class="subsubheading">RODFT10 (DST-II)</h5> | |
89 | |
90 <p><a name="index-RODFT10-308"></a>An <code>RODFT10</code> transform (type-II DST) in FFTW is defined by: | |
91 <center><img src="equation-rodft10.png" align="top">.</center> | |
92 | |
93 <h5 class="subsubheading">RODFT01 (DST-III)</h5> | |
94 | |
95 <p><a name="index-RODFT01-309"></a>An <code>RODFT01</code> transform (type-III DST) in FFTW is defined by: | |
96 <center><img src="equation-rodft01.png" align="top">.</center>In the case of n=1, this reduces to | |
97 <i>Y</i><sub>0</sub> = <i>X</i><sub>0</sub>. | |
98 | |
99 <h5 class="subsubheading">RODFT11 (DST-IV)</h5> | |
100 | |
101 <p><a name="index-RODFT11-310"></a>An <code>RODFT11</code> transform (type-IV DST) in FFTW is defined by: | |
102 <center><img src="equation-rodft11.png" align="top">.</center> | |
103 | |
104 <h5 class="subsubheading">Inverses and Normalization</h5> | |
105 | |
106 <p>These definitions correspond directly to the unnormalized DFTs used | |
107 elsewhere in FFTW (hence the factors of 2 in front of the | |
108 summations). The unnormalized inverse of <code>RODFT00</code> is | |
109 <code>RODFT00</code>, of <code>RODFT10</code> is <code>RODFT01</code> and vice versa, and | |
110 of <code>RODFT11</code> is <code>RODFT11</code>. Each unnormalized inverse results | |
111 in the original array multiplied by N, where N is the | |
112 <em>logical</em> DFT size. For <code>RODFT00</code>, N=2(n+1); | |
113 otherwise, N=2n. | |
114 <a name="index-normalization-311"></a> | |
115 In defining the discrete sine transform, some authors also include | |
116 additional factors of | |
117 √2(or its inverse) multiplying selected inputs and/or outputs. This is a | |
118 mostly cosmetic change that makes the transform orthogonal, but | |
119 sacrifices the direct equivalence to an antisymmetric DFT. | |
120 | |
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