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author | Chris Cannam |
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date | Wed, 20 Mar 2013 15:35:50 +0000 |
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3 <title>1d Real-even DFTs (DCTs) - FFTW 3.3.3</title> | |
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49 <a name="1d-Real-even-DFTs-(DCTs)"></a> | |
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51 <p> | |
52 Next: <a rel="next" accesskey="n" href="1d-Real_002dodd-DFTs-_0028DSTs_0029.html#g_t1d-Real_002dodd-DFTs-_0028DSTs_0029">1d Real-odd DFTs (DSTs)</a>, | |
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55 <hr> | |
56 </div> | |
57 | |
58 <h4 class="subsection">4.8.3 1d Real-even DFTs (DCTs)</h4> | |
59 | |
60 <p>The Real-even 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>even</dfn> symmetry. In | |
63 this case, the output array is likewise real and even symmetry. | |
64 <a name="index-real_002deven-DFT-301"></a><a name="index-REDFT-302"></a> | |
65 | |
66 <p><a name="index-REDFT00-303"></a>For the case of <code>REDFT00</code>, this even symmetry means that | |
67 <i>X<sub>j</sub> = X<sub>N-j</sub></i>,where we take X to be periodic so that | |
68 <i>X<sub>N</sub> = X</i><sub>0</sub>. Because of this redundancy, only the first n real numbers are | |
69 actually stored, where N = 2(n-1). | |
70 | |
71 <p>The proper definition of even symmetry for <code>REDFT10</code>, | |
72 <code>REDFT01</code>, and <code>REDFT11</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 even symmetry, however, | |
75 the sine terms in the DFT all cancel and the remaining cosine terms are | |
76 written explicitly below. This formulation often leads people to call | |
77 such a transform a <dfn>discrete cosine transform</dfn> (DCT), although it is | |
78 really just a special case of the DFT. | |
79 <a name="index-discrete-cosine-transform-304"></a><a name="index-DCT-305"></a> | |
80 | |
81 <p>In each of the definitions below, we transform a real array X of | |
82 length n to a real array Y of length n: | |
83 | |
84 <h5 class="subsubheading">REDFT00 (DCT-I)</h5> | |
85 | |
86 <p><a name="index-REDFT00-306"></a>An <code>REDFT00</code> transform (type-I DCT) in FFTW is defined by: | |
87 <center><img src="equation-redft00.png" align="top">.</center>Note that this transform is not defined for n=1. For n=2, | |
88 the summation term above is dropped as you might expect. | |
89 | |
90 <h5 class="subsubheading">REDFT10 (DCT-II)</h5> | |
91 | |
92 <p><a name="index-REDFT10-307"></a>An <code>REDFT10</code> transform (type-II DCT, sometimes called “the” DCT) in FFTW is defined by: | |
93 <center><img src="equation-redft10.png" align="top">.</center> | |
94 | |
95 <h5 class="subsubheading">REDFT01 (DCT-III)</h5> | |
96 | |
97 <p><a name="index-REDFT01-308"></a>An <code>REDFT01</code> transform (type-III DCT) in FFTW is defined by: | |
98 <center><img src="equation-redft01.png" align="top">.</center>In the case of n=1, this reduces to | |
99 <i>Y</i><sub>0</sub> = <i>X</i><sub>0</sub>. Up to a scale factor (see below), this is the inverse of <code>REDFT10</code> (“the” DCT), and so the <code>REDFT01</code> (DCT-III) is sometimes called the “IDCT”. | |
100 <a name="index-IDCT-309"></a> | |
101 | |
102 <h5 class="subsubheading">REDFT11 (DCT-IV)</h5> | |
103 | |
104 <p><a name="index-REDFT11-310"></a>An <code>REDFT11</code> transform (type-IV DCT) in FFTW is defined by: | |
105 <center><img src="equation-redft11.png" align="top">.</center> | |
106 | |
107 <h5 class="subsubheading">Inverses and Normalization</h5> | |
108 | |
109 <p>These definitions correspond directly to the unnormalized DFTs used | |
110 elsewhere in FFTW (hence the factors of 2 in front of the | |
111 summations). The unnormalized inverse of <code>REDFT00</code> is | |
112 <code>REDFT00</code>, of <code>REDFT10</code> is <code>REDFT01</code> and vice versa, and | |
113 of <code>REDFT11</code> is <code>REDFT11</code>. Each unnormalized inverse results | |
114 in the original array multiplied by N, where N is the | |
115 <em>logical</em> DFT size. For <code>REDFT00</code>, N=2(n-1) (note that | |
116 n=1 is not defined); otherwise, N=2n. | |
117 <a name="index-normalization-311"></a> | |
118 | |
119 <p>In defining the discrete cosine transform, some authors also include | |
120 additional factors of | |
121 √2(or its inverse) multiplying selected inputs and/or outputs. This is a | |
122 mostly cosmetic change that makes the transform orthogonal, but | |
123 sacrifices the direct equivalence to a symmetric DFT. | |
124 | |
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