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25 <title>FFTW 3.3.5: 1d Real-even DFTs (DCTs)</title>
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72 <a name="g_t1d-Real_002deven-DFTs-_0028DCTs_0029"></a>
73 <div class="header">
74 <p>
75 Next: <a href="1d-Real_002dodd-DFTs-_0028DSTs_0029.html#g_t1d-Real_002dodd-DFTs-_0028DSTs_0029" accesskey="n" rel="next">1d Real-odd DFTs (DSTs)</a>, Previous: <a href="The-1d-Real_002ddata-DFT.html#The-1d-Real_002ddata-DFT" accesskey="p" rel="prev">The 1d Real-data DFT</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>
76 </div>
77 <hr>
78 <a name="g_t1d-Real_002deven-DFTs-_0028DCTs_0029-1"></a>
79 <h4 class="subsection">4.8.3 1d Real-even DFTs (DCTs)</h4>
80
81 <p>The Real-even symmetry DFTs in FFTW are exactly equivalent to the unnormalized
82 forward (and backward) DFTs as defined above, where the input array
83 <em>X</em> of length <em>N</em> is purely real and is also <em>even</em> symmetry. In
84 this case, the output array is likewise real and even symmetry.
85 <a name="index-real_002deven-DFT-1"></a>
86 <a name="index-REDFT-1"></a>
87 </p>
88
89 <a name="index-REDFT00"></a>
90 <p>For the case of <code>REDFT00</code>, this even symmetry means that
91 <i>X<sub>j</sub> = X<sub>N-j</sub></i>,where we take <em>X</em> to be periodic so that
92 <i>X<sub>N</sub> = X</i><sub>0</sub>.Because of this redundancy, only the first <em>n</em> real numbers are
93 actually stored, where <em>N = 2(n-1)</em>.
94 </p>
95 <p>The proper definition of even symmetry for <code>REDFT10</code>,
96 <code>REDFT01</code>, and <code>REDFT11</code> transforms is somewhat more intricate
97 because of the shifts by <em>1/2</em> of the input and/or output, although
98 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,
99 the sine terms in the DFT all cancel and the remaining cosine terms are
100 written explicitly below. This formulation often leads people to call
101 such a transform a <em>discrete cosine transform</em> (DCT), although it is
102 really just a special case of the DFT.
103 <a name="index-discrete-cosine-transform-2"></a>
104 <a name="index-DCT-2"></a>
105 </p>
106
107 <p>In each of the definitions below, we transform a real array <em>X</em> of
108 length <em>n</em> to a real array <em>Y</em> of length <em>n</em>:
109 </p>
110 <a name="REDFT00-_0028DCT_002dI_0029"></a>
111 <h4 class="subsubheading">REDFT00 (DCT-I)</h4>
112 <a name="index-REDFT00-1"></a>
113 <p>An <code>REDFT00</code> transform (type-I DCT) in FFTW is defined by:
114 <center><img src="equation-redft00.png" align="top">.</center>Note that this transform is not defined for <em>n=1</em>. For <em>n=2</em>,
115 the summation term above is dropped as you might expect.
116 </p>
117 <a name="REDFT10-_0028DCT_002dII_0029"></a>
118 <h4 class="subsubheading">REDFT10 (DCT-II)</h4>
119 <a name="index-REDFT10"></a>
120 <p>An <code>REDFT10</code> transform (type-II DCT, sometimes called &ldquo;the&rdquo; DCT) in FFTW is defined by:
121 <center><img src="equation-redft10.png" align="top">.</center></p>
122 <a name="REDFT01-_0028DCT_002dIII_0029"></a>
123 <h4 class="subsubheading">REDFT01 (DCT-III)</h4>
124 <a name="index-REDFT01"></a>
125 <p>An <code>REDFT01</code> transform (type-III DCT) in FFTW is defined by:
126 <center><img src="equation-redft01.png" align="top">.</center>In the case of <em>n=1</em>, this reduces to
127 <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> (&ldquo;the&rdquo; DCT), and so the <code>REDFT01</code> (DCT-III) is sometimes called the &ldquo;IDCT&rdquo;.
128 <a name="index-IDCT-3"></a>
129 </p>
130 <a name="REDFT11-_0028DCT_002dIV_0029"></a>
131 <h4 class="subsubheading">REDFT11 (DCT-IV)</h4>
132 <a name="index-REDFT11"></a>
133 <p>An <code>REDFT11</code> transform (type-IV DCT) in FFTW is defined by:
134 <center><img src="equation-redft11.png" align="top">.</center></p>
135 <a name="Inverses-and-Normalization"></a>
136 <h4 class="subsubheading">Inverses and Normalization</h4>
137
138 <p>These definitions correspond directly to the unnormalized DFTs used
139 elsewhere in FFTW (hence the factors of <em>2</em> in front of the
140 summations). The unnormalized inverse of <code>REDFT00</code> is
141 <code>REDFT00</code>, of <code>REDFT10</code> is <code>REDFT01</code> and vice versa, and
142 of <code>REDFT11</code> is <code>REDFT11</code>. Each unnormalized inverse results
143 in the original array multiplied by <em>N</em>, where <em>N</em> is the
144 <em>logical</em> DFT size. For <code>REDFT00</code>, <em>N=2(n-1)</em> (note that
145 <em>n=1</em> is not defined); otherwise, <em>N=2n</em>.
146 <a name="index-normalization-10"></a>
147 </p>
148
149 <p>In defining the discrete cosine transform, some authors also include
150 additional factors of
151 &radic;2(or its inverse) multiplying selected inputs and/or outputs. This is a
152 mostly cosmetic change that makes the transform orthogonal, but
153 sacrifices the direct equivalence to a symmetric DFT.
154 </p>
155 <hr>
156 <div class="header">
157 <p>
158 Next: <a href="1d-Real_002dodd-DFTs-_0028DSTs_0029.html#g_t1d-Real_002dodd-DFTs-_0028DSTs_0029" accesskey="n" rel="next">1d Real-odd DFTs (DSTs)</a>, Previous: <a href="The-1d-Real_002ddata-DFT.html#The-1d-Real_002ddata-DFT" accesskey="p" rel="prev">The 1d Real-data DFT</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>
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