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1 /*
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2 * jidctflt.c
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3 *
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4 * Copyright (C) 1994-1998, Thomas G. Lane.
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5 * This file is part of the Independent JPEG Group's software.
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6 *
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7 * The authors make NO WARRANTY or representation, either express or implied,
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8 * with respect to this software, its quality, accuracy, merchantability, or
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9 * fitness for a particular purpose. This software is provided "AS IS", and you,
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10 * its user, assume the entire risk as to its quality and accuracy.
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11 *
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12 * This software is copyright (C) 1991-1998, Thomas G. Lane.
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13 * All Rights Reserved except as specified below.
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14 *
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15 * Permission is hereby granted to use, copy, modify, and distribute this
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16 * software (or portions thereof) for any purpose, without fee, subject to these
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17 * conditions:
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18 * (1) If any part of the source code for this software is distributed, then this
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19 * README file must be included, with this copyright and no-warranty notice
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20 * unaltered; and any additions, deletions, or changes to the original files
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21 * must be clearly indicated in accompanying documentation.
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22 * (2) If only executable code is distributed, then the accompanying
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23 * documentation must state that "this software is based in part on the work of
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24 * the Independent JPEG Group".
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25 * (3) Permission for use of this software is granted only if the user accepts
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26 * full responsibility for any undesirable consequences; the authors accept
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27 * NO LIABILITY for damages of any kind.
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28 *
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29 * These conditions apply to any software derived from or based on the IJG code,
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30 * not just to the unmodified library. If you use our work, you ought to
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31 * acknowledge us.
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32 *
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33 * Permission is NOT granted for the use of any IJG author's name or company name
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34 * in advertising or publicity relating to this software or products derived from
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35 * it. This software may be referred to only as "the Independent JPEG Group's
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36 * software".
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37 *
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38 * We specifically permit and encourage the use of this software as the basis of
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39 * commercial products, provided that all warranty or liability claims are
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40 * assumed by the product vendor.
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41 *
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42 *
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43 * This file contains a floating-point implementation of the
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44 * inverse DCT (Discrete Cosine Transform). In the IJG code, this routine
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45 * must also perform dequantization of the input coefficients.
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46 *
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47 * This implementation should be more accurate than either of the integer
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48 * IDCT implementations. However, it may not give the same results on all
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49 * machines because of differences in roundoff behavior. Speed will depend
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50 * on the hardware's floating point capacity.
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51 *
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52 * A 2-D IDCT can be done by 1-D IDCT on each column followed by 1-D IDCT
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53 * on each row (or vice versa, but it's more convenient to emit a row at
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54 * a time). Direct algorithms are also available, but they are much more
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55 * complex and seem not to be any faster when reduced to code.
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56 *
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57 * This implementation is based on Arai, Agui, and Nakajima's algorithm for
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58 * scaled DCT. Their original paper (Trans. IEICE E-71(11):1095) is in
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59 * Japanese, but the algorithm is described in the Pennebaker & Mitchell
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60 * JPEG textbook (see REFERENCES section in file README). The following code
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61 * is based directly on figure 4-8 in P&M.
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62 * While an 8-point DCT cannot be done in less than 11 multiplies, it is
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63 * possible to arrange the computation so that many of the multiplies are
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64 * simple scalings of the final outputs. These multiplies can then be
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65 * folded into the multiplications or divisions by the JPEG quantization
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66 * table entries. The AA&N method leaves only 5 multiplies and 29 adds
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67 * to be done in the DCT itself.
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68 * The primary disadvantage of this method is that with a fixed-point
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69 * implementation, accuracy is lost due to imprecise representation of the
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70 * scaled quantization values. However, that problem does not arise if
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71 * we use floating point arithmetic.
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72 */
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73
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74 #include <stdint.h>
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75 #include "tinyjpeg-internal.h"
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76
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77 #define FAST_FLOAT float
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78 #define DCTSIZE 8
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79 #define DCTSIZE2 (DCTSIZE*DCTSIZE)
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80
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81 #define DEQUANTIZE(coef,quantval) (((FAST_FLOAT) (coef)) * (quantval))
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82
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83 static inline unsigned char descale_and_clamp(int x, int shift)
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84 {
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85 x += (1UL<<(shift-1));
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86 if (x<0)
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87 x = (x >> shift) | ((~(0UL)) << (32-(shift)));
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88 else
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89 x >>= shift;
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90 x += 128;
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91 if (x>255)
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92 return 255;
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93 else if (x<0)
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94 return 0;
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95 else
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96 return x;
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97 }
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98
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99 /*
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100 * Perform dequantization and inverse DCT on one block of coefficients.
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101 */
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102 void tinyjpeg_idct_float (struct component *compptr, uint8_t *output_buf, int stride)
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103 {
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104 FAST_FLOAT tmp0, tmp1, tmp2, tmp3, tmp4, tmp5, tmp6, tmp7;
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105 FAST_FLOAT tmp10, tmp11, tmp12, tmp13;
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106 FAST_FLOAT z5, z10, z11, z12, z13;
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107 int16_t *inptr;
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108 FAST_FLOAT *quantptr;
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109 FAST_FLOAT *wsptr;
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110 uint8_t *outptr;
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111 int ctr;
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112 FAST_FLOAT workspace[DCTSIZE2]; /* buffers data between passes */
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113
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114 /* Pass 1: process columns from input, store into work array. */
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115
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116 inptr = compptr->DCT;
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117 quantptr = compptr->Q_table;
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118 wsptr = workspace;
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119 for (ctr = DCTSIZE; ctr > 0; ctr--) {
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120 /* Due to quantization, we will usually find that many of the input
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121 * coefficients are zero, especially the AC terms. We can exploit this
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122 * by short-circuiting the IDCT calculation for any column in which all
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123 * the AC terms are zero. In that case each output is equal to the
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124 * DC coefficient (with scale factor as needed).
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125 * With typical images and quantization tables, half or more of the
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126 * column DCT calculations can be simplified this way.
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127 */
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128
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129 if (inptr[DCTSIZE*1] == 0 && inptr[DCTSIZE*2] == 0 &&
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130 inptr[DCTSIZE*3] == 0 && inptr[DCTSIZE*4] == 0 &&
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131 inptr[DCTSIZE*5] == 0 && inptr[DCTSIZE*6] == 0 &&
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132 inptr[DCTSIZE*7] == 0) {
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133 /* AC terms all zero */
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134 FAST_FLOAT dcval = DEQUANTIZE(inptr[DCTSIZE*0], quantptr[DCTSIZE*0]);
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135
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136 wsptr[DCTSIZE*0] = dcval;
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137 wsptr[DCTSIZE*1] = dcval;
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138 wsptr[DCTSIZE*2] = dcval;
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139 wsptr[DCTSIZE*3] = dcval;
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140 wsptr[DCTSIZE*4] = dcval;
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141 wsptr[DCTSIZE*5] = dcval;
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142 wsptr[DCTSIZE*6] = dcval;
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143 wsptr[DCTSIZE*7] = dcval;
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144
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145 inptr++; /* advance pointers to next column */
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146 quantptr++;
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147 wsptr++;
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148 continue;
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149 }
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150
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151 /* Even part */
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152
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153 tmp0 = DEQUANTIZE(inptr[DCTSIZE*0], quantptr[DCTSIZE*0]);
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154 tmp1 = DEQUANTIZE(inptr[DCTSIZE*2], quantptr[DCTSIZE*2]);
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155 tmp2 = DEQUANTIZE(inptr[DCTSIZE*4], quantptr[DCTSIZE*4]);
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156 tmp3 = DEQUANTIZE(inptr[DCTSIZE*6], quantptr[DCTSIZE*6]);
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157
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158 tmp10 = tmp0 + tmp2; /* phase 3 */
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159 tmp11 = tmp0 - tmp2;
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160
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161 tmp13 = tmp1 + tmp3; /* phases 5-3 */
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162 tmp12 = (tmp1 - tmp3) * ((FAST_FLOAT) 1.414213562) - tmp13; /* 2*c4 */
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163
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164 tmp0 = tmp10 + tmp13; /* phase 2 */
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165 tmp3 = tmp10 - tmp13;
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166 tmp1 = tmp11 + tmp12;
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167 tmp2 = tmp11 - tmp12;
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168
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169 /* Odd part */
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170
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171 tmp4 = DEQUANTIZE(inptr[DCTSIZE*1], quantptr[DCTSIZE*1]);
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172 tmp5 = DEQUANTIZE(inptr[DCTSIZE*3], quantptr[DCTSIZE*3]);
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173 tmp6 = DEQUANTIZE(inptr[DCTSIZE*5], quantptr[DCTSIZE*5]);
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174 tmp7 = DEQUANTIZE(inptr[DCTSIZE*7], quantptr[DCTSIZE*7]);
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175
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176 z13 = tmp6 + tmp5; /* phase 6 */
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177 z10 = tmp6 - tmp5;
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178 z11 = tmp4 + tmp7;
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179 z12 = tmp4 - tmp7;
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180
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181 tmp7 = z11 + z13; /* phase 5 */
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182 tmp11 = (z11 - z13) * ((FAST_FLOAT) 1.414213562); /* 2*c4 */
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183
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184 z5 = (z10 + z12) * ((FAST_FLOAT) 1.847759065); /* 2*c2 */
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185 tmp10 = ((FAST_FLOAT) 1.082392200) * z12 - z5; /* 2*(c2-c6) */
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186 tmp12 = ((FAST_FLOAT) -2.613125930) * z10 + z5; /* -2*(c2+c6) */
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187
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188 tmp6 = tmp12 - tmp7; /* phase 2 */
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189 tmp5 = tmp11 - tmp6;
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190 tmp4 = tmp10 + tmp5;
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191
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192 wsptr[DCTSIZE*0] = tmp0 + tmp7;
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193 wsptr[DCTSIZE*7] = tmp0 - tmp7;
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194 wsptr[DCTSIZE*1] = tmp1 + tmp6;
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195 wsptr[DCTSIZE*6] = tmp1 - tmp6;
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196 wsptr[DCTSIZE*2] = tmp2 + tmp5;
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197 wsptr[DCTSIZE*5] = tmp2 - tmp5;
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198 wsptr[DCTSIZE*4] = tmp3 + tmp4;
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199 wsptr[DCTSIZE*3] = tmp3 - tmp4;
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200
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201 inptr++; /* advance pointers to next column */
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202 quantptr++;
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203 wsptr++;
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204 }
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205
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206 /* Pass 2: process rows from work array, store into output array. */
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207 /* Note that we must descale the results by a factor of 8 == 2**3. */
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208
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209 wsptr = workspace;
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210 outptr = output_buf;
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211 for (ctr = 0; ctr < DCTSIZE; ctr++) {
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212 /* Rows of zeroes can be exploited in the same way as we did with columns.
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213 * However, the column calculation has created many nonzero AC terms, so
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214 * the simplification applies less often (typically 5% to 10% of the time).
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215 * And testing floats for zero is relatively expensive, so we don't bother.
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216 */
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217
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218 /* Even part */
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219
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220 tmp10 = wsptr[0] + wsptr[4];
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221 tmp11 = wsptr[0] - wsptr[4];
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222
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223 tmp13 = wsptr[2] + wsptr[6];
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224 tmp12 = (wsptr[2] - wsptr[6]) * ((FAST_FLOAT) 1.414213562) - tmp13;
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225
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226 tmp0 = tmp10 + tmp13;
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227 tmp3 = tmp10 - tmp13;
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228 tmp1 = tmp11 + tmp12;
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229 tmp2 = tmp11 - tmp12;
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230
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231 /* Odd part */
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232
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233 z13 = wsptr[5] + wsptr[3];
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234 z10 = wsptr[5] - wsptr[3];
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235 z11 = wsptr[1] + wsptr[7];
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236 z12 = wsptr[1] - wsptr[7];
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237
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238 tmp7 = z11 + z13;
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239 tmp11 = (z11 - z13) * ((FAST_FLOAT) 1.414213562);
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240
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241 z5 = (z10 + z12) * ((FAST_FLOAT) 1.847759065); /* 2*c2 */
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242 tmp10 = ((FAST_FLOAT) 1.082392200) * z12 - z5; /* 2*(c2-c6) */
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243 tmp12 = ((FAST_FLOAT) -2.613125930) * z10 + z5; /* -2*(c2+c6) */
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244
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245 tmp6 = tmp12 - tmp7;
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246 tmp5 = tmp11 - tmp6;
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247 tmp4 = tmp10 + tmp5;
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248
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249 /* Final output stage: scale down by a factor of 8 and range-limit */
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250
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251 outptr[0] = descale_and_clamp((int)(tmp0 + tmp7), 3);
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252 outptr[7] = descale_and_clamp((int)(tmp0 - tmp7), 3);
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253 outptr[1] = descale_and_clamp((int)(tmp1 + tmp6), 3);
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254 outptr[6] = descale_and_clamp((int)(tmp1 - tmp6), 3);
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255 outptr[2] = descale_and_clamp((int)(tmp2 + tmp5), 3);
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256 outptr[5] = descale_and_clamp((int)(tmp2 - tmp5), 3);
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257 outptr[4] = descale_and_clamp((int)(tmp3 + tmp4), 3);
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258 outptr[3] = descale_and_clamp((int)(tmp3 - tmp4), 3);
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259
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260
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261 wsptr += DCTSIZE; /* advance pointer to next row */
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262 outptr += stride;
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263 }
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264 }
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265
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