Quelle jidctflt.c
Sprache: C
/*
* reserved comment block
* DO NOT REMOVE OR ALTER !
*/
/*
* jidctflt . c
*
* Copyright ( C ) 1994 - 1998 , Thomas G . Lane .
* This file is part of the Independent JPEG Group ' s software .
* For conditions of distribution and use , see the accompanying README file .
*
* This file contains a floating - point implementation of the
* inverse DCT ( Discrete Cosine Transform ) . In the IJG code , this routine
* must also perform dequantization of the input coefficients .
*
* This implementation should be more accurate than either of the integer
* IDCT implementations . However , it may not give the same results on all
* machines because of differences in roundoff behavior . Speed will depend
* on the hardware ' s floating point capacity .
*
* A 2 - D IDCT can be done by 1 - D IDCT on each column followed by 1 - D IDCT
* on each row ( or vice versa , but it ' s more convenient to emit a row at
* a time ) . Direct algorithms are also available , but they are much more
* complex and seem not to be any faster when reduced to code .
*
* This implementation is based on Arai , Agui , and Nakajima ' s algorithm for
* scaled DCT . Their original paper ( Trans . IEICE E - 71 ( 11 ) : 1095 ) is in
* Japanese , but the algorithm is described in the Pennebaker & Mitchell
* JPEG textbook ( see REFERENCES section in file README ) . The following code
* is based directly on figure 4 - 8 in P & M .
* While an 8 - point DCT cannot be done in less than 11 multiplies , it is
* possible to arrange the computation so that many of the multiplies are
* simple scalings of the final outputs . These multiplies can then be
* folded into the multiplications or divisions by the JPEG quantization
* table entries . The AA & N method leaves only 5 multiplies and 29 adds
* to be done in the DCT itself .
* The primary disadvantage of this method is that with a fixed - point
* implementation , accuracy is lost due to imprecise representation of the
* scaled quantization values . However , that problem does not arise if
* we use floating point arithmetic .
*/
#define JPEG_INTERNALS
#include "jinclude.h"
#include "jpeglib.h"
#include "jdct.h" /* Private declarations for DCT subsystem */
#ifdef DCT_FLOAT_SUPPORTED
/*
* This module is specialized to the case DCTSIZE = 8 .
*/
#if DCTSIZE != 8
Sorry, this code only copes with 8 x8 DCTs. /* deliberate syntax err */
#endif
/* Dequantize a coefficient by multiplying it by the multiplier-table
* entry ; produce a float result .
*/
#define DEQUANTIZE(coef,quantval) (((FAST_FLOAT) (coef)) * (quantval))
/*
* Perform dequantization and inverse DCT on one block of coefficients .
*/
GLOBAL(void )
jpeg_idct_float (j_decompress_ptr cinfo, jpeg_component_info * compptr,
JCOEFPTR coef_block,
JSAMPARRAY output_buf, JDIMENSION output_col)
{
FAST_FLOAT tmp0, tmp1, tmp2, tmp3, tmp4, tmp5, tmp6, tmp7;
FAST_FLOAT tmp10, tmp11, tmp12, tmp13;
FAST_FLOAT z5, z10, z11, z12, z13;
JCOEFPTR inptr;
FLOAT_MULT_TYPE * quantptr;
FAST_FLOAT * wsptr;
JSAMPROW outptr;
JSAMPLE *range_limit = IDCT_range_limit(cinfo);
int ctr;
FAST_FLOAT workspace[DCTSIZE2]; /* buffers data between passes */
SHIFT_TEMPS
/* Pass 1: process columns from input, store into work array. */
inptr = coef_block;
quantptr = (FLOAT_MULT_TYPE *) compptr->dct_table;
wsptr = workspace;
for (ctr = DCTSIZE; ctr > 0 ; ctr--) {
/* Due to quantization, we will usually find that many of the input
* coefficients are zero , especially the AC terms . We can exploit this
* by short - circuiting the IDCT calculation for any column in which all
* the AC terms are zero . In that case each output is equal to the
* DC coefficient ( with scale factor as needed ) .
* With typical images and quantization tables , half or more of the
* column DCT calculations can be simplified this way .
*/
if (inptr[DCTSIZE*1 ] == 0 && inptr[DCTSIZE*2 ] == 0 &&
inptr[DCTSIZE*3 ] == 0 && inptr[DCTSIZE*4 ] == 0 &&
inptr[DCTSIZE*5 ] == 0 && inptr[DCTSIZE*6 ] == 0 &&
inptr[DCTSIZE*7 ] == 0 ) {
/* AC terms all zero */
FAST_FLOAT dcval = DEQUANTIZE(inptr[DCTSIZE*0 ], quantptr[DCTSIZE*0 ]);
wsptr[DCTSIZE*0 ] = dcval;
wsptr[DCTSIZE*1 ] = dcval;
wsptr[DCTSIZE*2 ] = dcval;
wsptr[DCTSIZE*3 ] = dcval;
wsptr[DCTSIZE*4 ] = dcval;
wsptr[DCTSIZE*5 ] = dcval;
wsptr[DCTSIZE*6 ] = dcval;
wsptr[DCTSIZE*7 ] = dcval;
inptr++; /* advance pointers to next column */
quantptr++;
wsptr++;
continue ;
}
/* Even part */
tmp0 = DEQUANTIZE(inptr[DCTSIZE*0 ], quantptr[DCTSIZE*0 ]);
tmp1 = DEQUANTIZE(inptr[DCTSIZE*2 ], quantptr[DCTSIZE*2 ]);
tmp2 = DEQUANTIZE(inptr[DCTSIZE*4 ], quantptr[DCTSIZE*4 ]);
tmp3 = DEQUANTIZE(inptr[DCTSIZE*6 ], quantptr[DCTSIZE*6 ]);
tmp10 = tmp0 + tmp2; /* phase 3 */
tmp11 = tmp0 - tmp2;
tmp13 = tmp1 + tmp3; /* phases 5-3 */
tmp12 = (tmp1 - tmp3) * ((FAST_FLOAT) 1 .414213562 ) - tmp13; /* 2*c4 */
tmp0 = tmp10 + tmp13; /* phase 2 */
tmp3 = tmp10 - tmp13;
tmp1 = tmp11 + tmp12;
tmp2 = tmp11 - tmp12;
/* Odd part */
tmp4 = DEQUANTIZE(inptr[DCTSIZE*1 ], quantptr[DCTSIZE*1 ]);
tmp5 = DEQUANTIZE(inptr[DCTSIZE*3 ], quantptr[DCTSIZE*3 ]);
tmp6 = DEQUANTIZE(inptr[DCTSIZE*5 ], quantptr[DCTSIZE*5 ]);
tmp7 = DEQUANTIZE(inptr[DCTSIZE*7 ], quantptr[DCTSIZE*7 ]);
z13 = tmp6 + tmp5; /* phase 6 */
z10 = tmp6 - tmp5;
z11 = tmp4 + tmp7;
z12 = tmp4 - tmp7;
tmp7 = z11 + z13; /* phase 5 */
tmp11 = (z11 - z13) * ((FAST_FLOAT) 1 .414213562 ); /* 2*c4 */
z5 = (z10 + z12) * ((FAST_FLOAT) 1 .847759065 ); /* 2*c2 */
tmp10 = ((FAST_FLOAT) 1 .082392200 ) * z12 - z5; /* 2*(c2-c6) */
tmp12 = ((FAST_FLOAT) -2 .613125930 ) * z10 + z5; /* -2*(c2+c6) */
tmp6 = tmp12 - tmp7; /* phase 2 */
tmp5 = tmp11 - tmp6;
tmp4 = tmp10 + tmp5;
wsptr[DCTSIZE*0 ] = tmp0 + tmp7;
wsptr[DCTSIZE*7 ] = tmp0 - tmp7;
wsptr[DCTSIZE*1 ] = tmp1 + tmp6;
wsptr[DCTSIZE*6 ] = tmp1 - tmp6;
wsptr[DCTSIZE*2 ] = tmp2 + tmp5;
wsptr[DCTSIZE*5 ] = tmp2 - tmp5;
wsptr[DCTSIZE*4 ] = tmp3 + tmp4;
wsptr[DCTSIZE*3 ] = tmp3 - tmp4;
inptr++; /* advance pointers to next column */
quantptr++;
wsptr++;
}
/* Pass 2: process rows from work array, store into output array. */
/* Note that we must descale the results by a factor of 8 == 2**3. */
wsptr = workspace;
for (ctr = 0 ; ctr < DCTSIZE; ctr++) {
outptr = output_buf[ctr] + output_col;
/* Rows of zeroes can be exploited in the same way as we did with columns.
* However , the column calculation has created many nonzero AC terms , so
* the simplification applies less often ( typically 5 % to 10 % of the time ) .
* And testing floats for zero is relatively expensive , so we don ' t bother .
*/
/* Even part */
tmp10 = wsptr[0 ] + wsptr[4 ];
tmp11 = wsptr[0 ] - wsptr[4 ];
tmp13 = wsptr[2 ] + wsptr[6 ];
tmp12 = (wsptr[2 ] - wsptr[6 ]) * ((FAST_FLOAT) 1 .414213562 ) - tmp13;
tmp0 = tmp10 + tmp13;
tmp3 = tmp10 - tmp13;
tmp1 = tmp11 + tmp12;
tmp2 = tmp11 - tmp12;
/* Odd part */
z13 = wsptr[5 ] + wsptr[3 ];
z10 = wsptr[5 ] - wsptr[3 ];
z11 = wsptr[1 ] + wsptr[7 ];
z12 = wsptr[1 ] - wsptr[7 ];
tmp7 = z11 + z13;
tmp11 = (z11 - z13) * ((FAST_FLOAT) 1 .414213562 );
z5 = (z10 + z12) * ((FAST_FLOAT) 1 .847759065 ); /* 2*c2 */
tmp10 = ((FAST_FLOAT) 1 .082392200 ) * z12 - z5; /* 2*(c2-c6) */
tmp12 = ((FAST_FLOAT) -2 .613125930 ) * z10 + z5; /* -2*(c2+c6) */
tmp6 = tmp12 - tmp7;
tmp5 = tmp11 - tmp6;
tmp4 = tmp10 + tmp5;
/* Final output stage: scale down by a factor of 8 and range-limit */
outptr[0 ] = range_limit[(int) DESCALE((INT32) (tmp0 + tmp7), 3 )
& RANGE_MASK];
outptr[7 ] = range_limit[(int) DESCALE((INT32) (tmp0 - tmp7), 3 )
& RANGE_MASK];
outptr[1 ] = range_limit[(int) DESCALE((INT32) (tmp1 + tmp6), 3 )
& RANGE_MASK];
outptr[6 ] = range_limit[(int) DESCALE((INT32) (tmp1 - tmp6), 3 )
& RANGE_MASK];
outptr[2 ] = range_limit[(int) DESCALE((INT32) (tmp2 + tmp5), 3 )
& RANGE_MASK];
outptr[5 ] = range_limit[(int) DESCALE((INT32) (tmp2 - tmp5), 3 )
& RANGE_MASK];
outptr[4 ] = range_limit[(int) DESCALE((INT32) (tmp3 + tmp4), 3 )
& RANGE_MASK];
outptr[3 ] = range_limit[(int) DESCALE((INT32) (tmp3 - tmp4), 3 )
& RANGE_MASK];
wsptr += DCTSIZE; /* advance pointer to next row */
}
}
#endif /* DCT_FLOAT_SUPPORTED */
Messung V0.5 in Prozent C=86 H=100 G=93
¤ Dauer der Verarbeitung: 0.9 Sekunden
(vorverarbeitet am 2026-09-02)
¤
*© Formatika GbR, Deutschland
2026-08-25
Neuigkeiten
Aktuelles
Motto des Tages
Open Source Software
Jenseits des Üblichen ....
Besucherstatistik
Statistik
#Sources=1019547
#Domains=890699