|  | /* | 
|  | * jidctflt.c | 
|  | * | 
|  | * This file was part of the Independent JPEG Group's software: | 
|  | * Copyright (C) 1994-1998, Thomas G. Lane. | 
|  | * Modified 2010 by Guido Vollbeding. | 
|  | * libjpeg-turbo Modifications: | 
|  | * Copyright (C) 2014, D. R. Commander. | 
|  | * For conditions of distribution and use, see the accompanying README.ijg | 
|  | * 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.ijg).  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 8x8 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 = cinfo->sample_range_limit; | 
|  | int ctr; | 
|  | FAST_FLOAT workspace[DCTSIZE2]; /* buffers data between passes */ | 
|  | #define _0_125  ((FLOAT_MULT_TYPE)0.125) | 
|  |  | 
|  | /* 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] * _0_125); | 
|  |  | 
|  | 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] * _0_125); | 
|  | tmp1 = DEQUANTIZE(inptr[DCTSIZE * 2], quantptr[DCTSIZE * 2] * _0_125); | 
|  | tmp2 = DEQUANTIZE(inptr[DCTSIZE * 4], quantptr[DCTSIZE * 4] * _0_125); | 
|  | tmp3 = DEQUANTIZE(inptr[DCTSIZE * 6], quantptr[DCTSIZE * 6] * _0_125); | 
|  |  | 
|  | 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] * _0_125); | 
|  | tmp5 = DEQUANTIZE(inptr[DCTSIZE * 3], quantptr[DCTSIZE * 3] * _0_125); | 
|  | tmp6 = DEQUANTIZE(inptr[DCTSIZE * 5], quantptr[DCTSIZE * 5] * _0_125); | 
|  | tmp7 = DEQUANTIZE(inptr[DCTSIZE * 7], quantptr[DCTSIZE * 7] * _0_125); | 
|  |  | 
|  | 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 = z5 - z12 * ((FAST_FLOAT)1.082392200); /* 2*(c2-c6) */ | 
|  | tmp12 = z5 - z10 * ((FAST_FLOAT)2.613125930); /* 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 * 3] = tmp3 + tmp4; | 
|  | wsptr[DCTSIZE * 4] = tmp3 - tmp4; | 
|  |  | 
|  | inptr++;                    /* advance pointers to next column */ | 
|  | quantptr++; | 
|  | wsptr++; | 
|  | } | 
|  |  | 
|  | /* Pass 2: process rows from work array, store into output array. */ | 
|  |  | 
|  | 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 */ | 
|  |  | 
|  | /* Apply signed->unsigned and prepare float->int conversion */ | 
|  | z5 = wsptr[0] + ((FAST_FLOAT)CENTERJSAMPLE + (FAST_FLOAT)0.5); | 
|  | tmp10 = z5 + wsptr[4]; | 
|  | tmp11 = z5 - 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 = z5 - z12 * ((FAST_FLOAT)1.082392200); /* 2*(c2-c6) */ | 
|  | tmp12 = z5 - z10 * ((FAST_FLOAT)2.613125930); /* 2*(c2+c6) */ | 
|  |  | 
|  | tmp6 = tmp12 - tmp7; | 
|  | tmp5 = tmp11 - tmp6; | 
|  | tmp4 = tmp10 - tmp5; | 
|  |  | 
|  | /* Final output stage: float->int conversion and range-limit */ | 
|  |  | 
|  | outptr[0] = range_limit[((int)(tmp0 + tmp7)) & RANGE_MASK]; | 
|  | outptr[7] = range_limit[((int)(tmp0 - tmp7)) & RANGE_MASK]; | 
|  | outptr[1] = range_limit[((int)(tmp1 + tmp6)) & RANGE_MASK]; | 
|  | outptr[6] = range_limit[((int)(tmp1 - tmp6)) & RANGE_MASK]; | 
|  | outptr[2] = range_limit[((int)(tmp2 + tmp5)) & RANGE_MASK]; | 
|  | outptr[5] = range_limit[((int)(tmp2 - tmp5)) & RANGE_MASK]; | 
|  | outptr[3] = range_limit[((int)(tmp3 + tmp4)) & RANGE_MASK]; | 
|  | outptr[4] = range_limit[((int)(tmp3 - tmp4)) & RANGE_MASK]; | 
|  |  | 
|  | wsptr += DCTSIZE;           /* advance pointer to next row */ | 
|  | } | 
|  | } | 
|  |  | 
|  | #endif /* DCT_FLOAT_SUPPORTED */ |