| /* | |
| * 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 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 = 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 */ |