diff options
Diffstat (limited to 'plugins/FreeImage/Source/LibJPEG/jidctfst.c')
| -rw-r--r-- | plugins/FreeImage/Source/LibJPEG/jidctfst.c | 368 | 
1 files changed, 368 insertions, 0 deletions
diff --git a/plugins/FreeImage/Source/LibJPEG/jidctfst.c b/plugins/FreeImage/Source/LibJPEG/jidctfst.c new file mode 100644 index 0000000000..078b8c444e --- /dev/null +++ b/plugins/FreeImage/Source/LibJPEG/jidctfst.c @@ -0,0 +1,368 @@ +/*
 + * jidctfst.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 fast, not so accurate integer implementation of the
 + * inverse DCT (Discrete Cosine Transform).  In the IJG code, this routine
 + * must also perform dequantization of the input coefficients.
 + *
 + * 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 fixed-point math,
 + * accuracy is lost due to imprecise representation of the scaled
 + * quantization values.  The smaller the quantization table entry, the less
 + * precise the scaled value, so this implementation does worse with high-
 + * quality-setting files than with low-quality ones.
 + */
 +
 +#define JPEG_INTERNALS
 +#include "jinclude.h"
 +#include "jpeglib.h"
 +#include "jdct.h"		/* Private declarations for DCT subsystem */
 +
 +#ifdef DCT_IFAST_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
 +
 +
 +/* Scaling decisions are generally the same as in the LL&M algorithm;
 + * see jidctint.c for more details.  However, we choose to descale
 + * (right shift) multiplication products as soon as they are formed,
 + * rather than carrying additional fractional bits into subsequent additions.
 + * This compromises accuracy slightly, but it lets us save a few shifts.
 + * More importantly, 16-bit arithmetic is then adequate (for 8-bit samples)
 + * everywhere except in the multiplications proper; this saves a good deal
 + * of work on 16-bit-int machines.
 + *
 + * The dequantized coefficients are not integers because the AA&N scaling
 + * factors have been incorporated.  We represent them scaled up by PASS1_BITS,
 + * so that the first and second IDCT rounds have the same input scaling.
 + * For 8-bit JSAMPLEs, we choose IFAST_SCALE_BITS = PASS1_BITS so as to
 + * avoid a descaling shift; this compromises accuracy rather drastically
 + * for small quantization table entries, but it saves a lot of shifts.
 + * For 12-bit JSAMPLEs, there's no hope of using 16x16 multiplies anyway,
 + * so we use a much larger scaling factor to preserve accuracy.
 + *
 + * A final compromise is to represent the multiplicative constants to only
 + * 8 fractional bits, rather than 13.  This saves some shifting work on some
 + * machines, and may also reduce the cost of multiplication (since there
 + * are fewer one-bits in the constants).
 + */
 +
 +#if BITS_IN_JSAMPLE == 8
 +#define CONST_BITS  8
 +#define PASS1_BITS  2
 +#else
 +#define CONST_BITS  8
 +#define PASS1_BITS  1		/* lose a little precision to avoid overflow */
 +#endif
 +
 +/* Some C compilers fail to reduce "FIX(constant)" at compile time, thus
 + * causing a lot of useless floating-point operations at run time.
 + * To get around this we use the following pre-calculated constants.
 + * If you change CONST_BITS you may want to add appropriate values.
 + * (With a reasonable C compiler, you can just rely on the FIX() macro...)
 + */
 +
 +#if CONST_BITS == 8
 +#define FIX_1_082392200  ((INT32)  277)		/* FIX(1.082392200) */
 +#define FIX_1_414213562  ((INT32)  362)		/* FIX(1.414213562) */
 +#define FIX_1_847759065  ((INT32)  473)		/* FIX(1.847759065) */
 +#define FIX_2_613125930  ((INT32)  669)		/* FIX(2.613125930) */
 +#else
 +#define FIX_1_082392200  FIX(1.082392200)
 +#define FIX_1_414213562  FIX(1.414213562)
 +#define FIX_1_847759065  FIX(1.847759065)
 +#define FIX_2_613125930  FIX(2.613125930)
 +#endif
 +
 +
 +/* We can gain a little more speed, with a further compromise in accuracy,
 + * by omitting the addition in a descaling shift.  This yields an incorrectly
 + * rounded result half the time...
 + */
 +
 +#ifndef USE_ACCURATE_ROUNDING
 +#undef DESCALE
 +#define DESCALE(x,n)  RIGHT_SHIFT(x, n)
 +#endif
 +
 +
 +/* Multiply a DCTELEM variable by an INT32 constant, and immediately
 + * descale to yield a DCTELEM result.
 + */
 +
 +#define MULTIPLY(var,const)  ((DCTELEM) DESCALE((var) * (const), CONST_BITS))
 +
 +
 +/* Dequantize a coefficient by multiplying it by the multiplier-table
 + * entry; produce a DCTELEM result.  For 8-bit data a 16x16->16
 + * multiplication will do.  For 12-bit data, the multiplier table is
 + * declared INT32, so a 32-bit multiply will be used.
 + */
 +
 +#if BITS_IN_JSAMPLE == 8
 +#define DEQUANTIZE(coef,quantval)  (((IFAST_MULT_TYPE) (coef)) * (quantval))
 +#else
 +#define DEQUANTIZE(coef,quantval)  \
 +	DESCALE((coef)*(quantval), IFAST_SCALE_BITS-PASS1_BITS)
 +#endif
 +
 +
 +/* Like DESCALE, but applies to a DCTELEM and produces an int.
 + * We assume that int right shift is unsigned if INT32 right shift is.
 + */
 +
 +#ifdef RIGHT_SHIFT_IS_UNSIGNED
 +#define ISHIFT_TEMPS	DCTELEM ishift_temp;
 +#if BITS_IN_JSAMPLE == 8
 +#define DCTELEMBITS  16		/* DCTELEM may be 16 or 32 bits */
 +#else
 +#define DCTELEMBITS  32		/* DCTELEM must be 32 bits */
 +#endif
 +#define IRIGHT_SHIFT(x,shft)  \
 +    ((ishift_temp = (x)) < 0 ? \
 +     (ishift_temp >> (shft)) | ((~((DCTELEM) 0)) << (DCTELEMBITS-(shft))) : \
 +     (ishift_temp >> (shft)))
 +#else
 +#define ISHIFT_TEMPS
 +#define IRIGHT_SHIFT(x,shft)	((x) >> (shft))
 +#endif
 +
 +#ifdef USE_ACCURATE_ROUNDING
 +#define IDESCALE(x,n)  ((int) IRIGHT_SHIFT((x) + (1 << ((n)-1)), n))
 +#else
 +#define IDESCALE(x,n)  ((int) IRIGHT_SHIFT(x, n))
 +#endif
 +
 +
 +/*
 + * Perform dequantization and inverse DCT on one block of coefficients.
 + */
 +
 +GLOBAL(void)
 +jpeg_idct_ifast (j_decompress_ptr cinfo, jpeg_component_info * compptr,
 +		 JCOEFPTR coef_block,
 +		 JSAMPARRAY output_buf, JDIMENSION output_col)
 +{
 +  DCTELEM tmp0, tmp1, tmp2, tmp3, tmp4, tmp5, tmp6, tmp7;
 +  DCTELEM tmp10, tmp11, tmp12, tmp13;
 +  DCTELEM z5, z10, z11, z12, z13;
 +  JCOEFPTR inptr;
 +  IFAST_MULT_TYPE * quantptr;
 +  int * wsptr;
 +  JSAMPROW outptr;
 +  JSAMPLE *range_limit = IDCT_range_limit(cinfo);
 +  int ctr;
 +  int workspace[DCTSIZE2];	/* buffers data between passes */
 +  SHIFT_TEMPS			/* for DESCALE */
 +  ISHIFT_TEMPS			/* for IDESCALE */
 +
 +  /* Pass 1: process columns from input, store into work array. */
 +
 +  inptr = coef_block;
 +  quantptr = (IFAST_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 */
 +      int dcval = (int) 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 = MULTIPLY(tmp1 - tmp3, FIX_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 = MULTIPLY(z11 - z13, FIX_1_414213562); /* 2*c4 */
 +
 +    z5 = MULTIPLY(z10 + z12, FIX_1_847759065); /* 2*c2 */
 +    tmp10 = MULTIPLY(z12, FIX_1_082392200) - z5; /* 2*(c2-c6) */
 +    tmp12 = MULTIPLY(z10, - FIX_2_613125930) + z5; /* -2*(c2+c6) */
 +
 +    tmp6 = tmp12 - tmp7;	/* phase 2 */
 +    tmp5 = tmp11 - tmp6;
 +    tmp4 = tmp10 + tmp5;
 +
 +    wsptr[DCTSIZE*0] = (int) (tmp0 + tmp7);
 +    wsptr[DCTSIZE*7] = (int) (tmp0 - tmp7);
 +    wsptr[DCTSIZE*1] = (int) (tmp1 + tmp6);
 +    wsptr[DCTSIZE*6] = (int) (tmp1 - tmp6);
 +    wsptr[DCTSIZE*2] = (int) (tmp2 + tmp5);
 +    wsptr[DCTSIZE*5] = (int) (tmp2 - tmp5);
 +    wsptr[DCTSIZE*4] = (int) (tmp3 + tmp4);
 +    wsptr[DCTSIZE*3] = (int) (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, */
 +  /* and also undo the PASS1_BITS scaling. */
 +
 +  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).
 +     * On machines with very fast multiplication, it's possible that the
 +     * test takes more time than it's worth.  In that case this section
 +     * may be commented out.
 +     */
 +    
 +#ifndef NO_ZERO_ROW_TEST
 +    if (wsptr[1] == 0 && wsptr[2] == 0 && wsptr[3] == 0 && wsptr[4] == 0 &&
 +	wsptr[5] == 0 && wsptr[6] == 0 && wsptr[7] == 0) {
 +      /* AC terms all zero */
 +      JSAMPLE dcval = range_limit[IDESCALE(wsptr[0], PASS1_BITS+3)
 +				  & RANGE_MASK];
 +      
 +      outptr[0] = dcval;
 +      outptr[1] = dcval;
 +      outptr[2] = dcval;
 +      outptr[3] = dcval;
 +      outptr[4] = dcval;
 +      outptr[5] = dcval;
 +      outptr[6] = dcval;
 +      outptr[7] = dcval;
 +
 +      wsptr += DCTSIZE;		/* advance pointer to next row */
 +      continue;
 +    }
 +#endif
 +    
 +    /* Even part */
 +
 +    tmp10 = ((DCTELEM) wsptr[0] + (DCTELEM) wsptr[4]);
 +    tmp11 = ((DCTELEM) wsptr[0] - (DCTELEM) wsptr[4]);
 +
 +    tmp13 = ((DCTELEM) wsptr[2] + (DCTELEM) wsptr[6]);
 +    tmp12 = MULTIPLY((DCTELEM) wsptr[2] - (DCTELEM) wsptr[6], FIX_1_414213562)
 +	    - tmp13;
 +
 +    tmp0 = tmp10 + tmp13;
 +    tmp3 = tmp10 - tmp13;
 +    tmp1 = tmp11 + tmp12;
 +    tmp2 = tmp11 - tmp12;
 +
 +    /* Odd part */
 +
 +    z13 = (DCTELEM) wsptr[5] + (DCTELEM) wsptr[3];
 +    z10 = (DCTELEM) wsptr[5] - (DCTELEM) wsptr[3];
 +    z11 = (DCTELEM) wsptr[1] + (DCTELEM) wsptr[7];
 +    z12 = (DCTELEM) wsptr[1] - (DCTELEM) wsptr[7];
 +
 +    tmp7 = z11 + z13;		/* phase 5 */
 +    tmp11 = MULTIPLY(z11 - z13, FIX_1_414213562); /* 2*c4 */
 +
 +    z5 = MULTIPLY(z10 + z12, FIX_1_847759065); /* 2*c2 */
 +    tmp10 = MULTIPLY(z12, FIX_1_082392200) - z5; /* 2*(c2-c6) */
 +    tmp12 = MULTIPLY(z10, - FIX_2_613125930) + z5; /* -2*(c2+c6) */
 +
 +    tmp6 = tmp12 - tmp7;	/* phase 2 */
 +    tmp5 = tmp11 - tmp6;
 +    tmp4 = tmp10 + tmp5;
 +
 +    /* Final output stage: scale down by a factor of 8 and range-limit */
 +
 +    outptr[0] = range_limit[IDESCALE(tmp0 + tmp7, PASS1_BITS+3)
 +			    & RANGE_MASK];
 +    outptr[7] = range_limit[IDESCALE(tmp0 - tmp7, PASS1_BITS+3)
 +			    & RANGE_MASK];
 +    outptr[1] = range_limit[IDESCALE(tmp1 + tmp6, PASS1_BITS+3)
 +			    & RANGE_MASK];
 +    outptr[6] = range_limit[IDESCALE(tmp1 - tmp6, PASS1_BITS+3)
 +			    & RANGE_MASK];
 +    outptr[2] = range_limit[IDESCALE(tmp2 + tmp5, PASS1_BITS+3)
 +			    & RANGE_MASK];
 +    outptr[5] = range_limit[IDESCALE(tmp2 - tmp5, PASS1_BITS+3)
 +			    & RANGE_MASK];
 +    outptr[4] = range_limit[IDESCALE(tmp3 + tmp4, PASS1_BITS+3)
 +			    & RANGE_MASK];
 +    outptr[3] = range_limit[IDESCALE(tmp3 - tmp4, PASS1_BITS+3)
 +			    & RANGE_MASK];
 +
 +    wsptr += DCTSIZE;		/* advance pointer to next row */
 +  }
 +}
 +
 +#endif /* DCT_IFAST_SUPPORTED */
  | 
