CentrED/Imaging/JpegLib/imjidctfst.pas

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unit imjidctfst;
{ 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. }
{ Original : jidctfst.c ; Copyright (C) 1994-1996, Thomas G. Lane. }
interface
{$I imjconfig.inc}
uses
imjmorecfg,
imjinclude,
imjpeglib,
imjdct; { Private declarations for DCT subsystem }
{ Perform dequantization and inverse DCT on one block of coefficients. }
{GLOBAL}
procedure jpeg_idct_ifast (cinfo : j_decompress_ptr;
compptr : jpeg_component_info_ptr;
coef_block : JCOEFPTR;
output_buf : JSAMPARRAY;
output_col : JDIMENSION);
implementation
{ This module is specialized to the case DCTSIZE = 8. }
{$ifndef DCTSIZE_IS_8}
Sorry, this code only copes with 8x8 DCTs. { deliberate syntax err }
{$endif}
{ Scaling decisions are generally the same as in the LL&M algorithm;
see jidctint.c for more details. However, we choose to descale
(right shift) multiplication products as soon as they are formed,
rather than carrying additional fractional bits into subsequent additions.
This compromises accuracy slightly, but it lets us save a few shifts.
More importantly, 16-bit arithmetic is then adequate (for 8-bit samples)
everywhere except in the multiplications proper; this saves a good deal
of work on 16-bit-int machines.
The dequantized coefficients are not integers because the AA&N scaling
factors have been incorporated. We represent them scaled up by PASS1_BITS,
so that the first and second IDCT rounds have the same input scaling.
For 8-bit JSAMPLEs, we choose IFAST_SCALE_BITS = PASS1_BITS so as to
avoid a descaling shift; this compromises accuracy rather drastically
for small quantization table entries, but it saves a lot of shifts.
For 12-bit JSAMPLEs, there's no hope of using 16x16 multiplies anyway,
so we use a much larger scaling factor to preserve accuracy.
A final compromise is to represent the multiplicative constants to only
8 fractional bits, rather than 13. This saves some shifting work on some
machines, and may also reduce the cost of multiplication (since there
are fewer one-bits in the constants). }
{$ifdef BITS_IN_JSAMPLE_IS_8}
const
CONST_BITS = 8;
PASS1_BITS = 2;
{$else}
const
CONST_BITS = 8;
PASS1_BITS = 1; { lose a little precision to avoid overflow }
{$endif}
const
FIX_1_082392200 = INT32(Round((INT32(1) shl CONST_BITS)*1.082392200)); {277}
FIX_1_414213562 = INT32(Round((INT32(1) shl CONST_BITS)*1.414213562)); {362}
FIX_1_847759065 = INT32(Round((INT32(1) shl CONST_BITS)*1.847759065)); {473}
FIX_2_613125930 = INT32(Round((INT32(1) shl CONST_BITS)*2.613125930)); {669}
{ Descale and correctly round an INT32 value that's scaled by N bits.
We assume RIGHT_SHIFT rounds towards minus infinity, so adding
the fudge factor is correct for either sign of X. }
function DESCALE(x : INT32; n : int) : INT32;
var
shift_temp : INT32;
begin
{$ifdef USE_ACCURATE_ROUNDING}
shift_temp := x + (INT32(1) shl (n-1));
{$else}
{ 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... }
shift_temp := x;
{$endif}
{$ifdef RIGHT_SHIFT_IS_UNSIGNED}
if shift_temp < 0 then
Descale := (shift_temp shr n) or ((not INT32(0)) shl (32-n))
else
{$endif}
Descale := (shift_temp shr n);
end;
{ Multiply a DCTELEM variable by an INT32 constant, and immediately
descale to yield a DCTELEM result. }
{(DCTELEM( DESCALE((var) * (const), CONST_BITS))}
function Multiply(Avar, Aconst: Integer): DCTELEM;
begin
Multiply := DCTELEM( Avar*INT32(Aconst) div (INT32(1) shl CONST_BITS));
end;
{ Dequantize a coefficient by multiplying it by the multiplier-table
entry; produce a DCTELEM result. For 8-bit data a 16x16->16
multiplication will do. For 12-bit data, the multiplier table is
declared INT32, so a 32-bit multiply will be used. }
{$ifdef BITS_IN_JSAMPLE_IS_8}
function DEQUANTIZE(coef,quantval : int) : int;
begin
Dequantize := ( IFAST_MULT_TYPE(coef) * quantval);
end;
{$else}
function DEQUANTIZE(coef,quantval : INT32) : int;
begin
Dequantize := DESCALE((coef)*(quantval), IFAST_SCALE_BITS-PASS1_BITS);
end;
{$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. }
function IDESCALE(x : DCTELEM; n : int) : int;
{$ifdef BITS_IN_JSAMPLE_IS_8}
const
DCTELEMBITS = 16; { DCTELEM may be 16 or 32 bits }
{$else}
const
DCTELEMBITS = 32; { DCTELEM must be 32 bits }
{$endif}
var
ishift_temp : DCTELEM;
begin
{$ifndef USE_ACCURATE_ROUNDING}
ishift_temp := x + (INT32(1) shl (n-1));
{$else}
{ We can gain a little more speed, with a further compromise in accuracy,
by omitting the addition in a descaling shift. This yields an incorrectly
rounded result half the time... }
ishift_temp := x;
{$endif}
{$ifdef RIGHT_SHIFT_IS_UNSIGNED}
if ishift_temp < 0 then
IDescale := (ishift_temp shr n)
or ((not DCTELEM(0)) shl (DCTELEMBITS-n))
else
{$endif}
IDescale := (ishift_temp shr n);
end;
{ Perform dequantization and inverse DCT on one block of coefficients. }
{GLOBAL}
procedure jpeg_idct_ifast (cinfo : j_decompress_ptr;
compptr : jpeg_component_info_ptr;
coef_block : JCOEFPTR;
output_buf : JSAMPARRAY;
output_col : JDIMENSION);
type
PWorkspace = ^TWorkspace;
TWorkspace = coef_bits_field; { buffers data between passes }
var
tmp0, tmp1, tmp2, tmp3, tmp4, tmp5, tmp6, tmp7 : DCTELEM;
tmp10, tmp11, tmp12, tmp13 : DCTELEM;
z5, z10, z11, z12, z13 : DCTELEM;
inptr : JCOEFPTR;
quantptr : IFAST_MULT_TYPE_FIELD_PTR;
wsptr : PWorkspace;
outptr : JSAMPROW;
range_limit : JSAMPROW;
ctr : int;
workspace : TWorkspace; { buffers data between passes }
{SHIFT_TEMPS} { for DESCALE }
{ISHIFT_TEMPS} { for IDESCALE }
var
dcval : int;
var
dcval_ : JSAMPLE;
begin
{ Each IDCT routine is responsible for range-limiting its results and
converting them to unsigned form (0..MAXJSAMPLE). The raw outputs could
be quite far out of range if the input data is corrupt, so a bulletproof
range-limiting step is required. We use a mask-and-table-lookup method
to do the combined operations quickly. See the comments with
prepare_range_limit_table (in jdmaster.c) for more info. }
range_limit := JSAMPROW(@(cinfo^.sample_range_limit^[CENTERJSAMPLE]));
{ Pass 1: process columns from input, store into work array. }
inptr := coef_block;
quantptr := IFAST_MULT_TYPE_FIELD_PTR(compptr^.dct_table);
wsptr := @workspace;
for ctr := pred(DCTSIZE) downto 0 do
begin
{ 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) and (inptr^[DCTSIZE*2]=0) and (inptr^[DCTSIZE*3]=0) and
(inptr^[DCTSIZE*4]=0) and (inptr^[DCTSIZE*5]=0) and (inptr^[DCTSIZE*6]=0) and
(inptr^[DCTSIZE*7]=0) then
begin
{ AC terms all zero }
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;
Inc(JCOEF_PTR(inptr)); { advance pointers to next column }
Inc(IFAST_MULT_TYPE_PTR(quantptr));
Inc(int_ptr(wsptr));
continue;
end;
{ 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);
Inc(JCOEF_PTR(inptr)); { advance pointers to next column }
Inc(IFAST_MULT_TYPE_PTR(quantptr));
Inc(int_ptr(wsptr));
end;
{ 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 to pred(DCTSIZE) do
begin
outptr := JSAMPROW(@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. }
{$ifndef NO_ZERO_ROW_TEST}
if (wsptr^[1]=0) and (wsptr^[2]=0) and (wsptr^[3]=0) and (wsptr^[4]=0) and
(wsptr^[5]=0) and (wsptr^[6]=0) and (wsptr^[7]=0) then
begin
{ AC terms all zero }
dcval_ := range_limit^[IDESCALE(wsptr^[0], PASS1_BITS+3)
and RANGE_MASK];
outptr^[0] := dcval_;
outptr^[1] := dcval_;
outptr^[2] := dcval_;
outptr^[3] := dcval_;
outptr^[4] := dcval_;
outptr^[5] := dcval_;
outptr^[6] := dcval_;
outptr^[7] := dcval_;
Inc(int_ptr(wsptr), DCTSIZE); { advance pointer to next row }
continue;
end;
{$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)
and RANGE_MASK];
outptr^[7] := range_limit^[IDESCALE(tmp0 - tmp7, PASS1_BITS+3)
and RANGE_MASK];
outptr^[1] := range_limit^[IDESCALE(tmp1 + tmp6, PASS1_BITS+3)
and RANGE_MASK];
outptr^[6] := range_limit^[IDESCALE(tmp1 - tmp6, PASS1_BITS+3)
and RANGE_MASK];
outptr^[2] := range_limit^[IDESCALE(tmp2 + tmp5, PASS1_BITS+3)
and RANGE_MASK];
outptr^[5] := range_limit^[IDESCALE(tmp2 - tmp5, PASS1_BITS+3)
and RANGE_MASK];
outptr^[4] := range_limit^[IDESCALE(tmp3 + tmp4, PASS1_BITS+3)
and RANGE_MASK];
outptr^[3] := range_limit^[IDESCALE(tmp3 - tmp4, PASS1_BITS+3)
and RANGE_MASK];
Inc(int_ptr(wsptr), DCTSIZE); { advance pointer to next row }
end;
end;
end.