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author | Matthias P. Braendli <matthias.braendli@mpb.li> | 2016-02-15 02:44:20 +0100 |
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committer | Matthias P. Braendli <matthias.braendli@mpb.li> | 2016-02-15 02:44:20 +0100 |
commit | 22f1fce330059ef8a383cf327a023d6a9da5ad3e (patch) | |
tree | 6893f158dcaaaa1b9f1317923c32a841ba31f768 /libtoolame-dab/psycho_4.c | |
parent | 891bb2592944aa2be2d81e1583e73e632e70537f (diff) | |
download | fdk-aac-22f1fce330059ef8a383cf327a023d6a9da5ad3e.tar.gz fdk-aac-22f1fce330059ef8a383cf327a023d6a9da5ad3e.tar.bz2 fdk-aac-22f1fce330059ef8a383cf327a023d6a9da5ad3e.zip |
Include toolame-dab as library
Diffstat (limited to 'libtoolame-dab/psycho_4.c')
-rw-r--r-- | libtoolame-dab/psycho_4.c | 507 |
1 files changed, 507 insertions, 0 deletions
diff --git a/libtoolame-dab/psycho_4.c b/libtoolame-dab/psycho_4.c new file mode 100644 index 0000000..b2abc76 --- /dev/null +++ b/libtoolame-dab/psycho_4.c @@ -0,0 +1,507 @@ +#include <stdio.h> +#include <stdlib.h> +#include <math.h> +#include <string.h> +#include "common.h" +#include "options.h" +#include "encoder.h" +#include "mem.h" +#include "fft.h" +#include "ath.h" +#include "psycho_4.h" + +/**************************************************************** +PSYCHO_4 by MFC Feb 2003 + +This is a cleaned up implementation of psy model 2. +This is basically because I was sick of the inconsistencies between +the notation in the ISO docs and in the sourcecode. + +I've nicked a bunch of stuff from LAME to make this a bit easier to grok +- ATH values (this also overcomes the lack of mpeg-2 tables + which meant that LSF never had proper values) +- freq2bark() to convert frequencies directly to bark values. +- spreading_function() isolated the calculation of the spreading function. + Basically the same code as before, just isolated in its own function. + LAME seem to does some extra tweaks to the ISO1117s model. + Not really sure if they help or hinder, so I've commented them out (#ifdef LAME) + +NB: Because of some of the tweaks to bark value calculation etc, it is now possible +to have 64 CBANDS. There's no real limit on the actual number of paritions. +I wonder if it's worth experimenting with really higher numbers? Probably won't make +that much difference to the final SNR values, but it's something worth trying + Maybe CBANDS should be a dynamic value, calculated by the psycho_init function + CBANDS definition has been changed in encoder.h from 63 to 64 + +****************************************************************/ + + +/* The static variables "r", "phi_sav", "new", "old" and "oldest" have + to be remembered for the unpredictability measure. For "r" and + "phi_sav", the first index from the left is the channel select and + the second index is the "age" of the data. */ + +static int new = 0, old = 1, oldest = 0; +static int init = 0; + +/* NMT is a constant 5.5dB. ISO11172 Sec D.2.4.h */ +static double NMT = 5.5; + +/* The index into this array is a bark value + This array gives the 'minval' values from ISO11172 Tables D.3.x */ +static FLOAT minval[27] = { + 0.0, /* bark = 0 */ + 20.0, /* 1 */ + 20.0, /* 2 */ + 20.0, /* 3 */ + 20.0, /* 4 */ + 20.0, /* 5 */ + 17.0, /* 6 */ + 15.0, /* 7 */ + 10.0, /* 8 */ + 7.0, /* 9 */ + 4.4, /* 10 */ + 4.5, 4.5, 4.5,4.5, 4.5, 4.5, 4.5, 4.5, 4.5, 4.5, 4.5, 4.5, 4.5, 4.5, 4.5, /* 11 - 25 */ + 3.5 /* 26 */ +}; + + +static FLOAT *grouped_c, *grouped_e, *nb, *cb, *tb, *ecb, *bc; +static FLOAT *wsamp_r, *phi, *energy; +static FLOAT *c, *bark, *thr; +static F32 *snrtmp; + +static int *numlines; +static int *partition; +static FLOAT *cbval, *rnorm; +static FLOAT *window; +static FLOAT *ath; +static double *tmn; +static FCB *s; +static FHBLK *lthr; +static F2HBLK *r, *phi_sav; + +#define TRIGTABLESIZE 3142 +#define TRIGTABLESCALE 1000.0 +static FLOAT cos_table[TRIGTABLESIZE]; +static FLOAT sin_table[TRIGTABLESIZE]; +void psycho_4_trigtable_init(void) { + + int i; + for (i=0;i<TRIGTABLESIZE;i++) { + cos_table[i] = cos((double)i/TRIGTABLESCALE); + sin_table[i] = sin((double)i/TRIGTABLESCALE); + } +} + +FLOAT psycho_4_cos(FLOAT phi) { + int index; + int sign=1; + + index = (int)(fabs(phi) * TRIGTABLESCALE); + while (index>=TRIGTABLESIZE) { + index -= TRIGTABLESIZE; + sign*=-1; + } + return(sign * cos_table[index]); +} + +FLOAT psycho_4_sin(FLOAT phi) { + int index; + int sign=1; + + index = (int)(fabs(phi) * TRIGTABLESCALE); + while (index>=TRIGTABLESIZE) { + index -= TRIGTABLESIZE; + sign*=-1; + } + if (phi<0) + return(-1 * sign * sin_table[index]); + return(sign * sin_table[index]); +} + + +void psycho_4 (short int *buffer, short int savebuf[1056], int chn, + double *smr, double sfreq, options *glopts) +/* to match prototype : FLOAT args are always double */ +{ + unsigned int run, i, j, k; + FLOAT r_prime, phi_prime; + FLOAT npart, epart; + + if (init == 0) { + psycho_4_init (sfreq, glopts); + init++; + } + + for (run = 0; run < 2; run++) { + /* Net offset is 480 samples (1056-576) for layer 2; this is because one must + stagger input data by 256 samples to synchronize psychoacoustic model with + filter bank outputs, then stagger so that center of 1024 FFT window lines + up with center of 576 "new" audio samples. + + flush = 384*3.0/2.0; = 576 + syncsize = 1056; + sync_flush = syncsize - flush; 480 + BLKSIZE = 1024 */ + for (j = 0; j < 480; j++) { + savebuf[j] = savebuf[j + 576]; + wsamp_r[j] = window[j] * ((FLOAT) savebuf[j]); + } + for (; j < 1024; j++) { + savebuf[j] = *buffer++; + wsamp_r[j] = window[j] * ((FLOAT) savebuf[j]); + } + for (; j < 1056; j++) + savebuf[j] = *buffer++; + + + /* Compute FFT */ + psycho_2_fft (wsamp_r, energy, phi); + + /* calculate the unpredictability measure, given energy[f] and phi[f] + (the age pointers [new/old/oldest] are reset automatically on the second pass */ + { + if (new == 0) { + new = 1; + oldest = 1; + } else { + new = 0; + oldest = 0; + } + if (old == 0) + old = 1; + else + old = 0; + } + + for (j = 0; j < HBLKSIZE; j++) { +#ifdef NEWATAN + double temp1, temp2, temp3; + r_prime = 2.0 * r[chn][old][j] - r[chn][oldest][j]; + phi_prime = 2.0 * phi_sav[chn][old][j] - phi_sav[chn][oldest][j]; + + r[chn][new][j] = sqrt ((double) energy[j]); + phi_sav[chn][new][j] = phi[j]; + + { + temp1 = + r[chn][new][j] * psycho_4_cos(phi[j]) - + r_prime * psycho_4_cos(phi_prime); + temp2 = + r[chn][new][j] * psycho_4_sin(phi[j]) - + r_prime * psycho_4_sin(phi_prime); + //fprintf(stdout,"[%5.2f %5.2f] [%5.2f %5.2f]\n",temp1, mytemp1, temp2, mytemp2); + + } + + + temp3 = r[chn][new][j] + fabs ((double) r_prime); + if (temp3 != 0) + c[j] = sqrt (temp1 * temp1 + temp2 * temp2) / temp3; + else + c[j] = 0; +#else + double temp1, temp2, temp3; + r_prime = 2.0 * r[chn][old][j] - r[chn][oldest][j]; + phi_prime = 2.0 * phi_sav[chn][old][j] - phi_sav[chn][oldest][j]; + + r[chn][new][j] = sqrt ((double) energy[j]); + phi_sav[chn][new][j] = phi[j]; + + + temp1 = + r[chn][new][j] * cos ((double) phi[j]) - + r_prime * cos ((double) phi_prime); + temp2 = + r[chn][new][j] * sin ((double) phi[j]) - + r_prime * sin ((double) phi_prime); + + temp3 = r[chn][new][j] + fabs ((double) r_prime); + if (temp3 != 0) + c[j] = sqrt (temp1 * temp1 + temp2 * temp2) / temp3; + else + c[j] = 0; +#endif + } + + /* For each partition, sum all the energy in that partition - grouped_e + and calculated the energy-weighted unpredictability measure - grouped_c + ISO 11172 Section D.2.4.e */ + for (j = 1; j < CBANDS; j++) { + grouped_e[j] = 0; + grouped_c[j] = 0; + } + grouped_e[0] = energy[0]; + grouped_c[0] = energy[0] * c[0]; + for (j = 1; j < HBLKSIZE; j++) { + grouped_e[partition[j]] += energy[j]; + grouped_c[partition[j]] += energy[j] * c[j]; + } + + /* convolve the grouped energy-weighted unpredictability measure + and the grouped energy with the spreading function + ISO 11172 D.2.4.f */ + for (j = 0; j < CBANDS; j++) { + ecb[j] = 0; + cb[j] = 0; + for (k = 0; k < CBANDS; k++) { + if (s[j][k] != 0.0) { + ecb[j] += s[j][k] * grouped_e[k]; + cb[j] += s[j][k] * grouped_c[k]; + } + } + if (ecb[j] != 0) + cb[j] = cb[j] / ecb[j]; + else + cb[j] = 0; + } + + /* Convert cb to tb (the tonality index) + ISO11172 SecD.2.4.g */ + for (i=0;i<CBANDS;i++) { + if (cb[i] < 0.05) + cb[i] = 0.05; + else if (cb[i] > 0.5) + cb[i] = 0.5; + tb[i] = -0.301029996 - 0.434294482 * log((double) cb[i]); + } + + + /* Calculate the required SNR for each of the frequency partitions + ISO 11172 Sect D.2.4.h */ + for (j = 0; j < CBANDS; j++) { + FLOAT SNR, SNRtemp; + SNRtemp = tmn[j] * tb[j] + NMT * (1.0 - tb[j]); + SNR = MAX(SNRtemp, minval[(int)cbval[j]]); + bc[j] = exp ((double) -SNR * LN_TO_LOG10); + } + + /* Calculate the permissible noise energy level in each of the frequency + partitions. + This section used to have pre-echo control but only for LayerI + ISO 11172 Sec D.2.4.k - Spread the threshold energy over FFT lines */ + for (j = 0; j < CBANDS; j++) { + if (rnorm[j] && numlines[j]) + nb[j] = ecb[j] * bc[j] / (rnorm[j] * numlines[j]); + else + nb[j] = 0; + } + + /* ISO11172 Sec D.2.4.l - thr[] the final energy threshold of audibility */ + for (j = 0; j < HBLKSIZE; j++) + thr[j] = MAX(nb[partition[j]], ath[j]); + + /* Translate the 512 threshold values to the 32 filter bands of the coder + Using ISO 11172 Table D.5 and Section D.2.4.n */ + for (j = 0; j < 193; j += 16) { + /* WIDTH = 0 */ + npart = 60802371420160.0; + epart = 0.0; + for (k = 0; k < 17; k++) { + if (thr[j + k] < npart) + npart = thr[j + k]; /* For WIDTH==0, find the minimum noise, and + later multiply by the number of indexes i.e. 17 */ + epart += energy[j + k]; + } + snrtmp[run][j / 16] = 4.342944819 * log((double)(epart/(npart*17.0))); + } + for (j = 208; j < (HBLKSIZE - 1); j += 16) { + /* WIDTH = 1 */ + npart = 0.0; + epart = 0.0; + for (k = 0; k < 17; k++) { + npart += thr[j + k]; /* For WIDTH==1, sum the noise */ + epart += energy[j + k]; + } + snrtmp[run][j / 16] = 4.342944819 * log ((double) (epart/npart)); + } + } + + /* Pick the maximum value of the two runs ISO 11172 Sect D.2.1 */ + for (i = 0; i < 32; i++) + smr[i] = MAX(snrtmp[0][i], snrtmp[1][i]); + +} + +/******************************** + * init psycho model 2 + ********************************/ +void psycho_4_init (double sfreq, options *glopts) +{ + int i, j; + + /* Allocate memory for all the static variables */ + psycho_4_allocmem(); + + /* Set up the SIN/COS tables */ + psycho_4_trigtable_init(); + + /* calculate HANN window coefficients */ + for (i = 0; i < BLKSIZE; i++) + window[i] = 0.5 * (1 - cos (2.0 * PI * (i - 0.5) / BLKSIZE)); + + /* For each FFT line from 0(DC) to 512(Nyquist) calculate + - bark : the bark value of this fft line + - ath : the absolute threshold of hearing for this line [ATH] + + Since it is a 1024 point FFT, each line in the fft corresponds + to 1/1024 of the total frequency. + Line 0 should correspond to DC - which doesn't really have a ATH afaik + Line 1 should be 1/1024th of the Sampling Freq + Line 512 should be the nyquist freq */ + for (i=0; i<HBLKSIZE; i++) { + FLOAT freq = i * sfreq/BLKSIZE; + bark[i] = freq2bark(freq); + /* The ath tables in the dist10 code seem to be a little out of kilter. + they seem to start with index 0 corresponding to (sampling freq)/1024. + When in doubt, i'm going to assume that the dist10 code is wrong. MFC Feb2003 */ + ath[i] = ATH_energy(freq,glopts->athlevel); + //fprintf(stdout,"%.2f ",ath[i]); + } + + + /* Work out the partitions + Starting from line 0, all lines within 0.33 of the starting + bark are added to the same partition. When a line is greater + by 0.33 of a bark, start a new partition. */ + int partition_count = 0; /* keep a count of the partitions */ + int cbase = 0; /* current base index for the bark range calculation */ + for (i=0;i<HBLKSIZE;i++) { + if ((bark[i] - bark[cbase]) > 0.33) { /* 1/3 critical band? */ + /* this frequency line is too different from the starting line, + (in terms of the bark distance) + so close that previous partition, and make this line the first + member of the next partition */ + cbase = i; /* Start the new partition from this frequency */ + partition_count++; + } + /* partition[i] tells us which partition the i'th frequency line is in */ + partition[i] = partition_count; + /* keep a count of how many frequency lines are in each partition */ + numlines[partition_count]++; + } + + /* For each partition within the frequency space, + calculate the average bark value - cbval [central bark value] */ + for (i=0;i<HBLKSIZE;i++) + cbval[partition[i]] += bark[i]; /* sum up all the bark values */ + for (i=0;i<CBANDS;i++) { + if (numlines[i] != 0) + cbval[i] /= numlines[i]; /* divide by the number of values */ + else { + cbval[i]=0; /* this isn't a partition */ + } + } + + + /* Calculate the spreading function. ISO 11172 Section D.2.3 */ + for (i=0;i<CBANDS;i++) { + for (j=0;j<CBANDS;j++) { + s[i][j] = psycho_4_spreading_function( 1.05 * (cbval[i] - cbval[j]) ); + rnorm[i] += s[i][j]; /* sum the spreading function values for each partition so that + they can be normalised later on */ + } + } + + /* Calculate Tone Masking Noise values. ISO 11172 Tables D.3.x */ + for (j = 0; j < CBANDS; j++) + tmn[j] = MAX(15.5+cbval[j], 24.5); + + + if (glopts->verbosity > 10) { + /* Dump All the Values to STDOUT */ + int wlow, whigh=0; + int ntot=0; + fprintf(stdout,"psy model 4 init\n"); + fprintf(stdout,"index \tnlines \twlow \twhigh \tbval \tminval \ttmn\n"); + for (i=0;i<CBANDS;i++) + if (numlines[i] != 0) { + wlow = whigh+1; + whigh = wlow + numlines[i] - 1; + fprintf(stdout,"%i \t%i \t%i \t%i \t%5.2f \t%4.2f \t%4.2f\n",i+1, numlines[i],wlow, whigh, cbval[i],minval[(int)cbval[i]],tmn[i]); + ntot += numlines[i]; + } + fprintf(stdout,"total lines %i\n",ntot); + exit(0); + } +} + +/* The spreading function. Values returned in units of energy + Argument 'bark' is the difference in bark values between the + centre of two partitions. + This has been taken from LAME. MFC Feb 2003 */ +FLOAT8 psycho_4_spreading_function(FLOAT8 bark) { + + FLOAT8 tempx,x,tempy,temp; + tempx = bark; +#ifdef LAME + /* MP3 standard actually spreads these values a little more */ + if (tempx>=0) tempx *= 3; + else tempx *=1.5; +#endif + + if(tempx>=0.5 && tempx<=2.5) + { + temp = tempx - 0.5; + x = 8.0 * (temp*temp - 2.0 * temp); + } + else x = 0.0; + tempx += 0.474; + tempy = 15.811389 + 7.5*tempx - 17.5*sqrt(1.0+tempx*tempx); + + if (tempy <= -60.0) return 0.0; + + tempx = exp( (x + tempy)*LN_TO_LOG10 ); + +#ifdef LAME + /* I'm not sure where the magic value of 0.6609193 comes from. + toolame will just keep using the rnorm to normalise the spreading function + MFC Feb 2003 */ + /* Normalization. The spreading function should be normalized so that: + +inf + / + | s3 [ bark ] d(bark) = 1 + / + -inf + */ + tempx /= .6609193; +#endif + return tempx; + +} + +void psycho_4_allocmem() { + grouped_c = (FLOAT *) mem_alloc (sizeof (FCB), "grouped_c"); + grouped_e = (FLOAT *) mem_alloc (sizeof (FCB), "grouped_e"); + nb = (FLOAT *) mem_alloc (sizeof (FCB), "nb"); + cb = (FLOAT *) mem_alloc (sizeof (FCB), "cb"); + tb = (FLOAT *) mem_alloc (sizeof (FCB), "tb"); + ecb = (FLOAT *) mem_alloc (sizeof (FCB), "ecb"); + bc = (FLOAT *) mem_alloc (sizeof (FCB), "bc"); + wsamp_r = (FLOAT *) mem_alloc (sizeof (FBLK), "wsamp_r"); + phi = (FLOAT *) mem_alloc (sizeof (FBLK), "phi"); + energy = (FLOAT *) mem_alloc (sizeof (FBLK), "energy"); + c = (FLOAT *) mem_alloc (sizeof (FHBLK), "c"); + bark = (FLOAT *) mem_alloc (sizeof (FHBLK), "bark"); + thr = (FLOAT *) mem_alloc (sizeof (FHBLK), "thr"); + snrtmp = (F32 *) mem_alloc (sizeof (F2_32), "snrtmp"); + + numlines = (int *) mem_alloc (sizeof (ICB), "numlines"); + partition = (int *) mem_alloc (sizeof (IHBLK), "partition"); + cbval = (FLOAT *) mem_alloc (sizeof (FCB), "cbval"); + rnorm = (FLOAT *) mem_alloc (sizeof (FCB), "rnorm"); + window = (FLOAT *) mem_alloc (sizeof (FBLK), "window"); + ath = (FLOAT *) mem_alloc (sizeof (FHBLK), "ath"); + tmn = (double *) mem_alloc (sizeof (DCB), "tmn"); + s = (FCB *) mem_alloc (sizeof (FCBCB), "s"); + lthr = (FHBLK *) mem_alloc (sizeof (F2HBLK), "lthr"); + r = (F2HBLK *) mem_alloc (sizeof (F22HBLK), "r"); + phi_sav = (F2HBLK *) mem_alloc (sizeof (F22HBLK), "phi_sav"); + +} + + + + + |