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UHSDR/UHSDR-active-devel/mchf-eclipse/drivers/freedv/newamp2.c

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2022-11-08 16:13:55 +01:00
/*---------------------------------------------------------------------------*\
FILE........: newamp2.c
AUTHOR......: Thomas Kurin and Stefan Erhardt
INSTITUTE...: Institute for Electronics Engineering, University of Erlangen-Nuremberg
DATE CREATED: July 2018
BASED ON....: "newamp1" by David Rowe
Quantisation functions for the sinusoidal coder, using "newamp1"
algorithm that resamples variable rate L [Am} to a fixed rate K then
VQs.
\*---------------------------------------------------------------------------*/
/*
Copyright David Rowe 2017
All rights reserved.
This program is free software; you can redistribute it and/or modify
it under the terms of the GNU Lesser General Public License version 2.1, as
published by the Free Software Foundation. This program is
distributed in the hope that it will be useful, but WITHOUT ANY
WARRANTY; without even the implied warranty of MERCHANTABILITY or
FITNESS FOR A PARTICULAR PURPOSE. See the GNU General Public
License for more details.
You should have received a copy of the GNU Lesser General Public License
along with this program; if not, see <http://www.gnu.org/licenses/>.
*/
#include <assert.h>
#include <stdio.h>
#include <stdlib.h>
#include <string.h>
#include <math.h>
#include "defines.h"
#include "phase.h"
#include "quantise.h"
#include "mbest.h"
#include "newamp1.h"
#include "newamp2.h"
/*---------------------------------------------------------------------------*\
FUNCTION....: n2_mel_sample_freqs_kHz()
AUTHOR......: Thomas Kurin and Stefan Erhardt
INSTITUTE...: Institute for Electronics Engineering, University of Erlangen-Nuremberg
DATE CREATED: July 2018
Outputs fixed frequencies for the K-Vectors to be able to work with both 8k and 16k mode.
\*---------------------------------------------------------------------------*/
void n2_mel_sample_freqs_kHz(float rate_K_sample_freqs_kHz[], int K)
{
float freq[] = {0.199816, 0.252849, 0.309008, 0.368476, 0.431449, 0.498134, 0.568749, 0.643526, 0.722710, 0.806561, 0.895354, 0.989380,
1.088948, 1.194384, 1.306034, 1.424264, 1.549463, 1.682041, 1.822432, 1.971098, 2.128525, 2.295232, 2.471763, 2.658699,
2.856652, 3.066272, 3.288246, 3.523303, 3.772214, 4.035795, 4.314912, 4.610478, 4.923465, 5.254899, 5.605865, 5.977518,
6.371075, 6.787827, 7.229141, 7.696465};
int k;
//printf("\n\n");
for (k=0; k<K; k++) {
rate_K_sample_freqs_kHz[k] = freq[k];
// printf("%f ",mel);
// printf("%f \n",rate_K_sample_freqs_kHz[k]);
}
}
/*---------------------------------------------------------------------------*\
FUNCTION....: n2_resample_const_rate_f() still equal to resample_const_rate_f()
AUTHOR......: David Rowe
DATE CREATED: Jan 2017
Resample Am from time-varying rate L=floor(pi/Wo) to fixed rate K.
\*---------------------------------------------------------------------------*/
void n2_resample_const_rate_f(C2CONST *c2const, MODEL *model, float rate_K_vec[], float rate_K_sample_freqs_kHz[], int K)
{
int m;
float AmdB[MAX_AMP+1], rate_L_sample_freqs_kHz[MAX_AMP+1], AmdB_peak;
/* convert rate L=pi/Wo amplitude samples to fixed rate K */
AmdB_peak = -100.0;
for(m=1; m<=model->L; m++) {
AmdB[m] = 20.0*log10(model->A[m]+1E-16);
if (AmdB[m] > AmdB_peak) {
AmdB_peak = AmdB[m];
}
rate_L_sample_freqs_kHz[m] = m*model->Wo*(c2const->Fs/2000.0)/M_PI;
//printf("m: %d AmdB: %f AmdB_peak: %f sf: %f\n", m, AmdB[m], AmdB_peak, rate_L_sample_freqs_kHz[m]);
}
/* clip between peak and peak -50dB, to reduce dynamic range */
for(m=1; m<=model->L; m++) {
if (AmdB[m] < (AmdB_peak-50.0)) {
AmdB[m] = AmdB_peak-50.0;
}
}
interp_para(rate_K_vec, &rate_L_sample_freqs_kHz[1], &AmdB[1], model->L, rate_K_sample_freqs_kHz, K);
}
/*---------------------------------------------------------------------------*\
FUNCTION....: n2_rate_K_mbest_encode
AUTHOR......: Thomas Kurin and Stefan Erhardt
INSTITUTE...: Institute for Electronics Engineering, University of Erlangen-Nuremberg
DATE CREATED: July 2018
One stage rate K newamp2 VQ quantiser using mbest search.
\*---------------------------------------------------------------------------*/
void n2_rate_K_mbest_encode(int *indexes, float *x, float *xq, int ndim)
{
int i, n1;
const float *codebook1 = newamp2vq_cb[0].cb;
struct MBEST *mbest_stage1;
float w[ndim];
int index[1];
/* codebook is compiled for a fixed K */
//assert(ndim == newamp2vq_cb[0].k);
/* equal weights, could be argued mel freq axis gives freq dep weighting */
for(i=0; i<ndim; i++)
w[i] = 1.0;
mbest_stage1 = mbest_create(1);
index[0] = 0;
/* Stage 1 */
mbest_search450(codebook1, x, w, ndim,NEWAMP2_K, newamp2vq_cb[0].m, mbest_stage1, index);
MBEST_PRINT("Stage 1:", mbest_stage1);
n1 = mbest_stage1->list[0].index[0];
mbest_destroy(mbest_stage1);
//indexes[1]: legacy from newamp1
indexes[0] = n1; indexes[1] = n1;
}
/*---------------------------------------------------------------------------*\
FUNCTION....: n2_resample_rate_L
AUTHOR......: Thomas Kurin and Stefan Erhardt
INSTITUTE...: Institute for Electronics Engineering, University of Erlangen-Nuremberg
DATE CREATED: July 2018
Decoder side conversion of rate K vector back to rate L.
Plosives are set to zero for the first 2 of 4 frames.
\*---------------------------------------------------------------------------*/
void n2_resample_rate_L(C2CONST *c2const, MODEL *model, float rate_K_vec[], float rate_K_sample_freqs_kHz[], int K,int plosive_flag)
{
float rate_K_vec_term[K+2], rate_K_sample_freqs_kHz_term[K+2];
float AmdB[MAX_AMP+1], rate_L_sample_freqs_kHz[MAX_AMP+1];
int m,k;
/* terminate either end of the rate K vecs with 0dB points */
rate_K_vec_term[0] = rate_K_vec_term[K+1] = 0.0;
rate_K_sample_freqs_kHz_term[0] = 0.0;
rate_K_sample_freqs_kHz_term[K+1] = 4.0;
for(k=0; k<K; k++) {
rate_K_vec_term[k+1] = rate_K_vec[k];
rate_K_sample_freqs_kHz_term[k+1] = rate_K_sample_freqs_kHz[k];
//printf("k: %d f: %f rate_K: %f\n", k, rate_K_sample_freqs_kHz[k], rate_K_vec[k]);
}
for(m=1; m<=model->L; m++) {
rate_L_sample_freqs_kHz[m] = m*model->Wo*(c2const->Fs/2000.0)/M_PI;
}
interp_para(&AmdB[1], rate_K_sample_freqs_kHz_term, rate_K_vec_term, K+2, &rate_L_sample_freqs_kHz[1], model->L);
for(m=1; m<=model->L; m++) {
if(plosive_flag==0){
model->A[m] = pow(10.0, AmdB[m]/20.0);
}else{
model->A[m] = 0.1;
}
// printf("m: %d f: %f AdB: %f A: %f\n", m, rate_L_sample_freqs_kHz[m], AmdB[m], model->A[m]);
}
}
/*---------------------------------------------------------------------------*\
FUNCTION....: n2_post_filter_newamp2
AUTHOR......: Thomas Kurin and Stefan Erhardt
INSTITUTE...: Institute for Electronics Engineering, University of Erlangen-Nuremberg
DATE CREATED: July 2018
Postfilter for the pseudo wideband mode. Still has to be adapted!
\*---------------------------------------------------------------------------*/
void n2_post_filter_newamp2(float vec[], float sample_freq_kHz[], int K, float pf_gain)
{
int k;
/*
vec is rate K vector describing spectrum of current frame lets
pre-emp before applying PF. 20dB/dec over 300Hz. Postfilter
affects energy of frame so we measure energy before and after
and normalise. Plenty of room for experiment here as well.
*/
float pre[K];
float e_before = 0.0;
float e_after = 0.0;
for(k=0; k<K; k++) {
pre[k] = 20.0*log10f(sample_freq_kHz[k]/0.3);
vec[k] += pre[k];
e_before += POW10F(vec[k]/10.0);
vec[k] *= pf_gain;
e_after += POW10F(vec[k]/10.0);
}
float gain = e_after/e_before;
float gaindB = 10*log10f(gain);
for(k=0; k<K; k++) {
vec[k] -= gaindB;
vec[k] -= pre[k];
}
}
/*---------------------------------------------------------------------------*\
FUNCTION....: newamp2_model_to_indexes
AUTHOR......: Thomas Kurin and Stefan Erhardt
INSTITUTE...: Institute for Electronics Engineering, University of Erlangen-Nuremberg
DATE CREATED: July 2018
newamp2 encoder: Encodes the 8k sampled samples using mbest search (one stage)
\*---------------------------------------------------------------------------*/
void newamp2_model_to_indexes(C2CONST *c2const,
int indexes[],
MODEL *model,
float rate_K_vec[],
float rate_K_sample_freqs_kHz[],
int K,
float *mean,
float rate_K_vec_no_mean[],
float rate_K_vec_no_mean_[],
int plosive
)
{
int k;
/* convert variable rate L to fixed rate K */
resample_const_rate_f(c2const, model, rate_K_vec, rate_K_sample_freqs_kHz, K);
/* remove mean and two stage VQ */
float sum = 0.0;
for(k=0; k<K; k++)
sum += rate_K_vec[k];
*mean = sum/K;
for(k=0; k<K; k++)
{
rate_K_vec_no_mean[k] = rate_K_vec[k] - *mean;
}
//NEWAMP2_16K_K+1 because the last vector is not a vector for VQ (and not included in the constant)
//but a calculated medium mean value
n2_rate_K_mbest_encode(indexes, rate_K_vec_no_mean, rate_K_vec_no_mean_, NEWAMP2_16K_K+1);
/* scalar quantise mean (effectively the frame energy) */
float w[1] = {1.0};
float se;
indexes[2] = quantise(newamp2_energy_cb[0].cb,
mean,
w,
newamp2_energy_cb[0].k,
newamp2_energy_cb[0].m,
&se);
/* scalar quantise Wo. We steal the smallest Wo index to signal
an unvoiced frame */
if (model->voiced) {
int index = encode_log_Wo(c2const, model->Wo, 6);
if (index == 0) {
index = 1;
}
if (index == 63) {
index = 62;
}
indexes[3] = index;
}
else {
indexes[3] = 0;
}
if(plosive != 0){
indexes[3] = 63;
}
}
/*---------------------------------------------------------------------------*\
FUNCTION....: newamp2_indexes_to_rate_K_vec
AUTHOR......: Thomas Kurin and Stefan Erhardt
INSTITUTE...: Institute for Electronics Engineering, University of Erlangen-Nuremberg
DATE CREATED: July 2018
newamp2 decoder for amplitudes {Am}. Given the rate K VQ and energy
indexes, outputs rate K vector. Equal to newamp1 but using only one stage VQ.
\*---------------------------------------------------------------------------*/
void newamp2_indexes_to_rate_K_vec(float rate_K_vec_[],
float rate_K_vec_no_mean_[],
float rate_K_sample_freqs_kHz[],
int K,
float *mean_,
int indexes[],
float pf_gain)
{
int k;
const float *codebook1 = newamp2vq_cb[0].cb;
int n1 = indexes[0];
for(k=0; k<K; k++) {
rate_K_vec_no_mean_[k] = codebook1[(NEWAMP2_16K_K+1)*n1+k];
}
post_filter_newamp1(rate_K_vec_no_mean_, rate_K_sample_freqs_kHz, K, pf_gain);
*mean_ = newamp2_energy_cb[0].cb[indexes[2]];
for(k=0; k<K; k++) {
rate_K_vec_[k] = rate_K_vec_no_mean_[k] + *mean_;
}
}
/*---------------------------------------------------------------------------*\
FUNCTION....: newamp2_16k_indexes_to_rate_K_vec
AUTHOR......: Thomas Kurin and Stefan Erhardt
INSTITUTE...: Institute for Electronics Engineering, University of Erlangen-Nuremberg
DATE CREATED: July 2018
newamp2 decoder for amplitudes {Am}. Given the rate K VQ and energy
indexes, outputs rate K vector. Extends the sample rate by looking up the corresponding
higher frequency values with their energy difference to the base energy (=>mean2)
\*---------------------------------------------------------------------------*/
void newamp2_16k_indexes_to_rate_K_vec(float rate_K_vec_[],
float rate_K_vec_no_mean_[],
float rate_K_sample_freqs_kHz[],
int K,
float *mean_,
int indexes[],
float pf_gain)
{
int k;
const float *codebook1 = newamp2vq_cb[0].cb;
float mean2 = 0;
int n1 = indexes[0];
for(k=0; k<K; k++) {
rate_K_vec_no_mean_[k] = codebook1[(K+1)*n1+k];
}
n2_post_filter_newamp2(rate_K_vec_no_mean_, rate_K_sample_freqs_kHz, K, pf_gain);
*mean_ = newamp2_energy_cb[0].cb[indexes[2]];
mean2 = *mean_ + codebook1[(K+1)*n1+K] -10;
//HF ear Protection
if(mean2>50){
mean2 = 50;
}
for(k=0; k<K; k++) {
if(k<NEWAMP2_K){
rate_K_vec_[k] = rate_K_vec_no_mean_[k] + *mean_;
}
else{
//Amplify or Reduce ??
rate_K_vec_[k] = rate_K_vec_no_mean_[k] + mean2;
}
}
}
/*---------------------------------------------------------------------------*\
FUNCTION....: newamp2_interpolate
AUTHOR......: Thomas Kurin and Stefan Erhardt
INSTITUTE...: Institute for Electronics Engineering, University of Erlangen-Nuremberg
DATE CREATED: July 2018
Interpolates to the 4 10ms Frames and leaves the forst 2 empty for plosives
\*---------------------------------------------------------------------------*/
void newamp2_interpolate(float interpolated_surface_[], float left_vec[], float right_vec[], int K, int plosive_flag)
{
int i, k;
int M = 4;
float c;
/* (linearly) interpolate 25Hz amplitude vectors back to 100Hz */
if(plosive_flag == 0){
for(i=0,c=1.0; i<M; i++,c-=1.0/M) {
for(k=0; k<K; k++) {
interpolated_surface_[i*K+k] = left_vec[k]*c + right_vec[k]*(1.0-c);
}
}
}
else{
for(i=0,c=1.0; i<M; i++,c-=1.0/M) {
for(k=0; k<K; k++) {
if(i<2){
interpolated_surface_[i*K+k] = 0;
}
else{
//perhaps add some dB ?
interpolated_surface_[i*K+k] = right_vec[k];
}
}
}
}
}
/*---------------------------------------------------------------------------*\
FUNCTION....: newamp2_indexes_to_model
AUTHOR......: Thomas Kurin and Stefan Erhardt
INSTITUTE...: Institute for Electronics Engineering, University of Erlangen-Nuremberg
DATE CREATED: July 2018
newamp2 decoder. Chooses whether to decode to 16k mode or to 8k mode
\*---------------------------------------------------------------------------*/
void newamp2_indexes_to_model(C2CONST *c2const,
MODEL model_[],
COMP H[],
float *interpolated_surface_,
float prev_rate_K_vec_[],
float *Wo_left,
int *voicing_left,
float rate_K_sample_freqs_kHz[],
int K,
codec2_fft_cfg fwd_cfg,
codec2_fft_cfg inv_cfg,
int indexes[],
float pf_gain,
int flag16k)
{
float rate_K_vec_[K], rate_K_vec_no_mean_[K], mean_, Wo_right;
int voicing_right, k;
int M = 4;
/* extract latest rate K vector */
if(flag16k == 0){
newamp2_indexes_to_rate_K_vec(rate_K_vec_,
rate_K_vec_no_mean_,
rate_K_sample_freqs_kHz,
K,
&mean_,
indexes,
pf_gain);
}else{
newamp2_16k_indexes_to_rate_K_vec(rate_K_vec_,
rate_K_vec_no_mean_,
rate_K_sample_freqs_kHz,
K,
&mean_,
indexes,
pf_gain);
}
/* decode latest Wo and voicing and plosive */
int plosive_flag = 0;
//Voiced with Wo
if (indexes[3]>0 && indexes[3]<63) {
Wo_right = decode_log_Wo(c2const, indexes[3], 6);
voicing_right = 1;
}
//Unvoiced
else if(indexes[3] == 0){
Wo_right = 2.0*M_PI/100.0;
voicing_right = 0;
}
//indexes[3]=63 (= Plosive) and unvoiced
else {
Wo_right = 2.0*M_PI/100.0;
voicing_right = 0;
plosive_flag = 1;
}
/* interpolate 25Hz rate K vec back to 100Hz */
float *left_vec = prev_rate_K_vec_;
float *right_vec = rate_K_vec_;
newamp2_interpolate(interpolated_surface_, left_vec, right_vec, K,plosive_flag);
/* interpolate 25Hz v and Wo back to 100Hz */
float aWo_[M];
int avoicing_[M], aL_[M], i;
interp_Wo_v(aWo_, aL_, avoicing_, *Wo_left, Wo_right, *voicing_left, voicing_right);
/* back to rate L amplitudes, synthesis phase for each frame */
for(i=0; i<M; i++) {
model_[i].Wo = aWo_[i];
model_[i].L = aL_[i];
model_[i].voiced = avoicing_[i];
//Plosive Detected
if(plosive_flag>0){
//First two frames are set to zero
if (i<2){
n2_resample_rate_L(c2const, &model_[i], &interpolated_surface_[K*i], rate_K_sample_freqs_kHz, K,1);
}
else{
n2_resample_rate_L(c2const, &model_[i], &interpolated_surface_[K*i], rate_K_sample_freqs_kHz, K,0);
}
}
//No Plosive, standard resample
else{
n2_resample_rate_L(c2const, &model_[i], &interpolated_surface_[K*i], rate_K_sample_freqs_kHz, K,0);
}
determine_phase(c2const, &H[(MAX_AMP+1)*i], &model_[i], NEWAMP2_PHASE_NFFT, fwd_cfg, inv_cfg);
}
/* update memories for next time */
for(k=0; k<K; k++) {
prev_rate_K_vec_[k] = rate_K_vec_[k];
}
*Wo_left = Wo_right;
*voicing_left = voicing_right;
}
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