function out = sig_li2020(varargin)
% SIG_LI2020 modification of HRTFs/BRIRs for the Li2020 experiments
%
% Usage: HRTFs = sig_li2020(exp)
%
% Input parameters:
% exp : Experiment (exp A, exp B, exp C, exp D, exp E)
%
% Output parameters:
% Obj : modified HRTFs/BRIRs
%
% SIG_LI2020 generates modified HRTFs or BRIRs from
% Li et al. (2020) as specified by the exp flag.
%
% exp1 - exp4 (size of out matrix):
% 5x256x5x2 <---> Nr. subjects x HRIR length x conditions x left/right
% exp 5 (size of out matrix):
% 5x16384x5x5x2 <---> Nr. subjects x BRIR length x smoothing condition x compression condition x left/right
%
% Examples:
% ---------
% To get measured modified HRTFs for experiment A:
%
% sig_li2020('exp1');
%
% To get measured modified HRTFs for experiment B:
%
% sig_li2020('exp2');
%
% To get measured modified HRTFs for experiment C:
%
% sig_li2020('exp3');
%
% To get measured modified HRTFs for experiment D:
%
% sig_li2020('exp4');
%
% To get measured modified HRTFs for experiment E:
%
% sig_li2020('exp5');
%
% Url: http://amtoolbox.org/amt-1.2.0/doc/signals/sig_li2020.php
% Copyright (C) 2009-2022 Piotr Majdak, Clara Hollomey, and the AMT team.
% This file is part of Auditory Modeling Toolbox (AMT) version 1.2.0
%
% This program is free software: you can redistribute it and/or modify
% it under the terms of the GNU General Public License as published by
% the Free Software Foundation, either version 3 of the License, or
% (at your option) any later version.
%
% 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 General Public License
% along with this program. If not, see <http://www.gnu.org/licenses/>.
% Requirements:
% -------------
%
% 1) Data in hrtf/li2020 and auxdata/li2020 (Raw_BRIR_HRTF_dataset)
% References:
% S. Li, R. Baumgartner, and J. Peissig.
% Modeling perceived externalization of a static, lateral sound image.
% Acta Acust.,4(5) (2020)
% The implementation is based on data_hassager2016.m, sig_baumgartner2017looming.
% Copyright (C) 2009-2015 Piotr Majdak and the AMT team.
% This file is part of Auditory Modeling Toolbox (AMT) version 0.9.9
%
% This program is free software: you can redistribute it and/or modify
% it under the terms of the GNU General Public License as published by
% the Free Software Foundation, either version 3 of the License, or
% (at your option) any later version.
%
% 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 General Public License
% along with this program. If not, see <http://www.gnu.org/licenses/>.
% AUTHOR: Song Li, Institute of Communications Technology, Leibniz
% University of Hannover, Germany
%% Check input
definput.keyvals.Obj = [];
definput.flags.experiment = {'exp1','exp2','exp3','exp4','exp5'};
[flags,kv]=ltfatarghelper({'Obj'},definput,varargin);
%% HRTF/BRIR manipulation
fs =44100;
hrir_dataset = load('AMT Implementation\data\Raw_BRIR_HRTF_dataset.mat');
if flags.do_exp1 || flags.do_exp2 || flags.do_exp3 || flags.do_exp4
% Load original HRTFs
% size: 5 x 256 x 2
% 5: number of subject
% 256: HRIR length
% 2: left & right HRIR
dim = size(hrir_dataset.hrir_90_deg);
hrir_smooth =1; % Opt: smoohting to reduce the irreverent spectral details
hrir_template = zeros(dim);
if (hrir_smooth ==1)
% Opt: smoohting to reduce the irreverent spectral details
for i = 1: dim(1)
hrir_template(i,:,1:2) = sig_hassager2016(squeeze(hrir_dataset.hrir_90_deg(i,:,:)),.2,fs);
end
else
hrir_template = hrir_dataset.hrir_90_deg;
end
elseif flags.do_exp5
dim_pre = size(hrir_dataset.brir_90_deg);
brir_padded=zeros(dim_pre(1),2^nextpow2(length(hrir_dataset.brir_90_deg)),dim_pre(3));
for i=1:dim_pre(1)
brir_padded(i,:,:) = padarray(squeeze(hrir_dataset.brir_90_deg(i,:,:)),2^nextpow2(length(hrir_dataset.brir_90_deg))-dim_pre(2),0,'post');
end
hrir_dataset.brir_90_deg = brir_padded;
dim = size(hrir_dataset.brir_90_deg);
brir_smooth =1; % Opt: smoohting to reduce the irreverent spectral details
%window for extraction the direct sound part
wlen = 44*2; %length of window for raw IR measurements
wend1=110; %2.5 ms
win = tukeywin(wlen);
win_direct=[ones((wend1-wlen/4),1);win(length(win)*3/4+1:end);zeros((dim(2)-wend1),1)];
win_reverb=1-win_direct;
%3 direct sound extraction
brir_template_direct_raw = zeros(dim);
brir_template_direct = zeros(dim);
brir_template_reverb = zeros(dim);
for i = 1: dim(1)
brir_template_direct_raw(i,:,1:2) = squeeze(hrir_dataset.brir_90_deg(i,:,1:2)) .* win_direct;
brir_template_reverb(i,:,1:2) = squeeze(hrir_dataset.brir_90_deg(i,:,1:2)) .* win_reverb;
end
if (brir_smooth ==1)
for i = 1: dim(1)
brir_template_direct(i,:,1:2) = sig_hassager2016(squeeze(brir_template_direct_raw(i,:,:)),.2,fs);
end
else
brir_template_direct = brir_template_direct_raw;
end
end
%% Experiments
%% Experiment 1
if flags.do_exp1
%% Exp1: Modification of ILDs
ILD_increase=[0 5 10 15 20]; % ILD increase level
len_hrir=256;
hrir_low_modified_Exp1 = zeros(5,len_hrir,length(ILD_increase),2); %ILD compression at low frequencies
hrir_high_modified_Exp1 = zeros(5,len_hrir,length(ILD_increase),2); %ILD compression at high frequencies
hrir_bb_modified_Exp1 = zeros(5,len_hrir,length(ILD_increase),2); %ILD compression at broadband
for i = 1: dim(1)
individual_hrir_template=squeeze(hrir_template(i,:,1:2));
for k=1:length(ILD_increase)
hrir_low_modified_Exp1(i,:,k,:) = fun_ILD_increase(individual_hrir_template,fs,ILD_increase(k),200,3000);
hrir_high_modified_Exp1(i,:,k,:) = fun_ILD_increase(individual_hrir_template,fs,ILD_increase(k),3000,16000);
hrir_bb_modified_Exp1(i,:,k,:) = fun_ILD_increase(individual_hrir_template,fs,ILD_increase(k),200,16000);
end
end
out.HRTF_low = hrir_low_modified_Exp1;
out.HRTF_high = hrir_high_modified_Exp1;
out.HRTF_bb = hrir_bb_modified_Exp1;
end
%% Experiment 2
if flags.do_exp2
%% Exp2: Reaming the ILD, while reducing the magnitude spectral of one ear
bdwidth=[0 1 4 16 64]; % specra compression level
len_hrir=256;
hrir_modified_Exp2 = zeros(5,len_hrir,length(bdwidth),2);
for i = 1: dim(1)
individual_hrir_template=squeeze(hrir_template(i,:,1:2));
for k=1:length(bdwidth)
hrir_modified_Exp2(i,:,k,:) = fun_ipsi_compress(individual_hrir_template,fs,bdwidth(k));
end
end
out.HRTF = hrir_modified_Exp2;
end
%% Experiment 3
if flags.do_exp3
%% Exp3: Reducing the ILD contrast, while keeping the magnitude spectral of one ear
compression_factor=[1,0.75,0.5,0.25,0]; % ILD compression factor
len_hrir=256;
hrir_ipsi_modified_Exp3 = zeros(5,len_hrir,length(compression_factor),2); %modified ipsilateral HRTF
hrir_contra_modified_Exp3 = zeros(5,len_hrir,length(compression_factor),2); %modified contralateral HRTF
for i = 1: dim(1)
individual_hrir_template=squeeze(hrir_template(i,:,1:2));
for k=1:length(compression_factor)
[hrir_ipsi_modified_Exp3(i,:,k,:), hrir_contra_modified_Exp3(i,:,k,:)]=...
fun_ILD_compress(individual_hrir_template,fs,compression_factor(k),3000,16000);
end
end
out.HRTF_ipsi = hrir_ipsi_modified_Exp3;
out.HRTF_contra = hrir_contra_modified_Exp3;
end
%% Experiment 4
if flags.do_exp4
%% Exp4: reducing the spectral magnitude of one ear
bdwidth=[0 1 4 16 64];
len_hrir=256;
hrir_both_modified_Exp4 = zeros(5,len_hrir,length(bdwidth),2); %HRTF compression at both ear
hrir_ipsi_modified_Exp4 = zeros(5,len_hrir,length(bdwidth),2); %HRTF compression at ipsilateral ear
hrir_contra_modified_Exp4 = zeros(5,len_hrir,length(bdwidth),2); %HRTF compression at contralateral ear
for i = 1: dim(1)
individual_hrir_template=squeeze(hrir_template(i,:,1:2));
for k=1:length(bdwidth)
if (k==1)
y_modified=sig_hassager2016(individual_hrir_template,0.001,fs);
else
y_modified=sig_hassager2016(individual_hrir_template, bdwidth(k),fs);
end
hrir_both_modified_Exp4(i,:,k,:) = [y_modified(:,1), y_modified(:,2)];
hrir_ipsi_modified_Exp4(i,:,k,:) = [y_modified(:,1), individual_hrir_template(:,2)];
hrir_contra_modified_Exp4(i,:,k,:) = [individual_hrir_template(:,1), y_modified(:,2)];
end
end
out.HRTF_ipsi = hrir_ipsi_modified_Exp4;
out.HRTF_contra = hrir_contra_modified_Exp4;
out.HRTF_both = hrir_both_modified_Exp4;
end
%% Experiment 5
if flags.do_exp5
%% Exp5: reducing the spectral magnitude of one ear
bdwidth=[0,1,4,16,64];
compression_factor=[1,0.75,0.5,0.25,0];
len_hrir=256;
brir_both_modified_Exp5 = zeros(5,dim(2),length(bdwidth),length(compression_factor), 2); %BRIR compression at both ear
for i = 1:dim(1)
individual_brir_direct_template=squeeze(brir_template_direct(i,:,1:2));
individual_brir_reverb_template=squeeze(brir_template_reverb(i,:,1:2));
for k=1:length(bdwidth)
for j=1:length(compression_factor)
if (k==1)
brir_both_modified_Exp5(i,:,k,j,:) = ...
[sig_hassager2016(individual_brir_direct_template(1:len_hrir,:),0.01,fs);zeros(dim(2)-len_hrir,2)]+compression_factor(j)*individual_brir_reverb_template;
else
brir_both_modified_Exp5(i,:,k,j,:) = ...
[sig_hassager2016(individual_brir_direct_template(1:len_hrir,:),bdwidth(k),fs);zeros(dim(2)-len_hrir,2)]+compression_factor(j)*individual_brir_reverb_template;
end
end
end
end
out.BRIR = brir_both_modified_Exp5;
end
end
%% functions
function modified_hrir=fun_ILD_increase(hrir_part,fs,ILD_increase,f_low,f_high)
Nfft=length(hrir_part);
HRTF_part=fftreal(hrir_part);
HRTF_mag_part=db(abs(HRTF_part));
[~,excessPhaseTF] = RB_minphase(hrir_part,1,'freq');
ILD_ref=HRTF_mag_part(:,1)-HRTF_mag_part(:,2);
freq = 0:fs/Nfft:fs/2;
idf = freq >= f_low-1 & freq <= f_high+1; % indices for dedicated frequency range
modILD_mag=ILD_ref; % Initiate the modified ILD magnitude
modILD_mag(idf,:)=ILD_ref(idf,:)+ILD_increase; %compression_factor*meanmag + varmag;
HRTF_modmag_part=HRTF_mag_part; % Initiate the modified HRTF magnitude
HRTF_modmag_part(idf,1)=HRTF_modmag_part(idf,1); % left HRTF remained unchanged
HRTF_modmag_part(idf,2)=HRTF_modmag_part(idf,1)-modILD_mag(idf,:); % right HRTF spectra change with increased ILD
yRandPhase = ifftreal(10.^(HRTF_modmag_part./20),Nfft);
YminPhase = RB_minphase(yRandPhase,1,'freq');
y = ifft(YminPhase.*excessPhaseTF,Nfft);
modified_hrir=y;
end
function modified_hrir=fun_ipsi_compress(hrir_part,fs,compression_factor)
Nfft=length(hrir_part);
HRTF_part=fftreal(hrir_part);
HRTF_mag_part=db(abs(HRTF_part));
[~,excessPhaseTF] = RB_minphase(hrir_part,1,'freq');
ILD_ref=HRTF_mag_part(:,1)-HRTF_mag_part(:,2); % reference ILD
if (compression_factor==0)
modified_hrir(:,1) = sig_hassager2016(hrir_part(:,1),0.001,fs); % smoothing process according to Hassager et al. 2016
else
modified_hrir(:,1) = sig_hassager2016(hrir_part(:,1),compression_factor,fs);
end
mag_right = db(abs(fftreal(modified_hrir(:,1))))-ILD_ref;
yRandPhase = ifftreal(10.^(mag_right./20),Nfft);
YminPhase = RB_minphase(yRandPhase,1,'freq');
modified_hrir(:,2) = ifft(YminPhase.*excessPhaseTF(:,2),Nfft);
end
function [modified_ipsi_hrir, modified_contra_hrir]=fun_ILD_compress(hrir_part,fs,compression_factor,f_low,f_high)
Nfft=length(hrir_part);
HRTF_part=fftreal(hrir_part,Nfft);
HRTF_mag_part=db(abs(HRTF_part));
[~,excessPhaseTF] = RB_minphase(hrir_part,1,'freq');
ILD_ref=HRTF_mag_part(:,1)-HRTF_mag_part(:,2); % reference ILD
freq = 0:fs/Nfft:fs/2;
idf = freq >= f_low-1 & freq <= f_high+1; % indices for dedicated frequency range
idwf = idf(:) | circshift(idf(:),[1,0]); % include one neighbouring position for evaluation of frequency weighting
wf = diff(freqtoerb(freq(idwf))); % frequency weighting according to differentiated ERB scale
wf = wf(:)/sum(wf);
mag = ILD_ref(idf,:); % HRTF magnitudes in dB
meanmag = sum(wf.*mag,1);
varmag = mag - meanmag;
modmag = ILD_ref;
modmag(idf,:)= meanmag + compression_factor*varmag;
HRTF_modmag_part_contra=HRTF_mag_part;
HRTF_modmag_part_ipsi=HRTF_mag_part;
HRTF_modmag_part_contra(idf,1)=HRTF_modmag_part_contra(idf,1);
HRTF_modmag_part_contra(idf,2)=HRTF_modmag_part_contra(idf,1)-modmag(idf,:);
HRTF_modmag_part_ipsi(idf,2)=HRTF_modmag_part_ipsi(idf,2);
HRTF_modmag_part_ipsi(idf,1)=HRTF_modmag_part_ipsi(idf,2)+modmag(idf,:);
yRandPhase = ifftreal(10.^(HRTF_modmag_part_contra./20),Nfft);
YminPhase = RB_minphase(yRandPhase,1,'freq');
modified_contra_hrir = ifft(YminPhase.*excessPhaseTF,Nfft);
yRandPhase = ifftreal(10.^(HRTF_modmag_part_ipsi./20),Nfft);
YminPhase = RB_minphase(yRandPhase,1,'freq');
modified_ipsi_hrir = ifft(YminPhase.*excessPhaseTF,Nfft);
end
function [minPhase,excessPhase] = RB_minphase(IR,dim,TFdomainFlag)
% RB_minphase - create minimum-phase filter via causal cepstrum
%
% Usage: [minPhase,excessPhase] = RB_minphase(IR,dim,TFdomainFlag)
% amt toolbox
% RB, 2016/6/3
Nfft = 2.^nextpow2(size(IR,dim));
TF = fft(IR,Nfft,dim);
logTF = log(abs(TF)+eps);
cep = ifft(logTF,Nfft,dim);
Nshift = mod(dim-1,ndims(cep));
cep1 = shiftdim(cep,Nshift);
cep1(Nfft/2+2:Nfft,:,:,:,:) = 0; % set non-causal part to zero and
cep1(2:Nfft/2,:,:,:,:) = 2*cep1(2:Nfft/2,:,:,:,:); % multiply causal part by 2 (due to symmetry)
cepMinPhase = shiftdim(cep1,ndims(cep)-Nshift);
logTFminPhase = fft(cepMinPhase,Nfft,dim);
TFminPhase = exp(logTFminPhase);
switch TFdomainFlag
case 'freq'
minPhase = TFminPhase;
case 'time'
minPhase = ifft(TFminPhase,Nfft,dim);
end
if nargout == 2
switch TFdomainFlag
case 'freq'
excessPhase = TF./TFminPhase;
case 'time'
excessPhase = ifft(TF./TFminPhase,Nfft,dim);
end
end
end