I am having some trouble estimating the parameter for the log-linear realized Garch(1,1) model. The parameter values which I get from the optimisation are different from those derived in the paper and I'm not sure where I am going wrong. Any help would be great. The specification of the model from (Hansen et al. (2012)) is:
Realized GARCH specification
And the likelihood function is given by:
Log Likelihood
I am using the same data as used by Hansen and co-authors which can retrieved from the rugarch package with the command data(spyreal).
My matlab code is
function output = loglikRV(param, data)
r = data.SPY_OC;
RV = data.SPY_RK;
logRV = log(RV);
T = numel(RV); % time sample size
alpha0 = param(1);
alpha1 = param(2);
alpha2 = param(3);
omega0 = param(4);
omega1 = param(5);
omega2 = param(6);
omega3 = param(7);
sigmamu2 = param(8);
z = zeros(T,1);
logh = zeros(T,1);
u = zeros(T,1);
llhs = zeros(T,1);
logh(1) = 8.8296e-05;
u(1) = 0.005;
z(1) = 0.005;
llhs(1) = 0.005;
for i = 2:T
logh(i) = alpha0 + alpha1*logh(i-1) + alpha2*logRV(i-1);
z(i) = r(i) / sqrt(exp(logh(i)));
u(i) = logRV(i) - omega0 - omega1*logh(i) - omega2*z(i) - omega3*(z(i)^2 - 1);
llhs(i) = -(1/2)*(log(2*pi) + logh(i) + z(i)^2) - (1/2)*(log(2*pi) + log(sigmamu2) + u(1)^2 / sigmamu2);
end
output = sum(llhs(2:T-1));
return
And I am optimising this using the Matlab fmincon function with the code as shown below:
clear;close all;
RVfinal = readtable('spyreal.xlsx');
objfun = #(param)(-loglikRV(param,RVfinal)); % negative of the log-likelihood function
param0 = [0.07048753,0.43272574,0.52944743,-0.19368728,1.02540217,-0.06100213, 0.07437231, 0.38];
% constraints in the optimization
A = []; b = []; % no inequality constraints
Aeq=[]; beq=[]; % no equality constraints
% -- MLE Optimization using "fmincon" --
optim_options = optimset('Display','off','TolX',1e-4,'TolFun',1e-4);
[mymle,fval] = fmincon(objfun,param0,A,b,Aeq,beq,[],[],[],optim_options);
mymle
Thank You!
Related
I want to solve coupled partial differential equations of first order, which are of stiff nature. I have coded in MATLAB to solve this pde's, I have used Method of line to convert PDE into ODE, and i have used beam and warmings(second order upwind) method to discritize the spatial derivative. The discretization method is total variation diminishing(TVD) to eliminate the oscillation. But rather using TVD and ode15s solver to integrate resultant stiff ode's the resultant plot is oscillatory(not smooth). What should i do to eliminate this oscillation and get correct results.
I have attached my MATLAB code.. please see it and suggest some improvement.
∂y(1)/∂t=-0.1 ∂y(1)/∂x + (0.5*e^(15*(y(2)⁄(1+y(2))))*(1- y(1))
∂y(2)/∂t=-0.1 ∂y(2)/∂x - (0.4*e^(15*(y(2)⁄(1+y(2))))*(1- y(1))-0.4
Initial condition: at t = 0 y(1)= y(2)=0
Boundary condition: y(1)= y(2) = 0 at x=0
I have attached my MATLAB code.. please see it and suggest some improvement.
function brussode(N)
if nargin<1
N = 149;
end
tspan = [0 10];
m = 0.00035
t = (1:N)/(N+1)*m;
y0 = [repmat(0,1,N); repmat(0,1,N)];
p = 0.5
q = 0.4
options = odeset('Vectorized','on','JPattern',jpattern(N));
[t,y] = ode15s(#f,tspan,y0,options);
a = size(y,2)
u = y(:,1:2:end);
x = (1:N)/(N+1);
figure;
%surf(x,t(end,:),u);
plot(x,u(end,:))
xlabel('space');
ylabel('solution');
zlabel('solution u');
%--------------------------------------------------------------
%Nested function -- N is provided by the outer function.
%
function dydt = f(t,y)
%Derivative function
dydt = zeros(2*N,size(y,2)); %preallocate dy/dt
x = (1:N)/(N+1);
% Evaluate the 2 components of the function at one edge of the grid
% (with edge conditions).
i = 1;
%y(1,:) = 0;
%y(2,:) = 0;
dydt(i,:) = -0.1*(N+1)*(y(i+2,:)-0)+ (0.01/2)*m*((N+1).^3)*(y(i+2,:)-0) + p*exp(15*(0/(1+0)))*(1-0);
dydt(i+1,:) = -0.1*(N+1)*(y(i+3,:)-0)+ (0.01/2)*m*((N+1).^3)*(y(i+3,:)-0) - q*exp(15*(0/(1+0)))*(1-0)+0.25;
i = 3;
%y(1,:) = 0;
%y(2,:) = 0;
dydt(i,:) = -0.1*(N+1)*(y(i+2,:)-y(i,:)) + (0.01/2)*m*((N+1).^3)*(y(i+3,:)-y(i,:)) + p*exp(15*(y(i+1,:)/(1+y(i+1,:))))*(1-y(i,:));
dydt(i+1,:) = -0.1*(N+1)*(y(i+3,:)-y(i+1,:)) + (0.01/2)*m*((N+1).^3)*(y(i+3,:)-y(i,:)) - q*exp(15*(y(i+1,:)/(1+y(i+1,:))))*(1-y(i,:))+0.25;
%Evaluate the 2 components of the function at all interior grid
%points.
i = 5:2:2*N;
%y(1,:) = 0;
% y(2,:) = 0;
dydt(i,:) = (-0.1/2)*(N+1)*(3*y(i,:)-4*y(i-2,:)+y(i-4,:)) +(0.01/2)*m*((N+1).^3)*(y(i,:)-2*y(i-2,:)+y(i-4,:))+ p*exp(15*(y(i+1,:)/(1+y(i+1,:))))*(1-y(i,:));
dydt(i+1,:) = (-0.1/2)*(N+1)*(3*y(i+1,:)-4*y(i-1,:)+y(i-3,:))+(0.01/2)*m*((N+1).^3)*(y(i+1,:)-2*y(i-1,:)+y(i-3,:)) - q*exp(15*(y(i+1,:)/(1+y(i+1,:))))*(1-y(i,:))+0.25;
end
%-------------------------------------------------------------
end %brussode
%-------------------------------------------------------------
% Subfunction -- the sparsity pattern
%
function S = jpattern(N)
% Jacobian sparsity patter
B = ones(2*N,5);
B(2:2:2*N,2) = zeros(N,1);
B(1:2:2*N-1,4) = zeros(N,1);
S = spdiags(B,-2:2,2*N,2*N);
end
%-------------------------------------------------------------
I've programmed in MATLAB an adaptive step size RK4 to solve a system of ODEs. The code runs without error, however it does not produce the desired curve when I try to plot x against y. Instead of being a toroidal shape, I simply get a flat line. This is evident from the fact that r is outputting a constant value. After checking the outputs of each line, they are not outputting constants or errors or inf or NaN, rather they are outputting both a real and imaginary component (complex numbers). I have no idea as to why this is occurring and I believe it to be the source of my trouble.
function AdaptRK4()
parsec = 3.08*10^18;
r_1 = 8.5*1000.0*parsec; % in cm
theta_1 = 0.0;
a = 0.5*r_1;
gam = 1;
grav = 6.6720*10^-8;
amsun = 1.989*10^33;
amg = 1.5d11*amsun;
gm = grav*amg;
u_1 = 20.0*10^5;
v = sqrt(gm/r_1);
time = 0.0;
epsilon = 0.00001;
m1 = 0.5;
m2 = 0.5;
m3 = 0.5;
i = 1;
nsteps = 50000;
deltat = 5.0*10^12;
angmom = r_1*v;
angmom2 = angmom^2.0;
e = -2*10^5.0*gm/r_1+u_1*u_1/2.0+angmom2/(2.0*r_1*r_1);
for i=1:nsteps
deltat = min(deltat,nsteps-time);
fk3_1 = deltat*u_1;
fk4_1 = deltat*(-gm*r_1*r_1^(-gam)/(a+r_1)^(3- gam)+angmom2/(r_1^3.0));
fk5_1 = deltat*(angmom/(r_1^2.0));
r_2 = r_1+fk3_1/4.0;
u_2 = u_1+fk4_1/4.0;
theta_2 = theta_1+fk5_1/4.0;
fk3_2 = deltat*u_2;
fk4_2 = deltat*(-gm*r_2*r_2^(-gam)/(a+r_2)^(3-gam)+angmom2/(r_2^3.0));
fk5_2 = deltat*(angmom/(r_2^2.0));
r_3 = r_1+(3/32)*fk3_1 + (9/32)*fk3_2;
u_3 = u_1+(3/32)*fk4_1 + (9/32)*fk4_2;
theta_3 = theta_1+(3/32)*fk5_1 + (9/32)*fk5_2;
fk3_3 = deltat*u_3;
fk4_3 = deltat*(-gm*r_3*r_3^(-gam)/(a+r_3)^(3-gam)+angmom2/(r_3^3.0));
fk5_3 = deltat*(angmom/(r_3^2.0));
r_4 = r_1+(1932/2197)*fk3_1 - (7200/2197)*fk3_2 + (7296/2197)*fk3_3;
u_4 = u_1+(1932/2197)*fk4_1 - (7200/2197)*fk4_2 + (7296/2197)*fk4_3;
theta_4 = theta_1+(1932/2197)*fk5_1 - (7200/2197)*fk5_2 + (7296/2197)*fk5_3;
fk3_4 = deltat*u_4;
fk4_4 = deltat*(-gm*r_4*r_4^(-gam)/(a+r_4)^(3-gam)+angmom2/(r_4^3.0));
fk5_4 = deltat*(angmom/(r_4^2.0));
r_5 = r_1+(439/216)*fk3_1 - 8*fk3_2 + (3680/513)*fk3_3 - (845/4104)*fk3_4;
u_5 = u_1+(439/216)*fk4_1 - 8*fk4_2 + (3680/513)*fk4_3 - (845/4104)*fk4_4;
theta_5 = theta_1+(439/216)*fk5_1 - 8*fk5_2 + (3680/513)*fk5_3 - (845/4104)*fk5_4;
fk3_5 = deltat*u_5;
fk4_5 = deltat*(-gm*r_5*r_5^(-gam)/(a+r_5)^(3-gam)+angmom2/(r_5^3.0));
fk5_5 = deltat*(angmom/(r_5^2.0));
r_6 = r_1-(8/27)*fk3_1 - 2*fk3_2 - (3544/2565)*fk3_3 + (1859/4104)*fk3_4-(11/40)*fk3_5;
u_6 = u_1-(8/27)*fk4_1 - 2*fk4_2 - (3544/2565)*fk4_3 + (1859/4104)*fk4_4-(11/40)*fk4_5;
theta_6 = theta_1-(8/27)*fk5_1 - 2*fk5_2 - (3544/2565)*fk5_3 + (1859/4104)*fk5_4-(11/40)*fk5_5;
fk3_6 = deltat*u_6;
fk4_6 = deltat*(-gm*r_6*r_6^(-gam)/(a+r_6)^(3-gam)+angmom2/(r_6^3.0));
fk5_6 = deltat*(angmom/(r_6^2.0));
fm3_1 = m1 + 25*fk3_1/216+1408*fk3_3/2565+2197*fk3_4/4104-fk3_5/5;
fm4_1 = m2 + 25*fk4_1/216+1408*fk4_3/2565+2197*fk4_4/4104-fk4_5/5;
fm5_1 = m3 + 25*fk5_1/216+1408*fk5_3/2565+2197*fk5_4/4104-fk5_5/5;
fm3_2 = m1 + 16*fk3_1/135+6656*fk3_3/12825+28561*fk3_4/56430-9*fk3_5/50+2*fk3_6/55;
fm4_2 = m2 + 16*fk4_1/135+6656*fk4_3/12825+28561*fk4_4/56430-9*fk4_5/50+2*fk4_6/55;
fm5_2 = m3 + 16*fk5_1/135+6656*fk5_3/12825+28561*fk5_4/56430-9*fk5_5/50+2*fk5_6/55;
R3 = abs(fm3_1-fm3_2)/deltat;
R4 = abs(fm4_1-fm4_2)/deltat;
R5 = abs(fm5_1-fm5_2)/deltat;
err3 = 0.84*(epsilon/R3)^(1/4);
err4 = 0.84*(epsilon/R4)^(1/4);
err5 = 0.84*(epsilon/R5)^(1/4);
if R3<= epsilon
time = time+deltat;
fm3 = fm3_1;
i = i+1;
deltat = err3*deltat;
end
if R4<= epsilon
time = time+deltat;
fm4 = fm4_1;
i = i+1;
deltat = err4*deltat;
end
if R5<= epsilon
time = time+deltat;
fm5 = fm5_1;
i = i+1;
deltat = err5*deltat;
end
e=2*gm^2.0/(2*angmom2);
ecc=(1.0+(2.0*e*angmom2)/(gm^2.0))^0.5;
x(i)=r_1*cos(theta_1)/(1000.0*parsec);
y(i)=r_1*sin(theta_1)/(1000.0*parsec);
time=time+deltat;
r(i)=r_1;
time1(i)=time;
end
figure()
plot(x,y, '-k');
TeXString = title('Plot of Orbit in Gamma Potential Obtained Using RK4')
xlabel('x')
ylabel('y')
You are getting complex values because at some point npts - time < 0. You may want to print out the values of deltat to check the error.
Also, your code doesn't seem to take into account the case when the error estimate is larger than your tolerance. When your error estimate is greater than your tolerance you have to:
Shift back the time AND solution
calculate a new step-size based on a formula, and
recalculate your solution and error estimate.
The fact that you don't know how many iterations you will have to go through makes the use of a for-loop for adaptive runge Kutta a bit awkward. I suggest using a while loop instead.
You are using "i" in your code. "i" returns the basic imaginary unit. "i" is equivalent to sqrt(-1). Try to use another identifier in your loops and only use "i" or "j" in calculations where complex numbers are involved.
I have written a Matlab code which is a simulation of NOT gate implementation using ring lasers. Si variable is input in my code. But my code works only for Si = 0. for any other non zero value it doesn't show output.
%-----------Rate Equation MATLAB code ---------
function dydt = requations(t,y)
dydt = zeros(size(y));
%prompt = 'Sinput???';
%Si = input(prompt);
Si = 0; %MY INPUT
q = 1.6e-19; % charge of electron
tau_e = 1e-9; % carrier lifetime
No = 3.3e18; % # No of carriers at transparency
a = 1e-15; % Linear gain coefficient
Vg = 7.5e9; % group velocity
Vp = 3e-11; %Photon reservoir volume
V = 1e-11; %Carrier reservoir Volume
tau_p = 1.7e-12; % photon lifetime
beta = 1e-5; % spontateous emission coefficient
eps = 7.5e-17; % Nonlinear gain suppression coefficient
Ni = 0.8; %Internal quantum efficiency
w = 2*pi*10e5;
Io = 10e-3;
%I = Io*sin(w*t);
I = 2.5*Io; %for test purposes
tp = 1/tau_p;
te = 1/tau_e;
Aint = 6; %Internal losses inside cavity waveguides
%G = ((a/Vp)* (N-(V*No)))/(1-eps*(Sc + Scc));
alpha = -2; %alpha factor
L = 76e-4 ;%size of the ring
wcb = 2*pi*70;
%R = 0.25;
Wcb = wcb*1000000;
%r = 1/R;
tpcw = Vg*(Aint + ((1/L)*log(4)));
Tpcw = 1/tpcw;
%------Rate equations-------
N = y(1);
Sc = y(2); %Clock wise photon number
yc = y(3);
Scc = y(4); %anti clockwise photon number
ycc = y(5);
G = ((a/Vp)* (N-(V*No)))/(1-eps*(Sc + Scc));
dydt(1) = (Ni*I)/q - y(1)*te - Vg*G*(y(2) + y(4)); %dN/dt
dydt(2) = (Vg*G-Tpcw)*y(2) + beta*y(1)*te; %dSc/dt
dydt(3) = -(alpha/2)*(Vg*G-Tpcw); %dyc/dt
dydt(4) = (Vg*G-Tpcw)*y(4) + beta*y(1)*te + ((2*Vg)/L)*cos(y(5))*(sqrt(Si*y(4))); %dScc/dt
dydt(5) = -Wcb - ((alpha/2)*(Vg*G-Tpcw)) - ((Vg/L)*sin(y(5))*(sqrt(Si/y(4)))); %dycc/dt
Below is the Ode file
%------Rate equations for requation file------
format bank;
close all;
clear all;
clc;
%time interval
ti=0;
tf=200;
tspan=[ti tf];
x0 = [3.75e7, 2.25e6, 0, 2.25e6, 0]; %initial vectors
%options= odeset('RelTol',100, 'AbsTol',[3.75e7, 2.25e6]);
[t,y]= ode23t(#requations,tspan,x0);
%Plotting the graphs:
figure
subplot(5,1,1), plot(t,y(:,1),'r'),grid on;
title('Laserrate equations'),ylabel('N');
subplot(5,1,2), plot(t,y(:,2),'b'),grid on;
ylabel('Scw'); xlabel('t');
subplot(5,1,3), plot(t,y(:,3),'g'),grid on;
ylabel('ycw');xlabel('t');
subplot(5,1,4), plot(t,y(:,3),'g'),grid on;
ylabel('Sccw');xlabel('t');
subplot(5,1,5), plot(t,y(:,3),'g'),grid on;
ylabel('yccw');xlabel('t');
I run this code in matlab to minimize the parameters of my function real_egarchpartial with fminsearch:
data = xlsread('return_cc_in.xlsx');
SPY = data(:,25);
dailyrange = xlsread('DR_in.xlsx');
drSPY= dailyrange(:,28);
startingVals = [mean(SPY); 0.041246; 0.70121; 0.05; 0.04; 0.45068; -0.1799; 1.0375; 0.06781; 0.070518];
T = size(SPY,1);
options = optimset('fminsearch');
options.Display = 'iter';
estimates = fminsearch(#real_egarchpartial, startingVals, options, SPY, drSPY);
[ll, lls, u]=real_egarchpartial(estimates, SPY, drSPY);
And I get this message:
Exiting: Maximum number of function evaluations has been exceeded
- increase MaxFunEvals option.
I put the original starting values. So I assumed they are corrects. I used fminsearch and not fmincon because my function hasn't constraints and with fminunc my function gets a lot of red messages.
the real_egarchpartial function is the following:
function [ll,lls,lh] = real_egarchpartial(parameters, data, x_rk)
mu = parameters(1);
omega = parameters(2);
beta = parameters(3);
tau1 = parameters(4);
tau2 = parameters(5);
gamma = parameters(6);
csi = parameters(7);
phi = parameters(8);
delta1 = parameters(9);
delta2 = parameters(10);
%Data and h are T by 1 vectors
T = size(data,1);
eps = data-mu;
lh = zeros(T,1);
h = zeros(T,1);
u = zeros(T,1);
%Must use a back Cast to start the algorithm
h(1)=var(data);
lh(1) = log(h(1));
z= eps/sqrt(h(1));
u(1) = rand(1);
lxRK = log(x_rk);
for t = 2:T;
lh(t) = omega + beta*lh(t-1) + tau1*z(t-1) + tau2*((z(t-1).^2)-1)+ gamma*u(t-1);
h(t)=exp(lh(t));
z = eps/sqrt(h(t));
end
for t = 2:T
u(t)= lxRK(t) - csi - phi*h(t) - delta1*z(t) - delta2*((z(t).^2)-1);
end
lls = 0.5*(log(2*pi) + lh + eps.^2./h);
ll = sum(lls);
Could someone explain what is wrong? Is there another function more efficient for my estimation? Any help will be appreciated! Thank you.
A filter g is called separable if it can be expressed as the multiplication of two vectors grow and gcol . Employing one dimensional filters decreases the two dimensional filter's computational complexity from O(M^2 N^2) to O(2M N^2) where M and N are the width (and height) of the filter mask and the image respectively.
In this stackoverflow link, I wrote the equation of a Gabor filter in the spatial domain, then I wrote a matlab code which serves to create 64 gabor features.
According to the definition of separable filters, the Gabor filters are parallel to the image axes - theta = k*pi/2 where k=0,1,2,etc.. So if theta=pi/2 ==> the equation in this stackoverflow link can be rewritten as:
The equation above is extracted from this article.
Note: theta can be extented to be equal k*pi/4. By comparing to the equation in this stackoverflow link, we can consider that f= 1 / lambda.
By changing my previous code in this stackoverflow link, I wrote a matlab code to make the Gabor filters separable by using the equation above, but I am sure that my code below is not correct especially when I initialized the gbp and glp equations. That is why I need your help. I will appreciate your help very much.
Let's show now my code:
function [fSiz,filters1,filters2,c1OL,numSimpleFilters] = init_gabor(rot, RF_siz)
image=imread('xxx.jpg');
image_gray=rgb2gray(image);
image_gray=imresize(image_gray, [100 100]);
image_double=double(image_gray);
rot = [0 45 90 135]; % we have four orientations
RF_siz = [7:2:37]; %we get 16 scales (7x7 to 37x37 in steps of two pixels)
minFS = 7; % the minimum receptive field
maxFS = 37; % the maximum receptive field
sigma = 0.0036*RF_siz.^2 + 0.35*RF_siz + 0.18; %define the equation of effective width
lambda = sigma/0.8; % it the equation of wavelength (lambda)
G = 0.3; % spatial aspect ratio: 0.23 < gamma < 0.92
numFilterSizes = length(RF_siz); % we get 16
numSimpleFilters = length(rot); % we get 4
numFilters = numFilterSizes*numSimpleFilters; % we get 16x4 = 64 filters
fSiz = zeros(numFilters,1); % It is a vector of size numFilters where each cell contains the size of the filter (7,7,7,7,9,9,9,9,11,11,11,11,......,37,37,37,37)
filters1 = zeros(max(RF_siz),numFilters);
filters2 = zeros(numFilters,max(RF_siz));
for k = 1:numFilterSizes
for r = 1:numSimpleFilters
theta = rot(r)*pi/180;
filtSize = RF_siz(k);
center = ceil(filtSize/2);
filtSizeL = center-1;
filtSizeR = filtSize-filtSizeL-1;
sigmaq = sigma(k)^2;
for x = -filtSizeL:filtSizeR
fx = exp(-(x^2)/(2*sigmaq))*cos(2*pi*x/lambda(k));
f1(x+center,1) = fx;
end
for y = -filtSizeL:filtSizeR
gy = exp(-(y^2)/(2*sigmaq));
f2(1,y+center) = gy;
end
f1 = f1 - mean(mean(f1));
f1 = f1 ./ sqrt(sum(sum(f1.^2)));
f2 = f2 - mean(mean(f2));
f2 = f2 ./ sqrt(sum(sum(f2.^2)));
p = numSimpleFilters*(k-1) + r;
filters1(1:filtSize,p)=f1;
filters2(p,1:filtSize)=f2;
convv1=imfilter(image_double, filters1(1:filtSize,p),'conv');
convv2=imfilter(double(convv1), filters2(p,1:filtSize),'conv');
figure
imagesc(convv2);
colormap(gray);
end
end
I think the code is correct provided your previous version of Gabor filter code is correct too. The only thing is that if theta = k * pi/4;, your formula here should be separated to:
fx = exp(-(x^2)/(2*sigmaq))*cos(2*pi*x/lambda(k));
gy = exp(-(G^2 * y^2)/(2*sigmaq));
To be consistent, you may use
f1(1,x+center) = fx;
f2(y+center,1) = gy;
or keep f1 and f2 as it is but transpose your filters1 and filters2 thereafter.
Everything else looks good to me.
EDIT
My answer above works for theta = k * pi/4;, with other angles, based on your paper,
x = i*cos(theta) - j*sin(theta);
y = i*sin(theta) + j*cos(theta);
fx = exp(-(x^2)/(2*sigmaq))*exp(sqrt(-1)*x*cos(theta));
gy = exp(-(G^2 * y^2)/(2*sigmaq))*exp(sqrt(-1)*y*sin(theta));
The final code will be:
function [fSiz,filters1,filters2,c1OL,numSimpleFilters] = init_gabor(rot, RF_siz)
image=imread('xxx.jpg');
image_gray=rgb2gray(image);
image_gray=imresize(image_gray, [100 100]);
image_double=double(image_gray);
rot = [0 45 90 135];
RF_siz = [7:2:37];
minFS = 7;
maxFS = 37;
sigma = 0.0036*RF_siz.^2 + 0.35*RF_siz + 0.18;
lambda = sigma/0.8;
G = 0.3;
numFilterSizes = length(RF_siz);
numSimpleFilters = length(rot);
numFilters = numFilterSizes*numSimpleFilters;
fSiz = zeros(numFilters,1);
filters1 = zeros(max(RF_siz),numFilters);
filters2 = zeros(numFilters,max(RF_siz));
for k = 1:numFilterSizes
for r = 1:numSimpleFilters
theta = rot(r)*pi/180;
filtSize = RF_siz(k);
center = ceil(filtSize/2);
filtSizeL = center-1;
filtSizeR = filtSize-filtSizeL-1;
sigmaq = sigma(k)^2;
for x = -filtSizeL:filtSizeR
fx = exp(-(x^2)/(2*sigmaq))*exp(sqrt(-1)*x*cos(theta));
f1(1, x+center) = fx;
end
for y = -filtSizeL:filtSizeR
gy=exp(-(y^2)/(2*sigmaq))*exp(sqrt(-1)*y*sin(theta));
f2(y+center,1) = gy;
end
f1 = f1 - mean(mean(f1));
f1 = f1 ./ sqrt(sum(sum(f1.^2)));
f2 = f2 - mean(mean(f2));
f2 = f2 ./ sqrt(sum(sum(f2.^2)));
p = numSimpleFilters*(k-1) + r;
filters1(1:filtSize,p)=f1;
filters2(p,1:filtSize)=f2;
convv1=imfilter(image_double, filters1(1:filtSize,p),'conv');
convv2=imfilter(double(convv1), filters2(p,1:filtSize),'conv');
figure
imagesc(imag(convv2));
colormap(gray);
end
end