今天为大家带来混合高斯模型的EM推导求解过程。
全部代码如下!
def NDimensionGaussian(X_vector,U_Mean,CovarianceMatrix): #X=numpy.mat(X_vector) X=X_vector D=numpy.shape(X)[0] #U=numpy.mat(U_Mean) U=U_Mean #CM=numpy.mat(CovarianceMatrix) CM=CovarianceMatrix Y=X-U temp=Y.transpose() * CM.I * Y result=(1.0/((2*numpy.pi)**(D/2)))*(1.0/(numpy.linalg.det(CM)**0.5))*numpy.exp(-0.5*temp) return result def CalMean(X): D,N=numpy.shape(X) MeanVector=numpy.mat(numpy.zeros((D,1))) for d in range(D): for n in range(N): MeanVector[d,0] += X[d,n] MeanVector[d,0] /= float(N) return MeanVector def CalCovariance(X,MV): D,N=numpy.shape(X) CoV=numpy.mat(numpy.zeros((D,D))) for n in range(N): Temp=X[:,n]-MV CoV += Temp*Temp.transpose() CoV /= float(N) return CoV def CalEnergy(Xn,Pik,Uk,Cov): D,N=numpy.shape(Xn) D_k,K=numpy.shape(Uk) if D!=D_k: print ('dimension not equal, break') return energy=0.0 for n_iter in range(N): temp=0 for k_iter in range(K): temp += Pik[0,k_iter] * NDimensionGaussian(Xn[:,n_iter],Uk[:,k_iter],Cov[k_iter]) energy += numpy.log(temp) return float(energy) def SequentialEMforMixGaussian(InputData,K): #初始化piK pi_Cof=numpy.mat(numpy.ones((1,K))*(1.0/float(K))) X=numpy.mat(InputData) X_mean=CalMean(X) print (X_mean) X_cov=CalCovariance(X,X_mean) print (X_cov) #初始化uK,其中第k列表示第k个高斯函数的均值向量 #X为D维,N个样本点 D,N=numpy.shape(X) print (D,N) UK=numpy.mat(numpy.zeros((D,K))) for d_iter in range(D): for k_iter in range(K): UK[d_iter,k_iter] = X_mean[d_iter,0] + (-1)**k_iter + (-1)**d_iter print (UK) #初始化k个协方差矩阵的列表 List_cov=[] for k_iter in range(K): List_cov.append(numpy.mat(numpy.eye(X[:,0].size))) print (List_cov) List_cov_new=copy.deepcopy(List_cov) rZnk=numpy.mat(numpy.zeros((N,K))) denominator=numpy.mat(numpy.zeros((N,1))) rZnk_new=numpy.mat(numpy.zeros((N,K))) Nk=0.5*numpy.mat(numpy.ones((1,K))) print (Nk) Nk_new=numpy.mat(numpy.zeros((1,K))) UK_new=numpy.mat(numpy.zeros((D,K))) pi_Cof_new=numpy.mat(numpy.zeros((1,K))) for n_iter in range(1,N): #rZnk=pi_k*Gaussian(Xn|uk,Cov_k)/sum(pi_j*Gaussian(Xn|uj,Cov_j)) for k_iter in range(K): rZnk_new[n_iter,k_iter] = pi_Cof[0,k_iter] * NDimensionGaussian(X[:,n_iter],UK[:,k_iter],List_cov[k_iter]) denominator[n_iter,0] += rZnk_new[n_iter,k_iter] for k_iter in range(K): rZnk_new[n_iter,k_iter] /= denominator[n_iter,0] print ('rZnk_new', rZnk_new[n_iter,k_iter],'\n') for k_iter in range(K): Nk_new[0,k_iter] = Nk[0,k_iter] + rZnk_new[n_iter,k_iter] - rZnk[n_iter,k_iter] print ('Nk_new',Nk_new,'\n') ##############当前有(n_iter+1)样本########################### pi_Cof_new[0,k_iter] = Nk_new[0,k_iter]/float(n_iter+1) print ('pi_Cof_new',pi_Cof_new,'\n') UK_new[:,k_iter] = UK[:,k_iter] + ( (rZnk_new[n_iter,k_iter] - rZnk[n_iter,k_iter])/float(Nk_new[0,k_iter]) ) * (X[:,n_iter]-UK[:,k_iter]) print ('UK_new',UK_new,'\n') Temp = X[:,n_iter] - UK_new[:,k_iter] List_cov_new[k_iter] = List_cov[k_iter] + ((rZnk_new[n_iter,k_iter] - rZnk[n_iter,k_iter])/float(Nk_new[0,k_iter]))*(Temp*Temp.transpose()-List_cov[k_iter]) print ('List_cov_new',List_cov_new,'\n') rZnk=copy.deepcopy(rZnk_new) pi_Cof=copy.deepcopy(pi_Cof_new) UK_new=copy.deepcopy(UK) List_cov=copy.deepcopy(List_cov_new) print (pi_Cof,UK_new,List_cov) return pi_Cof,UK_new,List_cov def BatchEMforMixGaussian(InputData,K,MaxIter): #初始化piK pi_Cof=numpy.mat(numpy.ones((1,K))*(1.0/float(K))) X=numpy.mat(InputData) X_mean=CalMean(X) print (X_mean) X_cov=CalCovariance(X,X_mean) print (X_cov) #初始化uK,其中第k列表示第k个高斯函数的均值向量 #X为D维,N个样本点 D,N=numpy.shape(X) print (D,N) UK=numpy.mat(numpy.zeros((D,K))) for d_iter in range(D): for k_iter in range(K): UK[d_iter,k_iter] = X_mean[d_iter,0] + (-1)**k_iter + (-1)**d_iter print (UK) #初始化k个协方差矩阵的列表 List_cov=[] for k_iter in range(K): List_cov.append(numpy.mat(numpy.eye(X[:,0].size))) print (List_cov) energy_new=0 energy_old=CalEnergy(X,pi_Cof,UK,List_cov) print (energy_old) currentIter=0 while True: currentIter += 1 List_cov_new=[] rZnk=numpy.mat(numpy.zeros((N,K))) denominator=numpy.mat(numpy.zeros((N,1))) Nk=numpy.mat(numpy.zeros((1,K))) UK_new=numpy.mat(numpy.zeros((D,K))) pi_new=numpy.mat(numpy.zeros((1,K))) #rZnk=pi_k*Gaussian(Xn|uk,Cov_k)/sum(pi_j*Gaussian(Xn|uj,Cov_j)) for n_iter in range(N): for k_iter in range(K): rZnk[n_iter,k_iter] = pi_Cof[0,k_iter] * NDimensionGaussian(X[:,n_iter],UK[:,k_iter],List_cov[k_iter]) denominator[n_iter,0] += rZnk[n_iter,k_iter] for k_iter in range(K): rZnk[n_iter,k_iter] /= denominator[n_iter,0] #print 'rZnk', rZnk[n_iter,k_iter] #pi_new=sum(rZnk) for k_iter in range(K): for n_iter in range(N): Nk[0,k_iter] += rZnk[n_iter,k_iter] pi_new[0,k_iter] = Nk[0,k_iter]/(float(N)) #print 'pi_k_new',pi_new[0,k_iter] #uk_new= (1/sum(rZnk))*sum(rZnk*Xn) for k_iter in range(K): for n_iter in range(N): UK_new[:,k_iter] += (1.0/float(Nk[0,k_iter]))*rZnk[n_iter,k_iter]*X[:,n_iter] #print 'UK_new',UK_new[:,k_iter] for k_iter in range(K): X_cov_new=numpy.mat(numpy.zeros((D,D))) for n_iter in range(N): Temp = X[:,n_iter] - UK_new[:,k_iter] X_cov_new += (1.0/float(Nk[0,k_iter]))*rZnk[n_iter,k_iter] * Temp * Temp.transpose() #print 'X_cov_new',X_cov_new List_cov_new.append(X_cov_new) energy_new=CalEnergy(X,pi_new,UK_new,List_cov) print ('energy_new',energy_new) #print pi_new #print UK_new #print List_cov_new if energy_old>=energy_new or currentIter>MaxIter: UK=copy.deepcopy(UK_new) pi_Cof=copy.deepcopy(pi_new) List_cov=copy.deepcopy(List_cov_new) break else: UK=copy.deepcopy(UK_new) pi_Cof=copy.deepcopy(pi_new) List_cov=copy.deepcopy(List_cov_new) energy_old=energy_new return pi_Cof,UK,List_cov