文件名称:demo_nnls

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  • matlab例程
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  • [Matlab] [源码]
  • 上传时间:
  • 2012-11-26
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  • 639kb
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  • 0次
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  • w***
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PLS - DN是一个有限的牛顿为解决非退化的分段线性系统的算法。 PLS - DN的展品可证明半迭代

财产即在全球范围内的精确解在有限数量的迭代算法收敛。被证明是收敛速度

至少前终止线性。



广泛的算法是在我们的AISTATS 2011纸描述:“一个非退化的分段线性系统的有限牛顿算法”。此演示包重新运行

在解决非负最小二乘法(NNLS)问题上的三个稀疏的设计矩阵,从哈威尔波音收集(达夫等人,1989年)第4.2节的实验。



随着PLS - DN,此演示包建议实施五

其他NNLS求解:LCP_Fisher_Newton,LCP_Lemke,PQN,TRESNEI,和SCD

-PLS- DN is a finite non-degenerate Newton to solve the piecewise linear system algorithms. PLS- DN exhibits semi-iterative property to prove that the exact solutions worldwide in a limited number of iterative convergence. Proved to be terminated before the linear convergence rate at least. A wide range of algorithms in our AISTATS 2011 paper describes: " a non-degenerate sub-linear systems with limited Newton algorithm." This demo package to re-run in the settlement of non-negative least squares (NNLS) on the design of the three sparse matrices from the Harwell Boeing collection (Duff et al, 1989) Section 4.2 of the experiment. With PLS- DN, this demonstrates the implementation of five other NNLS package proposed solution: LCP_Fisher_Newton, LCP_Lemke, PQN, TRESNEI, and SCD
相关搜索: nnls

(系统自动生成,下载前可以参看下载内容)

下载文件列表

demo_nnls\algorithms\LCP_Fischer_Newton\source code\LCP.m

.........\..........\..................\...........\license.txt

.........\..........\..................\...........\Test_add20.asv

.........\..........\..................\...........\Test_add20.m

.........\..........\..................\...........\Test_illc1850.m

.........\..........\..................\...........\Test_well1850.m

.........\..........\....Lemke_method\source code\lemke.m

.........\..........\................\...........\lemke_prb.m

.........\..........\................\...........\lemke_prb_output.txt

.........\..........\................\...........\Test_add20.m

.........\..........\................\...........\Test_illc1850.m

.........\..........\................\...........\Test_well1850.m

.........\..........\PLS_DN\source code\NNLSR_PLS_DN.m

.........\..........\......\...........\PLS_DN_Solver.m

.........\..........\......\...........\SquaredErrorlasso.m

.........\..........\......\...........\Test_add20.m

.........\..........\......\...........\Test_illc1850.m

.........\..........\......\...........\Test_well1850.m

.........\..........\.QN\schmidt09a.pdf

.........\..........\...\.ource code\isLegal.m

.........\..........\...\...........\lbfgsC.c

.........\..........\...\...........\lbfgsHvFunc2.m

.........\..........\...\...........\lbfgsUpdate.m

.........\..........\...\...........\minConF_PQN.m

.........\..........\...\...........\minConF_SPG.m

.........\..........\...\...........\myProcessOptions.m

.........\..........\...\...........\polyinterp.m

.........\..........\...\...........\projectHalfSpace.m

.........\..........\...\...........\SquaredError.m

.........\..........\...\...........\Test_add20.m

.........\..........\...\...........\Test_illc1850.m

.........\..........\...\...........\Test_well1850.m

.........\..........\SCD\source code\SCD.m

.........\..........\...\...........\Test_add20.m

.........\..........\...\...........\Test_illc1850.m

.........\..........\...\...........\Test_well1850.m

.........\..........\TRESNEI\source code\SquaredError.m

.........\..........\.......\...........\SSquaredError.m

.........\..........\.......\...........\Test_add20.m

.........\..........\.......\...........\Test_illc1850.m

.........\..........\.......\...........\Test_well1850.m

.........\..........\.......\...........\TRESNEI.m

.........\data\data_add20.mat

.........\....\data_illc1850.mat

.........\....\data_well1850.mat

.........\.emo_script\exp_nnls.m

.........\...........\plot_draw_add20\finalPlot1.eps

.........\...........\...............\Plot_Draw_add20.m

.........\...........\...............\prettyPlot.m

.........\...........\...............\runningMin.m

.........\...........\..........illc1850\finalPlot1.eps

.........\...........\..................\Plot_Draw_illc1850.m

.........\...........\..................\prettyPlot.m

.........\...........\..................\runningMin.m

.........\...........\..........well1850\finalPlot1.eps

.........\...........\..................\LCP.m

.........\...........\..................\Plot_Draw_well1850.m

.........\...........\..................\prettyPlot.m

.........\...........\..................\runningMin.m

.........\README.txt

.........\result\LCP_Fischer_Result_add20.mat

.........\......\LCP_Fischer_Result_illc1850.mat

.........\......\LCP_Fischer_Result_well1850.mat

.........\......\LCP_Lemke_Result_add20.mat

.........\......\LCP_Lemke_Result_illc1850.mat

.........\......\LCP_Lemke_Result_well1850.mat

.........\......\PLS_Result_add20.mat

.........\......\PLS_Result_illc1850.mat

.........\......\PLS_Result_well1850.mat

.........\......\PQN_Result_add20.mat

.........\......\PQN_Result_illc1850.mat

.........\......\PQN_Result_well1850.mat

.........\......\SCD_Result_add20.mat

.........\......\SCD_Result_illc1850.mat

.........\......\SCD_Result_well1850.mat

.........\......\TRESNEI_Result_add20.mat

.........\......\TRESNEI_Result_illc1850.mat

.........\......\TRESNEI_Result_well1850.mat

.........\algorithms\LCP_Fischer_Newton\source code

.........\..........\....Lemke_method\source code

.........

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