Updated regression analysis, sad to come
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@@ -50,7 +50,16 @@ Automatically generated HTML file from DocOnce source
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('Interpretations and optimizing our parameters',
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('Interpretations and optimizing our parameters',
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('The singular value decompostion', 2, None, '___sec7')]}
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@@ -93,6 +102,9 @@ MathJax.Hub.Config({
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<!-- navigation toc: --> <li><a href="._Regression-bs003.html#___sec2" style="font-size: 80%;">Rewriting the fitting procedure as a linear algebra problem</a></li>
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<!-- navigation toc: --> <li><a href="._Regression-bs004.html#___sec3" style="font-size: 80%;">Generalizing the fitting procedure as a linear algebra problem</a></li>
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<!-- navigation toc: --> <li><a href="._Regression-bs005.html#___sec4" style="font-size: 80%;">Optimizing our parameters</a></li>
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<!-- navigation toc: --> <li><a href="._Regression-bs006.html#___sec5" style="font-size: 80%;">Interpretations and optimizing our parameters</a></li>
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||||
<!-- navigation toc: --> <li><a href="._Regression-bs007.html#___sec6" style="font-size: 80%;">Interpretations and optimizing our parameters</a></li>
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||||
<!-- navigation toc: --> <li><a href="._Regression-bs008.html#___sec7" style="font-size: 80%;">The singular value decompostion</a></li>
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</ul>
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</li>
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@@ -127,7 +139,7 @@ MathJax.Hub.Config({
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<center>[2] <b>Department of Physics and Astronomy and National Superconducting Cyclotron Laboratory, Michigan State University</b></center>
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<br>
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<p>
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<center><h4>Oct 14, 2017</h4></center> <!-- date -->
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<center><h4>Oct 17, 2017</h4></center> <!-- date -->
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<br>
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<p>
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@@ -146,6 +158,9 @@ MathJax.Hub.Config({
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<li><a href="._Regression-bs003.html">4</a></li>
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<li><a href="._Regression-bs004.html">5</a></li>
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<li><a href="._Regression-bs005.html">6</a></li>
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<li><a href="._Regression-bs006.html">7</a></li>
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<li><a href="._Regression-bs007.html">8</a></li>
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<li><a href="._Regression-bs008.html">9</a></li>
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<li><a href="._Regression-bs001.html">»</a></li>
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</ul>
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<!-- ------------------- end of main content --------------- -->
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@@ -50,7 +50,16 @@ Automatically generated HTML file from DocOnce source
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2,
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None,
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'___sec3'),
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('Optimizing our parameters', 2, None, '___sec4')]}
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('Optimizing our parameters', 2, None, '___sec4'),
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('Interpretations and optimizing our parameters',
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2,
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None,
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'___sec5'),
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('Interpretations and optimizing our parameters',
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2,
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None,
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'___sec6'),
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('The singular value decompostion', 2, None, '___sec7')]}
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end of tocinfo -->
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<body>
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@@ -65,8 +74,8 @@ MathJax.Hub.Config({
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@@ -93,6 +102,9 @@ MathJax.Hub.Config({
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<!-- navigation toc: --> <li><a href="._Regression-bs003.html#___sec2" style="font-size: 80%;">Rewriting the fitting procedure as a linear algebra problem</a></li>
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<!-- navigation toc: --> <li><a href="._Regression-bs004.html#___sec3" style="font-size: 80%;">Generalizing the fitting procedure as a linear algebra problem</a></li>
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<!-- navigation toc: --> <li><a href="._Regression-bs005.html#___sec4" style="font-size: 80%;">Optimizing our parameters</a></li>
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||||
<!-- navigation toc: --> <li><a href="._Regression-bs006.html#___sec5" style="font-size: 80%;">Interpretations and optimizing our parameters</a></li>
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||||
<!-- navigation toc: --> <li><a href="._Regression-bs007.html#___sec6" style="font-size: 80%;">Interpretations and optimizing our parameters</a></li>
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||||
<!-- navigation toc: --> <li><a href="._Regression-bs008.html#___sec7" style="font-size: 80%;">The singular value decompostion</a></li>
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</ul>
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</li>
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@@ -142,6 +154,9 @@ A regression model aims at finding a likelihood function \( p(y\vert \hat{x}) \)
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<li><a href="._Regression-bs003.html">4</a></li>
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<li><a href="._Regression-bs004.html">5</a></li>
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<li><a href="._Regression-bs005.html">6</a></li>
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<li><a href="._Regression-bs006.html">7</a></li>
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<li><a href="._Regression-bs007.html">8</a></li>
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<li><a href="._Regression-bs008.html">9</a></li>
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<li><a href="._Regression-bs002.html">»</a></li>
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</ul>
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<!-- ------------------- end of main content --------------- -->
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@@ -50,7 +50,16 @@ Automatically generated HTML file from DocOnce source
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2,
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None,
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'___sec3'),
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('Optimizing our parameters', 2, None, '___sec4')]}
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('Optimizing our parameters', 2, None, '___sec4'),
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('Interpretations and optimizing our parameters',
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2,
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None,
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'___sec5'),
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('Interpretations and optimizing our parameters',
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2,
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None,
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'___sec6'),
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('The singular value decompostion', 2, None, '___sec7')]}
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end of tocinfo -->
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<body>
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@@ -65,8 +74,8 @@ MathJax.Hub.Config({
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}
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});
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</script>
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@@ -93,6 +102,9 @@ MathJax.Hub.Config({
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<!-- navigation toc: --> <li><a href="._Regression-bs003.html#___sec2" style="font-size: 80%;">Rewriting the fitting procedure as a linear algebra problem</a></li>
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<!-- navigation toc: --> <li><a href="._Regression-bs004.html#___sec3" style="font-size: 80%;">Generalizing the fitting procedure as a linear algebra problem</a></li>
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<!-- navigation toc: --> <li><a href="._Regression-bs005.html#___sec4" style="font-size: 80%;">Optimizing our parameters</a></li>
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||||
<!-- navigation toc: --> <li><a href="._Regression-bs006.html#___sec5" style="font-size: 80%;">Interpretations and optimizing our parameters</a></li>
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||||
<!-- navigation toc: --> <li><a href="._Regression-bs007.html#___sec6" style="font-size: 80%;">Interpretations and optimizing our parameters</a></li>
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<!-- navigation toc: --> <li><a href="._Regression-bs008.html#___sec7" style="font-size: 80%;">The singular value decompostion</a></li>
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</ul>
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</li>
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@@ -136,6 +148,9 @@ where \( \epsilon_i \) is the error in our approximation.
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<li><a href="._Regression-bs003.html">4</a></li>
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<li><a href="._Regression-bs004.html">5</a></li>
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<li><a href="._Regression-bs005.html">6</a></li>
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<li><a href="._Regression-bs006.html">7</a></li>
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<li><a href="._Regression-bs007.html">8</a></li>
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<li><a href="._Regression-bs008.html">9</a></li>
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<li><a href="._Regression-bs003.html">»</a></li>
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</ul>
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<!-- ------------------- end of main content --------------- -->
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@@ -0,0 +1,209 @@
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<a class="navbar-brand" href="Regression-bs.html">Data Analysis and Machine Learning: Linear Regression and more Advanced Regression Analysis</a>
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<a href="#" class="dropdown-toggle" data-toggle="dropdown">Contents <b class="caret"></b></a>
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<ul class="dropdown-menu">
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<!-- navigation toc: --> <li><a href="._Regression-bs001.html#___sec0" style="font-size: 80%;">Regression analysis, overarching aims</a></li>
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<!-- navigation toc: --> <li><a href="._Regression-bs002.html#___sec1" style="font-size: 80%;">General linear models</a></li>
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<!-- navigation toc: --> <li><a href="#___sec2" style="font-size: 80%;">Rewriting the fitting procedure as a linear algebra problem</a></li>
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||||
<!-- navigation toc: --> <li><a href="._Regression-bs004.html#___sec3" style="font-size: 80%;">Generalizing the fitting procedure as a linear algebra problem</a></li>
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||||
<!-- navigation toc: --> <li><a href="._Regression-bs005.html#___sec4" style="font-size: 80%;">Optimizing our parameters</a></li>
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||||
<!-- navigation toc: --> <li><a href="._Regression-bs006.html#___sec5" style="font-size: 80%;">Interpretations and optimizing our parameters</a></li>
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||||
<!-- navigation toc: --> <li><a href="._Regression-bs007.html#___sec6" style="font-size: 80%;">Interpretations and optimizing our parameters</a></li>
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||||
<!-- navigation toc: --> <li><a href="._Regression-bs008.html#___sec7" style="font-size: 80%;">The singular value decompostion</a></li>
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||||
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</ul>
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<a name="part0003"></a>
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<!-- !split -->
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<h2 id="___sec2" class="anchor">Rewriting the fitting procedure as a linear algebra problem </h2>
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<div class="panel panel-default">
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<div class="panel-body">
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<p> <!-- subsequent paragraphs come in larger fonts, so start with a paragraph -->
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For every set of values \( y_i,x_i \) we have thus the corresponding set of equations
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$$
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\begin{align*}
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y_0&=\beta_0+\beta_1x_0^1+\beta_2x_0^2+\dots+\beta_{n-1}x_0^{n-1}+\epsilon_0\\
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y_1&=\beta_0+\beta_1x_1^1+\beta_2x_1^2+\dots+\beta_{n-1}x_1^{n-1}+\epsilon_1\\
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y_2&=\beta_0+\beta_1x_2^1+\beta_2x_2^2+\dots+\beta_{n-1}x_2^{n-1}+\epsilon_2\\
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\dots & \dots \\
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y_{n-1}&=\beta_0+\beta_1x_{n-1}^1+\beta_2x_{n-1}^2+\dots+\beta_1x_{n-1}^{n-1}+\epsilon_{n-1}.\\
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\end{align*}
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$$
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Defining the vectors
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$$
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\hat{y} = [y_0,y_1, y_2,\dots, y_{n-1}]^T,
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$$
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$$
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\hat{\beta} = [\beta_0,\beta_1, \beta_2,\dots, \beta_{n-1}]^T,
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$$
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$$
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\hat{\epsilon} = [\epsilon_0,\epsilon_1, \epsilon_2,\dots, \epsilon_{n-1}]^T,
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$$
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and the matrix
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$$
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\hat{X}=
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\begin{bmatrix}
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1& x_{0}^1 &x_{0}^2& \dots & \dots &x_{0}^{n-1}\\
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1& x_{1}^1 &x_{1}^2& \dots & \dots &x_{1}^{n-1}\\
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1& x_{2}^1 &x_{2}^2& \dots & \dots &x_{2}^{n-1}\\
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\dots& \dots &\dots& \dots & \dots &\dots\\
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1& x_{n-1}^1 &x_{n-1}^2& \dots & \dots &x_{n-1}^{n-1}\\
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\end{bmatrix}
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$$
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we can rewrite our equations as
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$$
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\hat{y} = \hat{X}\hat{\beta}+\hat{\epsilon}.
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$$
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</div>
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||||
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|
||||
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|
||||
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|
||||
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||||
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|
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|
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<!-- navigation toc: --> <li><a href="._Regression-bs008.html#___sec7" style="font-size: 80%;">The singular value decompostion</a></li>
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<a name="part0004"></a>
|
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<!-- !split -->
|
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|
||||
<h2 id="___sec3" class="anchor">Generalizing the fitting procedure as a linear algebra problem </h2>
|
||||
<div class="panel panel-default">
|
||||
<div class="panel-body">
|
||||
<p> <!-- subsequent paragraphs come in larger fonts, so start with a paragraph -->
|
||||
We are obviously not limited to the above polynomial. We could replace the various powers of \( x \) with elements of Fourier series, that is, instead of \( x_i^j \) we could have \( \cos{(j x_i)} \) or \( \sin{(j x_i)} \), or time series or other orthogonal functions.
|
||||
For every set of values \( y_i,x_i \) we can then generalize the equations to
|
||||
$$
|
||||
\begin{align*}
|
||||
y_0&=\beta_0x_{00}+\beta_1x_{01}+\beta_2x_{02}+\dots+\beta_{n-1}x_{0n-1}+\epsilon_0\\
|
||||
y_1&=\beta_0x_{10}+\beta_1x_{11}+\beta_2x_{12}+\dots+\beta_{n-1}x_{1n-1}+\epsilon_1\\
|
||||
y_2&=\beta_0x_{20}+\beta_1x_{21}+\beta_2x_{22}+\dots+\beta_{n-1}x_{2n-1}+\epsilon_2\\
|
||||
\dots & \dots \\
|
||||
y_{i}&=\beta_0x_{i0}+\beta_1x_{i1}+\beta_2x_{i2}+\dots+\beta_{n-1}x_{in-1}+\epsilon_i\\
|
||||
\dots & \dots \\
|
||||
y_{n-1}&=\beta_0x_{n-1,0}+\beta_1x_{n-1,2}+\beta_2x_{n-1,2}+\dots+\beta_1x_{n-1}^{n-1,n-1}+\epsilon_{n-1}.\\
|
||||
\end{align*}
|
||||
$$
|
||||
|
||||
We redefine in turn the matrix \( \hat{X} \) as
|
||||
$$
|
||||
\hat{X}=
|
||||
\begin{bmatrix}
|
||||
x_{00}& x_{01} &x_{02}& \dots & \dots &x_{0,n-1}\\
|
||||
x_{10}& x_{11} &x_{12}& \dots & \dots &x_{1,n-1}\\
|
||||
x_{20}& x_{21}^1 &x_{22}2& \dots & \dots &x_{2,n-1}\\
|
||||
\dots& \dots &\dots& \dots & \dots &\dots\\
|
||||
x_{n-1,00}& x_{n-1,1} &x_{n-1,2}& \dots & \dots &x_{n-1,n-1}\\
|
||||
\end{bmatrix}
|
||||
$$
|
||||
|
||||
and without loss of generality we rewrite again our equations as
|
||||
$$
|
||||
\hat{y} = \hat{X}\hat{\beta}+\hat{\epsilon}.
|
||||
$$
|
||||
|
||||
The left-hand side of this equation forms know. Our error vector \( \hat{\epsilon} \) and the parameter vector \( \hat{\beta} \) are our unknow quantities. How can we obtain the optimal set of \( \beta_i \) values?
|
||||
</div>
|
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||||
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|
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|
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|
||||
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|
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|
||||
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|
||||
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|
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<!-- navigation toc: --> <li><a href="._Regression-bs001.html#___sec0" style="font-size: 80%;">Regression analysis, overarching aims</a></li>
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|
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|
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|
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<!-- navigation toc: --> <li><a href="._Regression-bs008.html#___sec7" style="font-size: 80%;">The singular value decompostion</a></li>
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|
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|
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|
||||
<div class="panel panel-default">
|
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<div class="panel-body">
|
||||
<p> <!-- subsequent paragraphs come in larger fonts, so start with a paragraph -->
|
||||
We have defined the matrix \( \hat{X} \)
|
||||
$$
|
||||
\begin{align*}
|
||||
y_0&=\beta_0x_{00}+\beta_1x_{01}+\beta_2x_{02}+\dots+\beta_{n-1}x_{0n-1}+\epsilon_0\\
|
||||
y_1&=\beta_0x_{10}+\beta_1x_{11}+\beta_2x_{12}+\dots+\beta_{n-1}x_{1n-1}+\epsilon_1\\
|
||||
y_2&=\beta_0x_{20}+\beta_1x_{21}+\beta_2x_{22}+\dots+\beta_{n-1}x_{2n-1}+\epsilon_1\\
|
||||
\dots & \dots \\
|
||||
y_{i}&=\beta_0x_{i0}+\beta_1x_{i1}+\beta_2x_{i2}+\dots+\beta_{n-1}x_{in-1}+\epsilon_1\\
|
||||
\dots & \dots \\
|
||||
y_{n-1}&=\beta_0x_{n-1,0}+\beta_1x_{n-1,2}+\beta_2x_{n-1,2}+\dots+\beta_1x_{n-1,n-1}+\epsilon_{n-1}.\\
|
||||
\end{align*}
|
||||
$$
|
||||
|
||||
We well use this matrix to define the approximation \( \hat{\tilde{y}} \) via the unknown quantity \( \hat{\beta} \) as
|
||||
$$
|
||||
\hat{\tilde{y}}= \hat{X}\hat{\beta},
|
||||
$$
|
||||
|
||||
and in order to find the optimal parameters \( \beta_i \) instead of solving the above linear algebra problem, we define a function which gives a measure of the spread between the values \( y_i \) (which represent hopefully the exact values) and the parametrized values \( \tilde{y}_i \), namely
|
||||
$$
|
||||
Q(\hat{\beta})=\sum_{i=0}^{n-1}\left(y_i-\tilde{y}_i\right)^2=\left(\hat{y}-\hat{\tilde{y}}\right)^T\left(\hat{y}-\hat{\tilde{y}}\right),
|
||||
$$
|
||||
|
||||
or using the matrix \( \hat{X} \) as
|
||||
$$
|
||||
Q(\hat{\beta})=\left(\hat{y}-\hat{X}\hat{\beta}\right)^T\left(\hat{y}-\hat{X}\hat{\beta}\right).
|
||||
$$
|
||||
</div>
|
||||
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|
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|
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<p>
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|
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|
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|
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<!-- navigation toc: --> <li><a href="._Regression-bs008.html#___sec7" style="font-size: 80%;">The singular value decompostion</a></li>
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<!-- !split -->
|
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<h2 id="___sec5" class="anchor">Interpretations and optimizing our parameters </h2>
|
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<div class="panel panel-default">
|
||||
<div class="panel-body">
|
||||
<p> <!-- subsequent paragraphs come in larger fonts, so start with a paragraph -->
|
||||
The function
|
||||
$$
|
||||
Q(\hat{\beta})=\left(\hat{y}-\hat{X}\hat{\beta}\right)^T\left(\hat{y}-\hat{X}\hat{\beta}\right),
|
||||
$$
|
||||
|
||||
can be linked to the variance of the quantity \( y_i \) if we interpret the latter as the mean value of for example a numerical experiment. When linking below with the maximum likelihood approach below, we will indeed interpret \( y_i \) as a mean value
|
||||
$$
|
||||
y_{i}=\langle y_i \rangle = \beta_0x_{i,0}+\beta_1x_{i,1}+\beta_2x_{i,2}+\dots+\beta_{n-1}x_{i,n-1}+\epsilon_i,
|
||||
$$
|
||||
|
||||
where \( \langle y_i \rangle \) is the mean value. Keep in mind also that till now we have treated \( y_i \) as the exact value. Normally, the response (dependent or outcome) variable \( y_i \) the outcome of a numerical experiment or another type of experiment and is thus only an approximation to the true value. It is then always accompanied by an error estimate, often limited to a statistical error estimate given by the standard deviation discussed earlier. In the discussion here we will treat \( y_i \) as our exact value for the response variable.
|
||||
|
||||
<p>
|
||||
In order to find the parameters \( \beta_i \) we will then minimize the spread of \( Q(\hat{\beta}) \) by requiring
|
||||
$$
|
||||
\frac{\partial Q(\hat{\beta})}{\partial \beta_j} = \frac{\partial }{\partial \beta_j}\left[ \sum_{i=0}^{n-1}\left(y_i-\beta_0x_{i,0}+\beta_1x_{i,1}+\beta_2x_{i,2}+\dots+\beta_{n-1}x_{i,n-1}\right)^2\right]=0,
|
||||
$$
|
||||
|
||||
which results in
|
||||
$$
|
||||
\frac{\partial Q(\hat{\beta})}{\partial \beta_j} = -2\left[ \sum_{i=0}^{n-1}x_{ij}\left(y_i-\beta_0x_{i,0}+\beta_1x_{i,1}+\beta_2x_{i,2}+\dots+\beta_{n-1}x_{i,n-1}\right)\right]=0,
|
||||
$$
|
||||
|
||||
or in a matrix-vector form as
|
||||
$$
|
||||
\frac{\partial Q(\hat{\beta})}{\partial \hat{\beta}} = 0 = \hat{X}^T\left( \hat{y}-\hat{X}\hat{\beta}\right).
|
||||
$$
|
||||
|
||||
<p>
|
||||
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|
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|
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|
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<!-- !split -->
|
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|
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|
||||
<div class="panel panel-default">
|
||||
<div class="panel-body">
|
||||
<p> <!-- subsequent paragraphs come in larger fonts, so start with a paragraph -->
|
||||
We can rewrite
|
||||
$$
|
||||
\frac{\partial Q(\hat{\beta})}{\partial \hat{\beta}} = 0 = \hat{X}^T\left( \hat{y}-\hat{X}\hat{\beta}\right),
|
||||
$$
|
||||
|
||||
as
|
||||
$$
|
||||
\hat{X}^T\hat{y} = \hat{X}^T\hat{X}\hat{\beta},
|
||||
$$
|
||||
|
||||
and if the matrix \( \hat{X}^T\hat{X} \) is invertible we have the solution
|
||||
$$
|
||||
\hat{\beta} =\left(\hat{X}^T\hat{X}\right)^{-1}\hat{X}^T\hat{y}.
|
||||
$$
|
||||
|
||||
The residuals \( \hat{\epsilon} \) are in turn given by
|
||||
$$
|
||||
\hat{\epsilon} = \hat{y}-\hat{\tilde{y}} = \hat{y}-\hat{X}\hat{\beta},
|
||||
$$
|
||||
|
||||
and with
|
||||
$$
|
||||
\hat{X}^T\left( \hat{y}-\hat{X}\hat{\beta}\right)= 0,
|
||||
$$
|
||||
|
||||
we have
|
||||
$$
|
||||
\hat{X}^T\hat{\epsilon}=\hat{X}^T\left( \hat{y}-\hat{X}\hat{\beta}\right)= 0,
|
||||
$$
|
||||
|
||||
meaning that the solution for \( \hat{\beta} \) is the one which minimizes the residuals. Later we will link this with the maximum likelihood approach.
|
||||
|
||||
<p>
|
||||
</div>
|
||||
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|
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{'highest level': 2,
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||||
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|
||||
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|
||||
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|
||||
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|
||||
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|
||||
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|
||||
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|
||||
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|
||||
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|
||||
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|
||||
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|
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|
||||
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|
||||
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|
||||
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|
||||
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|
||||
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|
||||
None,
|
||||
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|
||||
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end of tocinfo -->
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||||
|
||||
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<a class="navbar-brand" href="Regression-bs.html">Data Analysis and Machine Learning: Linear Regression and more Advanced Regression Analysis</a>
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<!-- navigation toc: --> <li><a href="._Regression-bs001.html#___sec0" style="font-size: 80%;">Regression analysis, overarching aims</a></li>
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<!-- navigation toc: --> <li><a href="._Regression-bs002.html#___sec1" style="font-size: 80%;">General linear models</a></li>
|
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<!-- navigation toc: --> <li><a href="._Regression-bs003.html#___sec2" style="font-size: 80%;">Rewriting the fitting procedure as a linear algebra problem</a></li>
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<!-- navigation toc: --> <li><a href="._Regression-bs004.html#___sec3" style="font-size: 80%;">Generalizing the fitting procedure as a linear algebra problem</a></li>
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<!-- navigation toc: --> <li><a href="._Regression-bs005.html#___sec4" style="font-size: 80%;">Optimizing our parameters</a></li>
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<!-- navigation toc: --> <li><a href="._Regression-bs006.html#___sec5" style="font-size: 80%;">Interpretations and optimizing our parameters</a></li>
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<!-- navigation toc: --> <li><a href="._Regression-bs007.html#___sec6" style="font-size: 80%;">Interpretations and optimizing our parameters</a></li>
|
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<!-- navigation toc: --> <li><a href="#___sec7" style="font-size: 80%;">The singular value decompostion</a></li>
|
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|
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<p> </p><p> </p><p> </p> <!-- add vertical space -->
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||||
|
||||
<a name="part0008"></a>
|
||||
<!-- !split -->
|
||||
|
||||
<h2 id="___sec7" class="anchor">The singular value decompostion </h2>
|
||||
<div class="panel panel-default">
|
||||
<div class="panel-body">
|
||||
<p> <!-- subsequent paragraphs come in larger fonts, so start with a paragraph -->
|
||||
Here we derive the equations for the SVD.
|
||||
</div>
|
||||
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@@ -50,7 +50,16 @@ Automatically generated HTML file from DocOnce source
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2,
|
||||
None,
|
||||
'___sec3'),
|
||||
('Optimizing our parameters', 2, None, '___sec4')]}
|
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('Optimizing our parameters', 2, None, '___sec4'),
|
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('Interpretations and optimizing our parameters',
|
||||
2,
|
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None,
|
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'___sec5'),
|
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('Interpretations and optimizing our parameters',
|
||||
2,
|
||||
None,
|
||||
'___sec6'),
|
||||
('The singular value decompostion', 2, None, '___sec7')]}
|
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end of tocinfo -->
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<body>
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@@ -65,8 +74,8 @@ MathJax.Hub.Config({
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}
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});
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</script>
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<script type="text/javascript" async
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src="https://cdnjs.cloudflare.com/ajax/libs/mathjax/2.7.1/MathJax.js?config=TeX-AMS-MML_HTMLorMML">
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<script type="text/javascript"
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src="http://cdn.mathjax.org/mathjax/latest/MathJax.js?config=TeX-AMS-MML_HTMLorMML">
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||||
|
||||
@@ -93,6 +102,9 @@ MathJax.Hub.Config({
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||||
<!-- navigation toc: --> <li><a href="._Regression-bs003.html#___sec2" style="font-size: 80%;">Rewriting the fitting procedure as a linear algebra problem</a></li>
|
||||
<!-- navigation toc: --> <li><a href="._Regression-bs004.html#___sec3" style="font-size: 80%;">Generalizing the fitting procedure as a linear algebra problem</a></li>
|
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<!-- navigation toc: --> <li><a href="._Regression-bs005.html#___sec4" style="font-size: 80%;">Optimizing our parameters</a></li>
|
||||
<!-- navigation toc: --> <li><a href="._Regression-bs006.html#___sec5" style="font-size: 80%;">Interpretations and optimizing our parameters</a></li>
|
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<!-- navigation toc: --> <li><a href="._Regression-bs007.html#___sec6" style="font-size: 80%;">Interpretations and optimizing our parameters</a></li>
|
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<!-- navigation toc: --> <li><a href="._Regression-bs008.html#___sec7" style="font-size: 80%;">The singular value decompostion</a></li>
|
||||
|
||||
</ul>
|
||||
</li>
|
||||
@@ -127,7 +139,7 @@ MathJax.Hub.Config({
|
||||
<center>[2] <b>Department of Physics and Astronomy and National Superconducting Cyclotron Laboratory, Michigan State University</b></center>
|
||||
<br>
|
||||
<p>
|
||||
<center><h4>Oct 14, 2017</h4></center> <!-- date -->
|
||||
<center><h4>Oct 17, 2017</h4></center> <!-- date -->
|
||||
<br>
|
||||
<p>
|
||||
|
||||
@@ -146,6 +158,9 @@ MathJax.Hub.Config({
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||||
<li><a href="._Regression-bs003.html">4</a></li>
|
||||
<li><a href="._Regression-bs004.html">5</a></li>
|
||||
<li><a href="._Regression-bs005.html">6</a></li>
|
||||
<li><a href="._Regression-bs006.html">7</a></li>
|
||||
<li><a href="._Regression-bs007.html">8</a></li>
|
||||
<li><a href="._Regression-bs008.html">9</a></li>
|
||||
<li><a href="._Regression-bs001.html">»</a></li>
|
||||
</ul>
|
||||
<!-- ------------------- end of main content --------------- -->
|
||||
|
||||
@@ -1,4 +1,3 @@
|
||||
\
|
||||
<!DOCTYPE html>
|
||||
|
||||
<meta http-equiv="Content-Type" content="text/html; charset=utf-8" />
|
||||
@@ -117,8 +116,8 @@ MathJax.Hub.Config({
|
||||
}
|
||||
});
|
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</script>
|
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<script type="text/javascript" async
|
||||
src="https://cdnjs.cloudflare.com/ajax/libs/mathjax/2.7.1/MathJax.js?config=TeX-AMS-MML_HTMLorMML">
|
||||
<script type="text/javascript"
|
||||
src="http://cdn.mathjax.org/mathjax/latest/MathJax.js?config=TeX-AMS-MML_HTMLorMML">
|
||||
</script>
|
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|
||||
|
||||
@@ -148,7 +147,7 @@ MathJax.Hub.Config({
|
||||
<center>[2] <b>Department of Physics and Astronomy and National Superconducting Cyclotron Laboratory, Michigan State University</b></center>
|
||||
<br>
|
||||
<p> <br>
|
||||
<center><h4>Oct 14, 2017</h4></center> <!-- date -->
|
||||
<center><h4>Oct 17, 2017</h4></center> <!-- date -->
|
||||
<br>
|
||||
<p>
|
||||
|
||||
@@ -211,19 +210,13 @@ where \( \epsilon_i \) is the error in our approximation.
|
||||
For every set of values \( y_i,x_i \) we have thus the corresponding set of equations
|
||||
<p> <br>
|
||||
$$
|
||||
\begin{align}
|
||||
y_0&=\beta_0+\beta_1x_0^1+\beta_2x_0^2+\dots+\beta_{n-1}x_0^{n-1}+\epsilon_0
|
||||
\tag{1}\\
|
||||
y_1&=\beta_0+\beta_1x_1^1+\beta_2x_1^2+\dots+\beta_{n-1}x_1^{n-1}+\epsilon_1
|
||||
\tag{2}\\
|
||||
y_2&=\beta_0+\beta_1x_2^1+\beta_2x_2^2+\dots+\beta_{n-1}x_2^{n-1}+\epsilon_2
|
||||
\tag{3}\\
|
||||
\dots & \dots
|
||||
\tag{4}\\
|
||||
y_{n-1}&=\beta_0+\beta_1x_{n-1}^1+\beta_2x_{n-1}^2+\dots+\beta_1x_{n-1}^{n-1}+\epsilon_{n-1}.
|
||||
\tag{5}\\
|
||||
\tag{6}
|
||||
\end{align}
|
||||
\begin{align*}
|
||||
y_0&=\beta_0+\beta_1x_0^1+\beta_2x_0^2+\dots+\beta_{n-1}x_0^{n-1}+\epsilon_0\\
|
||||
y_1&=\beta_0+\beta_1x_1^1+\beta_2x_1^2+\dots+\beta_{n-1}x_1^{n-1}+\epsilon_1\\
|
||||
y_2&=\beta_0+\beta_1x_2^1+\beta_2x_2^2+\dots+\beta_{n-1}x_2^{n-1}+\epsilon_2\\
|
||||
\dots & \dots \\
|
||||
y_{n-1}&=\beta_0+\beta_1x_{n-1}^1+\beta_2x_{n-1}^2+\dots+\beta_1x_{n-1}^{n-1}+\epsilon_{n-1}.\\
|
||||
\end{align*}
|
||||
$$
|
||||
<p> <br>
|
||||
|
||||
@@ -279,23 +272,15 @@ We are obviously not limited to the above polynomial. We could replace the vario
|
||||
For every set of values \( y_i,x_i \) we can then generalize the equations to
|
||||
<p> <br>
|
||||
$$
|
||||
\begin{align}
|
||||
y_0&=\beta_0x_{00}+\beta_1x_{01}+\beta_2x_{02}+\dots+\beta_{n-1}x_{0n-1}+\epsilon_0
|
||||
\tag{7}\\
|
||||
y_1&=\beta_0x_{10}+\beta_1x_{11}+\beta_2x_{12}+\dots+\beta_{n-1}x_{1n-1}+\epsilon_1
|
||||
\tag{8}\\
|
||||
y_2&=\beta_0x_{20}+\beta_1x_{21}+\beta_2x_{22}+\dots+\beta_{n-1}x_{2n-1}+\epsilon_1
|
||||
\tag{9}\\
|
||||
\dots & \dots
|
||||
\tag{10}\\
|
||||
y_{i}&=\beta_0x_{i0}+\beta_1x_{i1}+\beta_2x_{i2}+\dots+\beta_{n-1}x_{in-1}+\epsilon_1
|
||||
\tag{11}\\
|
||||
\dots & \dots
|
||||
\tag{12}\\
|
||||
y_{n-1}&=\beta_0x_{n-1,0}+\beta_1x_{n-1,2}+\beta_2x_{n-1,2}+\dots+\beta_1x_{n-1}^{n-1,n-1}+\epsilon_{n-1}.
|
||||
\tag{13}\\
|
||||
\tag{14}
|
||||
\end{align}
|
||||
\begin{align*}
|
||||
y_0&=\beta_0x_{00}+\beta_1x_{01}+\beta_2x_{02}+\dots+\beta_{n-1}x_{0n-1}+\epsilon_0\\
|
||||
y_1&=\beta_0x_{10}+\beta_1x_{11}+\beta_2x_{12}+\dots+\beta_{n-1}x_{1n-1}+\epsilon_1\\
|
||||
y_2&=\beta_0x_{20}+\beta_1x_{21}+\beta_2x_{22}+\dots+\beta_{n-1}x_{2n-1}+\epsilon_2\\
|
||||
\dots & \dots \\
|
||||
y_{i}&=\beta_0x_{i0}+\beta_1x_{i1}+\beta_2x_{i2}+\dots+\beta_{n-1}x_{in-1}+\epsilon_i\\
|
||||
\dots & \dots \\
|
||||
y_{n-1}&=\beta_0x_{n-1,0}+\beta_1x_{n-1,2}+\beta_2x_{n-1,2}+\dots+\beta_1x_{n-1}^{n-1,n-1}+\epsilon_{n-1}.\\
|
||||
\end{align*}
|
||||
$$
|
||||
<p> <br>
|
||||
|
||||
@@ -329,27 +314,154 @@ The left-hand side of this equation forms know. Our error vector \( \hat{\epsilo
|
||||
<h2 id="___sec4">Optimizing our parameters </h2>
|
||||
<div class="alert alert-block alert-block alert-text-normal">
|
||||
<b></b>
|
||||
<p>
|
||||
We have defined the matrix \( \hat{X} \)
|
||||
<p> <br>
|
||||
$$
|
||||
\begin{align}
|
||||
y_0&=\beta_0x_{00}+\beta_1x_{01}+\beta_2x_{02}+\dots+\beta_{n-1}x_{0n-1}+\epsilon_0
|
||||
\tag{15}\\
|
||||
y_1&=\beta_0x_{10}+\beta_1x_{11}+\beta_2x_{12}+\dots+\beta_{n-1}x_{1n-1}+\epsilon_1
|
||||
\tag{16}\\
|
||||
y_2&=\beta_0x_{20}+\beta_1x_{21}+\beta_2x_{22}+\dots+\beta_{n-1}x_{2n-1}+\epsilon_1
|
||||
\tag{17}\\
|
||||
\dots & \dots
|
||||
\tag{18}\\
|
||||
y_{i}&=\beta_0x_{i0}+\beta_1x_{i1}+\beta_2x_{i2}+\dots+\beta_{n-1}x_{in-1}+\epsilon_1
|
||||
\tag{19}\\
|
||||
\dots & \dots
|
||||
\tag{20}\\
|
||||
y_{n-1}&=\beta_0x_{n-1,0}+\beta_1x_{n-1,2}+\beta_2x_{n-1,2}+\dots+\beta_1x_{n-1}^{n-1,n-1}+\epsilon_{n-1}.
|
||||
\tag{21}\\
|
||||
\tag{22}
|
||||
\end{align}
|
||||
\begin{align*}
|
||||
y_0&=\beta_0x_{00}+\beta_1x_{01}+\beta_2x_{02}+\dots+\beta_{n-1}x_{0n-1}+\epsilon_0\\
|
||||
y_1&=\beta_0x_{10}+\beta_1x_{11}+\beta_2x_{12}+\dots+\beta_{n-1}x_{1n-1}+\epsilon_1\\
|
||||
y_2&=\beta_0x_{20}+\beta_1x_{21}+\beta_2x_{22}+\dots+\beta_{n-1}x_{2n-1}+\epsilon_1\\
|
||||
\dots & \dots \\
|
||||
y_{i}&=\beta_0x_{i0}+\beta_1x_{i1}+\beta_2x_{i2}+\dots+\beta_{n-1}x_{in-1}+\epsilon_1\\
|
||||
\dots & \dots \\
|
||||
y_{n-1}&=\beta_0x_{n-1,0}+\beta_1x_{n-1,2}+\beta_2x_{n-1,2}+\dots+\beta_1x_{n-1,n-1}+\epsilon_{n-1}.\\
|
||||
\end{align*}
|
||||
$$
|
||||
<p> <br>
|
||||
|
||||
We well use this matrix to define the approximation \( \hat{\tilde{y}} \) via the unknown quantity \( \hat{\beta} \) as
|
||||
<p> <br>
|
||||
$$
|
||||
\hat{\tilde{y}}= \hat{X}\hat{\beta},
|
||||
$$
|
||||
<p> <br>
|
||||
|
||||
and in order to find the optimal parameters \( \beta_i \) instead of solving the above linear algebra problem, we define a function which gives a measure of the spread between the values \( y_i \) (which represent hopefully the exact values) and the parametrized values \( \tilde{y}_i \), namely
|
||||
<p> <br>
|
||||
$$
|
||||
Q(\hat{\beta})=\sum_{i=0}^{n-1}\left(y_i-\tilde{y}_i\right)^2=\left(\hat{y}-\hat{\tilde{y}}\right)^T\left(\hat{y}-\hat{\tilde{y}}\right),
|
||||
$$
|
||||
<p> <br>
|
||||
|
||||
or using the matrix \( \hat{X} \) as
|
||||
<p> <br>
|
||||
$$
|
||||
Q(\hat{\beta})=\left(\hat{y}-\hat{X}\hat{\beta}\right)^T\left(\hat{y}-\hat{X}\hat{\beta}\right).
|
||||
$$
|
||||
<p> <br>
|
||||
</div>
|
||||
</section>
|
||||
|
||||
|
||||
<section>
|
||||
<h2 id="___sec5">Interpretations and optimizing our parameters </h2>
|
||||
<div class="alert alert-block alert-block alert-text-normal">
|
||||
<b></b>
|
||||
<p>
|
||||
The function
|
||||
<p> <br>
|
||||
$$
|
||||
Q(\hat{\beta})=\left(\hat{y}-\hat{X}\hat{\beta}\right)^T\left(\hat{y}-\hat{X}\hat{\beta}\right),
|
||||
$$
|
||||
<p> <br>
|
||||
|
||||
can be linked to the variance of the quantity \( y_i \) if we interpret the latter as the mean value of for example a numerical experiment. When linking below with the maximum likelihood approach below, we will indeed interpret \( y_i \) as a mean value
|
||||
<p> <br>
|
||||
$$
|
||||
y_{i}=\langle y_i \rangle = \beta_0x_{i,0}+\beta_1x_{i,1}+\beta_2x_{i,2}+\dots+\beta_{n-1}x_{i,n-1}+\epsilon_i,
|
||||
$$
|
||||
<p> <br>
|
||||
|
||||
where \( \langle y_i \rangle \) is the mean value. Keep in mind also that till now we have treated \( y_i \) as the exact value. Normally, the response (dependent or outcome) variable \( y_i \) the outcome of a numerical experiment or another type of experiment and is thus only an approximation to the true value. It is then always accompanied by an error estimate, often limited to a statistical error estimate given by the standard deviation discussed earlier. In the discussion here we will treat \( y_i \) as our exact value for the response variable.
|
||||
|
||||
<p>
|
||||
In order to find the parameters \( \beta_i \) we will then minimize the spread of \( Q(\hat{\beta}) \) by requiring
|
||||
<p> <br>
|
||||
$$
|
||||
\frac{\partial Q(\hat{\beta})}{\partial \beta_j} = \frac{\partial }{\partial \beta_j}\left[ \sum_{i=0}^{n-1}\left(y_i-\beta_0x_{i,0}+\beta_1x_{i,1}+\beta_2x_{i,2}+\dots+\beta_{n-1}x_{i,n-1}\right)^2\right]=0,
|
||||
$$
|
||||
<p> <br>
|
||||
|
||||
which results in
|
||||
<p> <br>
|
||||
$$
|
||||
\frac{\partial Q(\hat{\beta})}{\partial \beta_j} = -2\left[ \sum_{i=0}^{n-1}x_{ij}\left(y_i-\beta_0x_{i,0}+\beta_1x_{i,1}+\beta_2x_{i,2}+\dots+\beta_{n-1}x_{i,n-1}\right)\right]=0,
|
||||
$$
|
||||
<p> <br>
|
||||
|
||||
or in a matrix-vector form as
|
||||
<p> <br>
|
||||
$$
|
||||
\frac{\partial Q(\hat{\beta})}{\partial \hat{\beta}} = 0 = \hat{X}^T\left( \hat{y}-\hat{X}\hat{\beta}\right).
|
||||
$$
|
||||
<p> <br>
|
||||
|
||||
|
||||
</div>
|
||||
</section>
|
||||
|
||||
|
||||
<section>
|
||||
<h2 id="___sec6">Interpretations and optimizing our parameters </h2>
|
||||
<div class="alert alert-block alert-block alert-text-normal">
|
||||
<b></b>
|
||||
<p>
|
||||
We can rewrite
|
||||
<p> <br>
|
||||
$$
|
||||
\frac{\partial Q(\hat{\beta})}{\partial \hat{\beta}} = 0 = \hat{X}^T\left( \hat{y}-\hat{X}\hat{\beta}\right),
|
||||
$$
|
||||
<p> <br>
|
||||
|
||||
as
|
||||
<p> <br>
|
||||
$$
|
||||
\hat{X}^T\hat{y} = \hat{X}^T\hat{X}\hat{\beta},
|
||||
$$
|
||||
<p> <br>
|
||||
|
||||
and if the matrix \( \hat{X}^T\hat{X} \) is invertible we have the solution
|
||||
<p> <br>
|
||||
$$
|
||||
\hat{\beta} =\left(\hat{X}^T\hat{X}\right)^{-1}\hat{X}^T\hat{y}.
|
||||
$$
|
||||
<p> <br>
|
||||
|
||||
The residuals \( \hat{\epsilon} \) are in turn given by
|
||||
<p> <br>
|
||||
$$
|
||||
\hat{\epsilon} = \hat{y}-\hat{\tilde{y}} = \hat{y}-\hat{X}\hat{\beta},
|
||||
$$
|
||||
<p> <br>
|
||||
|
||||
and with
|
||||
<p> <br>
|
||||
$$
|
||||
\hat{X}^T\left( \hat{y}-\hat{X}\hat{\beta}\right)= 0,
|
||||
$$
|
||||
<p> <br>
|
||||
|
||||
we have
|
||||
<p> <br>
|
||||
$$
|
||||
\hat{X}^T\hat{\epsilon}=\hat{X}^T\left( \hat{y}-\hat{X}\hat{\beta}\right)= 0,
|
||||
$$
|
||||
<p> <br>
|
||||
|
||||
meaning that the solution for \( \hat{\beta} \) is the one which minimizes the residuals. Later we will link this with the maximum likelihood approach.
|
||||
|
||||
|
||||
</div>
|
||||
</section>
|
||||
|
||||
|
||||
<section>
|
||||
<h2 id="___sec7">The singular value decompostion </h2>
|
||||
<div class="alert alert-block alert-block alert-text-normal">
|
||||
<b></b>
|
||||
<p>
|
||||
Here we derive the equations for the SVD.
|
||||
</div>
|
||||
</section>
|
||||
|
||||
|
||||
@@ -70,7 +70,16 @@ div { text-align: justify; text-justify: inter-word; }
|
||||
2,
|
||||
None,
|
||||
'___sec3'),
|
||||
('Optimizing our parameters', 2, None, '___sec4')]}
|
||||
('Optimizing our parameters', 2, None, '___sec4'),
|
||||
('Interpretations and optimizing our parameters',
|
||||
2,
|
||||
None,
|
||||
'___sec5'),
|
||||
('Interpretations and optimizing our parameters',
|
||||
2,
|
||||
None,
|
||||
'___sec6'),
|
||||
('The singular value decompostion', 2, None, '___sec7')]}
|
||||
end of tocinfo -->
|
||||
|
||||
<body>
|
||||
@@ -85,8 +94,8 @@ MathJax.Hub.Config({
|
||||
}
|
||||
});
|
||||
</script>
|
||||
<script type="text/javascript" async
|
||||
src="https://cdnjs.cloudflare.com/ajax/libs/mathjax/2.7.1/MathJax.js?config=TeX-AMS-MML_HTMLorMML">
|
||||
<script type="text/javascript"
|
||||
src="http://cdn.mathjax.org/mathjax/latest/MathJax.js?config=TeX-AMS-MML_HTMLorMML">
|
||||
</script>
|
||||
|
||||
|
||||
@@ -112,7 +121,7 @@ MathJax.Hub.Config({
|
||||
<center>[2] <b>Department of Physics and Astronomy and National Superconducting Cyclotron Laboratory, Michigan State University</b></center>
|
||||
<br>
|
||||
<p>
|
||||
<center><h4>Oct 14, 2017</h4></center> <!-- date -->
|
||||
<center><h4>Oct 17, 2017</h4></center> <!-- date -->
|
||||
<br>
|
||||
<p>
|
||||
<!-- !split --><br><br><br><br><br><br><br><br><br><br>
|
||||
@@ -167,19 +176,13 @@ where \( \epsilon_i \) is the error in our approximation.
|
||||
<p>
|
||||
For every set of values \( y_i,x_i \) we have thus the corresponding set of equations
|
||||
$$
|
||||
\begin{align}
|
||||
y_0&=\beta_0+\beta_1x_0^1+\beta_2x_0^2+\dots+\beta_{n-1}x_0^{n-1}+\epsilon_0
|
||||
\label{_auto1}\\
|
||||
y_1&=\beta_0+\beta_1x_1^1+\beta_2x_1^2+\dots+\beta_{n-1}x_1^{n-1}+\epsilon_1
|
||||
\label{_auto2}\\
|
||||
y_2&=\beta_0+\beta_1x_2^1+\beta_2x_2^2+\dots+\beta_{n-1}x_2^{n-1}+\epsilon_2
|
||||
\label{_auto3}\\
|
||||
\dots & \dots
|
||||
\label{_auto4}\\
|
||||
y_{n-1}&=\beta_0+\beta_1x_{n-1}^1+\beta_2x_{n-1}^2+\dots+\beta_1x_{n-1}^{n-1}+\epsilon_{n-1}.
|
||||
\label{_auto5}\\
|
||||
\label{_auto6}
|
||||
\end{align}
|
||||
\begin{align*}
|
||||
y_0&=\beta_0+\beta_1x_0^1+\beta_2x_0^2+\dots+\beta_{n-1}x_0^{n-1}+\epsilon_0\\
|
||||
y_1&=\beta_0+\beta_1x_1^1+\beta_2x_1^2+\dots+\beta_{n-1}x_1^{n-1}+\epsilon_1\\
|
||||
y_2&=\beta_0+\beta_1x_2^1+\beta_2x_2^2+\dots+\beta_{n-1}x_2^{n-1}+\epsilon_2\\
|
||||
\dots & \dots \\
|
||||
y_{n-1}&=\beta_0+\beta_1x_{n-1}^1+\beta_2x_{n-1}^2+\dots+\beta_1x_{n-1}^{n-1}+\epsilon_{n-1}.\\
|
||||
\end{align*}
|
||||
$$
|
||||
|
||||
Defining the vectors
|
||||
@@ -224,23 +227,15 @@ $$
|
||||
We are obviously not limited to the above polynomial. We could replace the various powers of \( x \) with elements of Fourier series, that is, instead of \( x_i^j \) we could have \( \cos{(j x_i)} \) or \( \sin{(j x_i)} \), or time series or other orthogonal functions.
|
||||
For every set of values \( y_i,x_i \) we can then generalize the equations to
|
||||
$$
|
||||
\begin{align}
|
||||
y_0&=\beta_0x_{00}+\beta_1x_{01}+\beta_2x_{02}+\dots+\beta_{n-1}x_{0n-1}+\epsilon_0
|
||||
\label{_auto7}\\
|
||||
y_1&=\beta_0x_{10}+\beta_1x_{11}+\beta_2x_{12}+\dots+\beta_{n-1}x_{1n-1}+\epsilon_1
|
||||
\label{_auto8}\\
|
||||
y_2&=\beta_0x_{20}+\beta_1x_{21}+\beta_2x_{22}+\dots+\beta_{n-1}x_{2n-1}+\epsilon_1
|
||||
\label{_auto9}\\
|
||||
\dots & \dots
|
||||
\label{_auto10}\\
|
||||
y_{i}&=\beta_0x_{i0}+\beta_1x_{i1}+\beta_2x_{i2}+\dots+\beta_{n-1}x_{in-1}+\epsilon_1
|
||||
\label{_auto11}\\
|
||||
\dots & \dots
|
||||
\label{_auto12}\\
|
||||
y_{n-1}&=\beta_0x_{n-1,0}+\beta_1x_{n-1,2}+\beta_2x_{n-1,2}+\dots+\beta_1x_{n-1}^{n-1,n-1}+\epsilon_{n-1}.
|
||||
\label{_auto13}\\
|
||||
\label{_auto14}
|
||||
\end{align}
|
||||
\begin{align*}
|
||||
y_0&=\beta_0x_{00}+\beta_1x_{01}+\beta_2x_{02}+\dots+\beta_{n-1}x_{0n-1}+\epsilon_0\\
|
||||
y_1&=\beta_0x_{10}+\beta_1x_{11}+\beta_2x_{12}+\dots+\beta_{n-1}x_{1n-1}+\epsilon_1\\
|
||||
y_2&=\beta_0x_{20}+\beta_1x_{21}+\beta_2x_{22}+\dots+\beta_{n-1}x_{2n-1}+\epsilon_2\\
|
||||
\dots & \dots \\
|
||||
y_{i}&=\beta_0x_{i0}+\beta_1x_{i1}+\beta_2x_{i2}+\dots+\beta_{n-1}x_{in-1}+\epsilon_i\\
|
||||
\dots & \dots \\
|
||||
y_{n-1}&=\beta_0x_{n-1,0}+\beta_1x_{n-1,2}+\beta_2x_{n-1,2}+\dots+\beta_1x_{n-1}^{n-1,n-1}+\epsilon_{n-1}.\\
|
||||
\end{align*}
|
||||
$$
|
||||
|
||||
We redefine in turn the matrix \( \hat{X} \) as
|
||||
@@ -271,28 +266,131 @@ The left-hand side of this equation forms know. Our error vector \( \hat{\epsilo
|
||||
<div class="alert alert-block alert-block alert-text-normal">
|
||||
<b></b>
|
||||
<p>
|
||||
We have defined the matrix \( \hat{X} \)
|
||||
$$
|
||||
\begin{align}
|
||||
y_0&=\beta_0x_{00}+\beta_1x_{01}+\beta_2x_{02}+\dots+\beta_{n-1}x_{0n-1}+\epsilon_0
|
||||
\label{_auto15}\\
|
||||
y_1&=\beta_0x_{10}+\beta_1x_{11}+\beta_2x_{12}+\dots+\beta_{n-1}x_{1n-1}+\epsilon_1
|
||||
\label{_auto16}\\
|
||||
y_2&=\beta_0x_{20}+\beta_1x_{21}+\beta_2x_{22}+\dots+\beta_{n-1}x_{2n-1}+\epsilon_1
|
||||
\label{_auto17}\\
|
||||
\dots & \dots
|
||||
\label{_auto18}\\
|
||||
y_{i}&=\beta_0x_{i0}+\beta_1x_{i1}+\beta_2x_{i2}+\dots+\beta_{n-1}x_{in-1}+\epsilon_1
|
||||
\label{_auto19}\\
|
||||
\dots & \dots
|
||||
\label{_auto20}\\
|
||||
y_{n-1}&=\beta_0x_{n-1,0}+\beta_1x_{n-1,2}+\beta_2x_{n-1,2}+\dots+\beta_1x_{n-1}^{n-1,n-1}+\epsilon_{n-1}.
|
||||
\label{_auto21}\\
|
||||
\label{_auto22}
|
||||
\end{align}
|
||||
\begin{align*}
|
||||
y_0&=\beta_0x_{00}+\beta_1x_{01}+\beta_2x_{02}+\dots+\beta_{n-1}x_{0n-1}+\epsilon_0\\
|
||||
y_1&=\beta_0x_{10}+\beta_1x_{11}+\beta_2x_{12}+\dots+\beta_{n-1}x_{1n-1}+\epsilon_1\\
|
||||
y_2&=\beta_0x_{20}+\beta_1x_{21}+\beta_2x_{22}+\dots+\beta_{n-1}x_{2n-1}+\epsilon_1\\
|
||||
\dots & \dots \\
|
||||
y_{i}&=\beta_0x_{i0}+\beta_1x_{i1}+\beta_2x_{i2}+\dots+\beta_{n-1}x_{in-1}+\epsilon_1\\
|
||||
\dots & \dots \\
|
||||
y_{n-1}&=\beta_0x_{n-1,0}+\beta_1x_{n-1,2}+\beta_2x_{n-1,2}+\dots+\beta_1x_{n-1,n-1}+\epsilon_{n-1}.\\
|
||||
\end{align*}
|
||||
$$
|
||||
|
||||
We well use this matrix to define the approximation \( \hat{\tilde{y}} \) via the unknown quantity \( \hat{\beta} \) as
|
||||
$$
|
||||
\hat{\tilde{y}}= \hat{X}\hat{\beta},
|
||||
$$
|
||||
|
||||
and in order to find the optimal parameters \( \beta_i \) instead of solving the above linear algebra problem, we define a function which gives a measure of the spread between the values \( y_i \) (which represent hopefully the exact values) and the parametrized values \( \tilde{y}_i \), namely
|
||||
$$
|
||||
Q(\hat{\beta})=\sum_{i=0}^{n-1}\left(y_i-\tilde{y}_i\right)^2=\left(\hat{y}-\hat{\tilde{y}}\right)^T\left(\hat{y}-\hat{\tilde{y}}\right),
|
||||
$$
|
||||
|
||||
or using the matrix \( \hat{X} \) as
|
||||
$$
|
||||
Q(\hat{\beta})=\left(\hat{y}-\hat{X}\hat{\beta}\right)^T\left(\hat{y}-\hat{X}\hat{\beta}\right).
|
||||
$$
|
||||
</div>
|
||||
|
||||
|
||||
<p>
|
||||
<!-- !split --><br><br><br><br><br><br><br><br><br><br>
|
||||
|
||||
<h2 id="___sec5">Interpretations and optimizing our parameters </h2>
|
||||
<div class="alert alert-block alert-block alert-text-normal">
|
||||
<b></b>
|
||||
<p>
|
||||
The function
|
||||
$$
|
||||
Q(\hat{\beta})=\left(\hat{y}-\hat{X}\hat{\beta}\right)^T\left(\hat{y}-\hat{X}\hat{\beta}\right),
|
||||
$$
|
||||
|
||||
can be linked to the variance of the quantity \( y_i \) if we interpret the latter as the mean value of for example a numerical experiment. When linking below with the maximum likelihood approach below, we will indeed interpret \( y_i \) as a mean value
|
||||
$$
|
||||
y_{i}=\langle y_i \rangle = \beta_0x_{i,0}+\beta_1x_{i,1}+\beta_2x_{i,2}+\dots+\beta_{n-1}x_{i,n-1}+\epsilon_i,
|
||||
$$
|
||||
|
||||
where \( \langle y_i \rangle \) is the mean value. Keep in mind also that till now we have treated \( y_i \) as the exact value. Normally, the response (dependent or outcome) variable \( y_i \) the outcome of a numerical experiment or another type of experiment and is thus only an approximation to the true value. It is then always accompanied by an error estimate, often limited to a statistical error estimate given by the standard deviation discussed earlier. In the discussion here we will treat \( y_i \) as our exact value for the response variable.
|
||||
|
||||
<p>
|
||||
In order to find the parameters \( \beta_i \) we will then minimize the spread of \( Q(\hat{\beta}) \) by requiring
|
||||
$$
|
||||
\frac{\partial Q(\hat{\beta})}{\partial \beta_j} = \frac{\partial }{\partial \beta_j}\left[ \sum_{i=0}^{n-1}\left(y_i-\beta_0x_{i,0}+\beta_1x_{i,1}+\beta_2x_{i,2}+\dots+\beta_{n-1}x_{i,n-1}\right)^2\right]=0,
|
||||
$$
|
||||
|
||||
which results in
|
||||
$$
|
||||
\frac{\partial Q(\hat{\beta})}{\partial \beta_j} = -2\left[ \sum_{i=0}^{n-1}x_{ij}\left(y_i-\beta_0x_{i,0}+\beta_1x_{i,1}+\beta_2x_{i,2}+\dots+\beta_{n-1}x_{i,n-1}\right)\right]=0,
|
||||
$$
|
||||
|
||||
or in a matrix-vector form as
|
||||
$$
|
||||
\frac{\partial Q(\hat{\beta})}{\partial \hat{\beta}} = 0 = \hat{X}^T\left( \hat{y}-\hat{X}\hat{\beta}\right).
|
||||
$$
|
||||
|
||||
|
||||
</div>
|
||||
|
||||
|
||||
<p>
|
||||
<!-- !split --><br><br><br><br><br><br><br><br><br><br>
|
||||
|
||||
<h2 id="___sec6">Interpretations and optimizing our parameters </h2>
|
||||
<div class="alert alert-block alert-block alert-text-normal">
|
||||
<b></b>
|
||||
<p>
|
||||
We can rewrite
|
||||
$$
|
||||
\frac{\partial Q(\hat{\beta})}{\partial \hat{\beta}} = 0 = \hat{X}^T\left( \hat{y}-\hat{X}\hat{\beta}\right),
|
||||
$$
|
||||
|
||||
as
|
||||
$$
|
||||
\hat{X}^T\hat{y} = \hat{X}^T\hat{X}\hat{\beta},
|
||||
$$
|
||||
|
||||
and if the matrix \( \hat{X}^T\hat{X} \) is invertible we have the solution
|
||||
$$
|
||||
\hat{\beta} =\left(\hat{X}^T\hat{X}\right)^{-1}\hat{X}^T\hat{y}.
|
||||
$$
|
||||
|
||||
The residuals \( \hat{\epsilon} \) are in turn given by
|
||||
$$
|
||||
\hat{\epsilon} = \hat{y}-\hat{\tilde{y}} = \hat{y}-\hat{X}\hat{\beta},
|
||||
$$
|
||||
|
||||
and with
|
||||
$$
|
||||
\hat{X}^T\left( \hat{y}-\hat{X}\hat{\beta}\right)= 0,
|
||||
$$
|
||||
|
||||
we have
|
||||
$$
|
||||
\hat{X}^T\hat{\epsilon}=\hat{X}^T\left( \hat{y}-\hat{X}\hat{\beta}\right)= 0,
|
||||
$$
|
||||
|
||||
meaning that the solution for \( \hat{\beta} \) is the one which minimizes the residuals. Later we will link this with the maximum likelihood approach.
|
||||
|
||||
|
||||
</div>
|
||||
|
||||
|
||||
<p>
|
||||
<!-- !split --><br><br><br><br><br><br><br><br><br><br>
|
||||
|
||||
<h2 id="___sec7">The singular value decompostion </h2>
|
||||
<div class="alert alert-block alert-block alert-text-normal">
|
||||
<b></b>
|
||||
<p>
|
||||
Here we derive the equations for the SVD.
|
||||
</div>
|
||||
|
||||
|
||||
<p>
|
||||
|
||||
<!-- ------------------- end of main content --------------- -->
|
||||
|
||||
|
||||
|
||||
@@ -75,7 +75,16 @@ div { text-align: justify; text-justify: inter-word; }
|
||||
2,
|
||||
None,
|
||||
'___sec3'),
|
||||
('Optimizing our parameters', 2, None, '___sec4')]}
|
||||
('Optimizing our parameters', 2, None, '___sec4'),
|
||||
('Interpretations and optimizing our parameters',
|
||||
2,
|
||||
None,
|
||||
'___sec5'),
|
||||
('Interpretations and optimizing our parameters',
|
||||
2,
|
||||
None,
|
||||
'___sec6'),
|
||||
('The singular value decompostion', 2, None, '___sec7')]}
|
||||
end of tocinfo -->
|
||||
|
||||
<body>
|
||||
@@ -90,8 +99,8 @@ MathJax.Hub.Config({
|
||||
}
|
||||
});
|
||||
</script>
|
||||
<script type="text/javascript" async
|
||||
src="https://cdnjs.cloudflare.com/ajax/libs/mathjax/2.7.1/MathJax.js?config=TeX-AMS-MML_HTMLorMML">
|
||||
<script type="text/javascript"
|
||||
src="http://cdn.mathjax.org/mathjax/latest/MathJax.js?config=TeX-AMS-MML_HTMLorMML">
|
||||
</script>
|
||||
|
||||
|
||||
@@ -117,7 +126,7 @@ MathJax.Hub.Config({
|
||||
<center>[2] <b>Department of Physics and Astronomy and National Superconducting Cyclotron Laboratory, Michigan State University</b></center>
|
||||
<br>
|
||||
<p>
|
||||
<center><h4>Oct 14, 2017</h4></center> <!-- date -->
|
||||
<center><h4>Oct 17, 2017</h4></center> <!-- date -->
|
||||
<br>
|
||||
<p>
|
||||
<!-- !split --><br><br><br><br><br><br><br><br><br><br>
|
||||
@@ -172,19 +181,13 @@ where \( \epsilon_i \) is the error in our approximation.
|
||||
<p>
|
||||
For every set of values \( y_i,x_i \) we have thus the corresponding set of equations
|
||||
$$
|
||||
\begin{align}
|
||||
y_0&=\beta_0+\beta_1x_0^1+\beta_2x_0^2+\dots+\beta_{n-1}x_0^{n-1}+\epsilon_0
|
||||
\label{_auto1}\\
|
||||
y_1&=\beta_0+\beta_1x_1^1+\beta_2x_1^2+\dots+\beta_{n-1}x_1^{n-1}+\epsilon_1
|
||||
\label{_auto2}\\
|
||||
y_2&=\beta_0+\beta_1x_2^1+\beta_2x_2^2+\dots+\beta_{n-1}x_2^{n-1}+\epsilon_2
|
||||
\label{_auto3}\\
|
||||
\dots & \dots
|
||||
\label{_auto4}\\
|
||||
y_{n-1}&=\beta_0+\beta_1x_{n-1}^1+\beta_2x_{n-1}^2+\dots+\beta_1x_{n-1}^{n-1}+\epsilon_{n-1}.
|
||||
\label{_auto5}\\
|
||||
\label{_auto6}
|
||||
\end{align}
|
||||
\begin{align*}
|
||||
y_0&=\beta_0+\beta_1x_0^1+\beta_2x_0^2+\dots+\beta_{n-1}x_0^{n-1}+\epsilon_0\\
|
||||
y_1&=\beta_0+\beta_1x_1^1+\beta_2x_1^2+\dots+\beta_{n-1}x_1^{n-1}+\epsilon_1\\
|
||||
y_2&=\beta_0+\beta_1x_2^1+\beta_2x_2^2+\dots+\beta_{n-1}x_2^{n-1}+\epsilon_2\\
|
||||
\dots & \dots \\
|
||||
y_{n-1}&=\beta_0+\beta_1x_{n-1}^1+\beta_2x_{n-1}^2+\dots+\beta_1x_{n-1}^{n-1}+\epsilon_{n-1}.\\
|
||||
\end{align*}
|
||||
$$
|
||||
|
||||
Defining the vectors
|
||||
@@ -229,23 +232,15 @@ $$
|
||||
We are obviously not limited to the above polynomial. We could replace the various powers of \( x \) with elements of Fourier series, that is, instead of \( x_i^j \) we could have \( \cos{(j x_i)} \) or \( \sin{(j x_i)} \), or time series or other orthogonal functions.
|
||||
For every set of values \( y_i,x_i \) we can then generalize the equations to
|
||||
$$
|
||||
\begin{align}
|
||||
y_0&=\beta_0x_{00}+\beta_1x_{01}+\beta_2x_{02}+\dots+\beta_{n-1}x_{0n-1}+\epsilon_0
|
||||
\label{_auto7}\\
|
||||
y_1&=\beta_0x_{10}+\beta_1x_{11}+\beta_2x_{12}+\dots+\beta_{n-1}x_{1n-1}+\epsilon_1
|
||||
\label{_auto8}\\
|
||||
y_2&=\beta_0x_{20}+\beta_1x_{21}+\beta_2x_{22}+\dots+\beta_{n-1}x_{2n-1}+\epsilon_1
|
||||
\label{_auto9}\\
|
||||
\dots & \dots
|
||||
\label{_auto10}\\
|
||||
y_{i}&=\beta_0x_{i0}+\beta_1x_{i1}+\beta_2x_{i2}+\dots+\beta_{n-1}x_{in-1}+\epsilon_1
|
||||
\label{_auto11}\\
|
||||
\dots & \dots
|
||||
\label{_auto12}\\
|
||||
y_{n-1}&=\beta_0x_{n-1,0}+\beta_1x_{n-1,2}+\beta_2x_{n-1,2}+\dots+\beta_1x_{n-1}^{n-1,n-1}+\epsilon_{n-1}.
|
||||
\label{_auto13}\\
|
||||
\label{_auto14}
|
||||
\end{align}
|
||||
\begin{align*}
|
||||
y_0&=\beta_0x_{00}+\beta_1x_{01}+\beta_2x_{02}+\dots+\beta_{n-1}x_{0n-1}+\epsilon_0\\
|
||||
y_1&=\beta_0x_{10}+\beta_1x_{11}+\beta_2x_{12}+\dots+\beta_{n-1}x_{1n-1}+\epsilon_1\\
|
||||
y_2&=\beta_0x_{20}+\beta_1x_{21}+\beta_2x_{22}+\dots+\beta_{n-1}x_{2n-1}+\epsilon_2\\
|
||||
\dots & \dots \\
|
||||
y_{i}&=\beta_0x_{i0}+\beta_1x_{i1}+\beta_2x_{i2}+\dots+\beta_{n-1}x_{in-1}+\epsilon_i\\
|
||||
\dots & \dots \\
|
||||
y_{n-1}&=\beta_0x_{n-1,0}+\beta_1x_{n-1,2}+\beta_2x_{n-1,2}+\dots+\beta_1x_{n-1}^{n-1,n-1}+\epsilon_{n-1}.\\
|
||||
\end{align*}
|
||||
$$
|
||||
|
||||
We redefine in turn the matrix \( \hat{X} \) as
|
||||
@@ -276,28 +271,131 @@ The left-hand side of this equation forms know. Our error vector \( \hat{\epsilo
|
||||
<div class="alert alert-block alert-block alert-text-normal">
|
||||
<b></b>
|
||||
<p>
|
||||
We have defined the matrix \( \hat{X} \)
|
||||
$$
|
||||
\begin{align}
|
||||
y_0&=\beta_0x_{00}+\beta_1x_{01}+\beta_2x_{02}+\dots+\beta_{n-1}x_{0n-1}+\epsilon_0
|
||||
\label{_auto15}\\
|
||||
y_1&=\beta_0x_{10}+\beta_1x_{11}+\beta_2x_{12}+\dots+\beta_{n-1}x_{1n-1}+\epsilon_1
|
||||
\label{_auto16}\\
|
||||
y_2&=\beta_0x_{20}+\beta_1x_{21}+\beta_2x_{22}+\dots+\beta_{n-1}x_{2n-1}+\epsilon_1
|
||||
\label{_auto17}\\
|
||||
\dots & \dots
|
||||
\label{_auto18}\\
|
||||
y_{i}&=\beta_0x_{i0}+\beta_1x_{i1}+\beta_2x_{i2}+\dots+\beta_{n-1}x_{in-1}+\epsilon_1
|
||||
\label{_auto19}\\
|
||||
\dots & \dots
|
||||
\label{_auto20}\\
|
||||
y_{n-1}&=\beta_0x_{n-1,0}+\beta_1x_{n-1,2}+\beta_2x_{n-1,2}+\dots+\beta_1x_{n-1}^{n-1,n-1}+\epsilon_{n-1}.
|
||||
\label{_auto21}\\
|
||||
\label{_auto22}
|
||||
\end{align}
|
||||
\begin{align*}
|
||||
y_0&=\beta_0x_{00}+\beta_1x_{01}+\beta_2x_{02}+\dots+\beta_{n-1}x_{0n-1}+\epsilon_0\\
|
||||
y_1&=\beta_0x_{10}+\beta_1x_{11}+\beta_2x_{12}+\dots+\beta_{n-1}x_{1n-1}+\epsilon_1\\
|
||||
y_2&=\beta_0x_{20}+\beta_1x_{21}+\beta_2x_{22}+\dots+\beta_{n-1}x_{2n-1}+\epsilon_1\\
|
||||
\dots & \dots \\
|
||||
y_{i}&=\beta_0x_{i0}+\beta_1x_{i1}+\beta_2x_{i2}+\dots+\beta_{n-1}x_{in-1}+\epsilon_1\\
|
||||
\dots & \dots \\
|
||||
y_{n-1}&=\beta_0x_{n-1,0}+\beta_1x_{n-1,2}+\beta_2x_{n-1,2}+\dots+\beta_1x_{n-1,n-1}+\epsilon_{n-1}.\\
|
||||
\end{align*}
|
||||
$$
|
||||
|
||||
We well use this matrix to define the approximation \( \hat{\tilde{y}} \) via the unknown quantity \( \hat{\beta} \) as
|
||||
$$
|
||||
\hat{\tilde{y}}= \hat{X}\hat{\beta},
|
||||
$$
|
||||
|
||||
and in order to find the optimal parameters \( \beta_i \) instead of solving the above linear algebra problem, we define a function which gives a measure of the spread between the values \( y_i \) (which represent hopefully the exact values) and the parametrized values \( \tilde{y}_i \), namely
|
||||
$$
|
||||
Q(\hat{\beta})=\sum_{i=0}^{n-1}\left(y_i-\tilde{y}_i\right)^2=\left(\hat{y}-\hat{\tilde{y}}\right)^T\left(\hat{y}-\hat{\tilde{y}}\right),
|
||||
$$
|
||||
|
||||
or using the matrix \( \hat{X} \) as
|
||||
$$
|
||||
Q(\hat{\beta})=\left(\hat{y}-\hat{X}\hat{\beta}\right)^T\left(\hat{y}-\hat{X}\hat{\beta}\right).
|
||||
$$
|
||||
</div>
|
||||
|
||||
|
||||
<p>
|
||||
<!-- !split --><br><br><br><br><br><br><br><br><br><br>
|
||||
|
||||
<h2 id="___sec5">Interpretations and optimizing our parameters </h2>
|
||||
<div class="alert alert-block alert-block alert-text-normal">
|
||||
<b></b>
|
||||
<p>
|
||||
The function
|
||||
$$
|
||||
Q(\hat{\beta})=\left(\hat{y}-\hat{X}\hat{\beta}\right)^T\left(\hat{y}-\hat{X}\hat{\beta}\right),
|
||||
$$
|
||||
|
||||
can be linked to the variance of the quantity \( y_i \) if we interpret the latter as the mean value of for example a numerical experiment. When linking below with the maximum likelihood approach below, we will indeed interpret \( y_i \) as a mean value
|
||||
$$
|
||||
y_{i}=\langle y_i \rangle = \beta_0x_{i,0}+\beta_1x_{i,1}+\beta_2x_{i,2}+\dots+\beta_{n-1}x_{i,n-1}+\epsilon_i,
|
||||
$$
|
||||
|
||||
where \( \langle y_i \rangle \) is the mean value. Keep in mind also that till now we have treated \( y_i \) as the exact value. Normally, the response (dependent or outcome) variable \( y_i \) the outcome of a numerical experiment or another type of experiment and is thus only an approximation to the true value. It is then always accompanied by an error estimate, often limited to a statistical error estimate given by the standard deviation discussed earlier. In the discussion here we will treat \( y_i \) as our exact value for the response variable.
|
||||
|
||||
<p>
|
||||
In order to find the parameters \( \beta_i \) we will then minimize the spread of \( Q(\hat{\beta}) \) by requiring
|
||||
$$
|
||||
\frac{\partial Q(\hat{\beta})}{\partial \beta_j} = \frac{\partial }{\partial \beta_j}\left[ \sum_{i=0}^{n-1}\left(y_i-\beta_0x_{i,0}+\beta_1x_{i,1}+\beta_2x_{i,2}+\dots+\beta_{n-1}x_{i,n-1}\right)^2\right]=0,
|
||||
$$
|
||||
|
||||
which results in
|
||||
$$
|
||||
\frac{\partial Q(\hat{\beta})}{\partial \beta_j} = -2\left[ \sum_{i=0}^{n-1}x_{ij}\left(y_i-\beta_0x_{i,0}+\beta_1x_{i,1}+\beta_2x_{i,2}+\dots+\beta_{n-1}x_{i,n-1}\right)\right]=0,
|
||||
$$
|
||||
|
||||
or in a matrix-vector form as
|
||||
$$
|
||||
\frac{\partial Q(\hat{\beta})}{\partial \hat{\beta}} = 0 = \hat{X}^T\left( \hat{y}-\hat{X}\hat{\beta}\right).
|
||||
$$
|
||||
|
||||
|
||||
</div>
|
||||
|
||||
|
||||
<p>
|
||||
<!-- !split --><br><br><br><br><br><br><br><br><br><br>
|
||||
|
||||
<h2 id="___sec6">Interpretations and optimizing our parameters </h2>
|
||||
<div class="alert alert-block alert-block alert-text-normal">
|
||||
<b></b>
|
||||
<p>
|
||||
We can rewrite
|
||||
$$
|
||||
\frac{\partial Q(\hat{\beta})}{\partial \hat{\beta}} = 0 = \hat{X}^T\left( \hat{y}-\hat{X}\hat{\beta}\right),
|
||||
$$
|
||||
|
||||
as
|
||||
$$
|
||||
\hat{X}^T\hat{y} = \hat{X}^T\hat{X}\hat{\beta},
|
||||
$$
|
||||
|
||||
and if the matrix \( \hat{X}^T\hat{X} \) is invertible we have the solution
|
||||
$$
|
||||
\hat{\beta} =\left(\hat{X}^T\hat{X}\right)^{-1}\hat{X}^T\hat{y}.
|
||||
$$
|
||||
|
||||
The residuals \( \hat{\epsilon} \) are in turn given by
|
||||
$$
|
||||
\hat{\epsilon} = \hat{y}-\hat{\tilde{y}} = \hat{y}-\hat{X}\hat{\beta},
|
||||
$$
|
||||
|
||||
and with
|
||||
$$
|
||||
\hat{X}^T\left( \hat{y}-\hat{X}\hat{\beta}\right)= 0,
|
||||
$$
|
||||
|
||||
we have
|
||||
$$
|
||||
\hat{X}^T\hat{\epsilon}=\hat{X}^T\left( \hat{y}-\hat{X}\hat{\beta}\right)= 0,
|
||||
$$
|
||||
|
||||
meaning that the solution for \( \hat{\beta} \) is the one which minimizes the residuals. Later we will link this with the maximum likelihood approach.
|
||||
|
||||
|
||||
</div>
|
||||
|
||||
|
||||
<p>
|
||||
<!-- !split --><br><br><br><br><br><br><br><br><br><br>
|
||||
|
||||
<h2 id="___sec7">The singular value decompostion </h2>
|
||||
<div class="alert alert-block alert-block alert-text-normal">
|
||||
<b></b>
|
||||
<p>
|
||||
Here we derive the equations for the SVD.
|
||||
</div>
|
||||
|
||||
|
||||
<p>
|
||||
|
||||
<!-- ------------------- end of main content --------------- -->
|
||||
|
||||
|
||||
|
||||
Binary file not shown.
Binary file not shown.
Binary file not shown.
Binary file not shown.
@@ -37,13 +37,13 @@ where $\epsilon_i$ is the error in our approximation.
|
||||
!bblock
|
||||
For every set of values $y_i,x_i$ we have thus the corresponding set of equations
|
||||
!bt
|
||||
\begin{align}
|
||||
\begin{align*}
|
||||
y_0&=\beta_0+\beta_1x_0^1+\beta_2x_0^2+\dots+\beta_{n-1}x_0^{n-1}+\epsilon_0\\
|
||||
y_1&=\beta_0+\beta_1x_1^1+\beta_2x_1^2+\dots+\beta_{n-1}x_1^{n-1}+\epsilon_1\\
|
||||
y_2&=\beta_0+\beta_1x_2^1+\beta_2x_2^2+\dots+\beta_{n-1}x_2^{n-1}+\epsilon_2\\
|
||||
\dots & \dots \\
|
||||
y_{n-1}&=\beta_0+\beta_1x_{n-1}^1+\beta_2x_{n-1}^2+\dots+\beta_1x_{n-1}^{n-1}+\epsilon_{n-1}.\\
|
||||
\end{align}
|
||||
\end{align*}
|
||||
!et
|
||||
Defining the vectors
|
||||
!bt
|
||||
@@ -89,7 +89,7 @@ we can rewrite our equations as
|
||||
We are obviously not limited to the above polynomial. We could replace the various powers of $x$ with elements of Fourier series, that is, instead of $x_i^j$ we could have $\cos{(j x_i)}$ or $\sin{(j x_i)}$, or time series or other orthogonal functions.
|
||||
For every set of values $y_i,x_i$ we can then generalize the equations to
|
||||
!bt
|
||||
\begin{align}
|
||||
\begin{align*}
|
||||
y_0&=\beta_0x_{00}+\beta_1x_{01}+\beta_2x_{02}+\dots+\beta_{n-1}x_{0n-1}+\epsilon_0\\
|
||||
y_1&=\beta_0x_{10}+\beta_1x_{11}+\beta_2x_{12}+\dots+\beta_{n-1}x_{1n-1}+\epsilon_1\\
|
||||
y_2&=\beta_0x_{20}+\beta_1x_{21}+\beta_2x_{22}+\dots+\beta_{n-1}x_{2n-1}+\epsilon_2\\
|
||||
@@ -97,7 +97,7 @@ y_2&=\beta_0x_{20}+\beta_1x_{21}+\beta_2x_{22}+\dots+\beta_{n-1}x_{2n-1}+\epsilo
|
||||
y_{i}&=\beta_0x_{i0}+\beta_1x_{i1}+\beta_2x_{i2}+\dots+\beta_{n-1}x_{in-1}+\epsilon_i\\
|
||||
\dots & \dots \\
|
||||
y_{n-1}&=\beta_0x_{n-1,0}+\beta_1x_{n-1,2}+\beta_2x_{n-1,2}+\dots+\beta_1x_{n-1}^{n-1,n-1}+\epsilon_{n-1}.\\
|
||||
\end{align}
|
||||
\end{align*}
|
||||
!et
|
||||
We redefine in turn the matrix $\hat{X}$ as
|
||||
!bt
|
||||
@@ -127,7 +127,7 @@ The left-hand side of this equation forms know. Our error vector $\hat{\epsilon}
|
||||
!bblock
|
||||
We have defined the matrix $\hat{X}$
|
||||
!bt
|
||||
\begin{align}
|
||||
\begin{align*}
|
||||
y_0&=\beta_0x_{00}+\beta_1x_{01}+\beta_2x_{02}+\dots+\beta_{n-1}x_{0n-1}+\epsilon_0\\
|
||||
y_1&=\beta_0x_{10}+\beta_1x_{11}+\beta_2x_{12}+\dots+\beta_{n-1}x_{1n-1}+\epsilon_1\\
|
||||
y_2&=\beta_0x_{20}+\beta_1x_{21}+\beta_2x_{22}+\dots+\beta_{n-1}x_{2n-1}+\epsilon_1\\
|
||||
@@ -135,7 +135,7 @@ y_2&=\beta_0x_{20}+\beta_1x_{21}+\beta_2x_{22}+\dots+\beta_{n-1}x_{2n-1}+\epsilo
|
||||
y_{i}&=\beta_0x_{i0}+\beta_1x_{i1}+\beta_2x_{i2}+\dots+\beta_{n-1}x_{in-1}+\epsilon_1\\
|
||||
\dots & \dots \\
|
||||
y_{n-1}&=\beta_0x_{n-1,0}+\beta_1x_{n-1,2}+\beta_2x_{n-1,2}+\dots+\beta_1x_{n-1,n-1}+\epsilon_{n-1}.\\
|
||||
\end{align}
|
||||
\end{align*}
|
||||
!et
|
||||
We well use this matrix to define the approximation $\hat{\tilde{y}}$ via the unknown quantity $\hat{\beta}$ as
|
||||
!bt
|
||||
@@ -146,13 +146,13 @@ We well use this matrix to define the approximation $\hat{\tilde{y}}$ via the un
|
||||
and in order to find the optimal parameters $\beta_i$ instead of solving the above linear algebra problem, we define a function which gives a measure of the spread between the values $y_i$ (which represent hopefully the exact values) and the parametrized values $\tilde{y}_i$, namely
|
||||
!bt
|
||||
\[
|
||||
Q(\hat{\beta})=\sum_{i=0}^{n-1}\left(y_i-\tilde{y}_i\right)^2=\left \hat{y}-\hat{\tilde{y}}\right)^T\left \hat{y}-\hat{\tilde{y}}\right),
|
||||
Q(\hat{\beta})=\sum_{i=0}^{n-1}\left(y_i-\tilde{y}_i\right)^2=\left(\hat{y}-\hat{\tilde{y}}\right)^T\left(\hat{y}-\hat{\tilde{y}}\right),
|
||||
\]
|
||||
!et
|
||||
or using the matrix $\hat{X}$ as
|
||||
!bt
|
||||
\[
|
||||
Q(\hat{\beta})=\left \hat{y}-\hat{X}\hat{\beta}\right)^T\left \hat{y}-\hat{X}\hat{\beta}\right).
|
||||
Q(\hat{\beta})=\left(\hat{y}-\hat{X}\hat{\beta}\right)^T\left(\hat{y}-\hat{X}\hat{\beta}\right).
|
||||
\]
|
||||
!et
|
||||
!eblock
|
||||
@@ -164,7 +164,7 @@ Q(\hat{\beta})=\left \hat{y}-\hat{X}\hat{\beta}\right)^T\left \hat{y}-\hat{X}\ha
|
||||
The function
|
||||
!bt
|
||||
\[
|
||||
Q(\hat{\beta})=\left \hat{y}-\hat{X}\hat{\beta}\right)^T\left \hat{y}-\hat{X}\hat{\beta}\right),
|
||||
Q(\hat{\beta})=\left(\hat{y}-\hat{X}\hat{\beta}\right)^T\left(\hat{y}-\hat{X}\hat{\beta}\right),
|
||||
\]
|
||||
!et
|
||||
can be linked to the variance of the quantity $y_i$ if we interpret the latter as the mean value of for example a numerical experiment. When linking below with the maximum likelihood approach below, we will indeed interpret $y_i$ as a mean value
|
||||
@@ -178,7 +178,7 @@ where $\langle y_i \rangle$ is the mean value. Keep in mind also that till now
|
||||
In order to find the parameters $\beta_i$ we will then minimize the spread of $Q(\hat{\beta})$ by requiring
|
||||
!bt
|
||||
\[
|
||||
\frac{\partial Q(\hat{\beta})}{\partial \beta_j} = \frac{ }{\partial \beta_j}\left[ \sum_{i=0}^{n-1}\left(y_i-\beta_0x_{i,0}+\beta_1x_{i,1}+\beta_2x_{i,2}+\dots+\beta_{n-1}x_{i,n-1}\right)^2\right]=0,
|
||||
\frac{\partial Q(\hat{\beta})}{\partial \beta_j} = \frac{\partial }{\partial \beta_j}\left[ \sum_{i=0}^{n-1}\left(y_i-\beta_0x_{i,0}+\beta_1x_{i,1}+\beta_2x_{i,2}+\dots+\beta_{n-1}x_{i,n-1}\right)^2\right]=0,
|
||||
\]
|
||||
!et
|
||||
which results in
|
||||
@@ -196,3 +196,56 @@ or in a matrix-vector form as
|
||||
|
||||
|
||||
!eblock
|
||||
|
||||
|
||||
!split
|
||||
===== Interpretations and optimizing our parameters =====
|
||||
!bblock
|
||||
We can rewrite
|
||||
!bt
|
||||
\[
|
||||
\frac{\partial Q(\hat{\beta})}{\partial \hat{\beta}} = 0 = \hat{X}^T\left( \hat{y}-\hat{X}\hat{\beta}\right),
|
||||
\]
|
||||
!et
|
||||
as
|
||||
!bt
|
||||
\[
|
||||
\hat{X}^T\hat{y} = \hat{X}^T\hat{X}\hat{\beta},
|
||||
\]
|
||||
!et
|
||||
and if the matrix $\hat{X}^T\hat{X}$ is invertible we have the solution
|
||||
!bt
|
||||
\[
|
||||
\hat{\beta} =\left(\hat{X}^T\hat{X}\right)^{-1}\hat{X}^T\hat{y}.
|
||||
\]
|
||||
!et
|
||||
The residuals $\hat{\epsilon}$ are in turn given by
|
||||
!bt
|
||||
\[
|
||||
\hat{\epsilon} = \hat{y}-\hat{\tilde{y}} = \hat{y}-\hat{X}\hat{\beta},
|
||||
\]
|
||||
!et
|
||||
and with
|
||||
!bt
|
||||
\[
|
||||
\hat{X}^T\left( \hat{y}-\hat{X}\hat{\beta}\right)= 0,
|
||||
\]
|
||||
!et
|
||||
we have
|
||||
!bt
|
||||
\[
|
||||
\hat{X}^T\hat{\epsilon}=\hat{X}^T\left( \hat{y}-\hat{X}\hat{\beta}\right)= 0,
|
||||
\]
|
||||
!et
|
||||
meaning that the solution for $\hat{\beta}$ is the one which minimizes the residuals. Later we will link this with the maximum likelihood approach.
|
||||
|
||||
!eblock
|
||||
|
||||
|
||||
!split
|
||||
===== The singular value decompostion =====
|
||||
!bblock
|
||||
Here we derive the equations for the SVD.
|
||||
!eblock
|
||||
|
||||
|
||||
|
||||
Reference in New Issue
Block a user