adding update to regression slides
This commit is contained in:
@@ -405,7 +405,7 @@ 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>Aug 21, 2019</h4></center> <!-- date -->
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<center><h4>Aug 27, 2019</h4></center> <!-- date -->
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<br>
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<p>
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@@ -398,10 +398,15 @@ The examples we have looked at so far are cases where we normally can
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invert the matrix \( \boldsymbol{X}^T\boldsymbol{X} \). Using a polynomial expansion as we
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did both for the masses and the fitting of the equation of state,
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leads to row vectors of the design matrix which are essentially
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orthogonal due to the polynomial character of our model. This may
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orthogonal due to the polynomial character of our model. Obtaining the inverse of the design matrix is then often done via a so-called LU, QR or Cholesky decomposition.
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More material to come here.
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<p>
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This may
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however not the be case in general and a standard matrix inversion
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algorithm based on say LU decomposition may lead to singularities. We will see an example of this below when we try to fit
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the coupling constant of the widely used Ising model.
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algorithm based on say LU, QR or Cholesky decomposition may lead to singularities. We will see examples of this below.
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<p>
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There is however a way to partially circumvent this problem and also gain some insight about the ordinary least squares approach.
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<p>
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@@ -415,6 +420,9 @@ inversion algorithm. Thereafter we dive into the math of the SVD.
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</div>
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<p>
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<!-- todo: change model here. -->
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<p>
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<p>
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<!-- navigation buttons at the bottom of the page -->
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@@ -405,7 +405,7 @@ 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>Aug 21, 2019</h4></center> <!-- date -->
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<center><h4>Aug 27, 2019</h4></center> <!-- date -->
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<br>
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<p>
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@@ -148,7 +148,7 @@ 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> <br>
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<center><h4>Aug 21, 2019</h4></center> <!-- date -->
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<center><h4>Aug 27, 2019</h4></center> <!-- date -->
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<br>
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<p>
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@@ -1300,10 +1300,15 @@ The examples we have looked at so far are cases where we normally can
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invert the matrix \( \boldsymbol{X}^T\boldsymbol{X} \). Using a polynomial expansion as we
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did both for the masses and the fitting of the equation of state,
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leads to row vectors of the design matrix which are essentially
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orthogonal due to the polynomial character of our model. This may
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orthogonal due to the polynomial character of our model. Obtaining the inverse of the design matrix is then often done via a so-called LU, QR or Cholesky decomposition.
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More material to come here.
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<p>
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This may
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however not the be case in general and a standard matrix inversion
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algorithm based on say LU decomposition may lead to singularities. We will see an example of this below when we try to fit
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the coupling constant of the widely used Ising model.
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algorithm based on say LU, QR or Cholesky decomposition may lead to singularities. We will see examples of this below.
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<p>
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There is however a way to partially circumvent this problem and also gain some insight about the ordinary least squares approach.
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<p>
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@@ -1314,6 +1319,9 @@ inversion algorithm. Thereafter we dive into the math of the SVD.
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</div>
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<p>
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<!-- todo: change model here. -->
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</section>
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@@ -291,7 +291,7 @@ 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>Aug 21, 2019</h4></center> <!-- date -->
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<center><h4>Aug 27, 2019</h4></center> <!-- date -->
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<br>
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<p>
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<!-- !split --><br><br><br><br><br><br><br><br><br><br>
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@@ -1368,10 +1368,15 @@ The examples we have looked at so far are cases where we normally can
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invert the matrix \( \boldsymbol{X}^T\boldsymbol{X} \). Using a polynomial expansion as we
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did both for the masses and the fitting of the equation of state,
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leads to row vectors of the design matrix which are essentially
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orthogonal due to the polynomial character of our model. This may
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orthogonal due to the polynomial character of our model. Obtaining the inverse of the design matrix is then often done via a so-called LU, QR or Cholesky decomposition.
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More material to come here.
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<p>
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This may
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however not the be case in general and a standard matrix inversion
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algorithm based on say LU decomposition may lead to singularities. We will see an example of this below when we try to fit
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the coupling constant of the widely used Ising model.
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algorithm based on say LU, QR or Cholesky decomposition may lead to singularities. We will see examples of this below.
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<p>
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There is however a way to partially circumvent this problem and also gain some insight about the ordinary least squares approach.
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<p>
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@@ -1384,6 +1389,9 @@ inversion algorithm. Thereafter we dive into the math of the SVD.
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</div>
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<p>
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<!-- todo: change model here. -->
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<p>
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<!-- !split --><br><br><br><br><br><br><br><br><br><br>
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@@ -296,7 +296,7 @@ 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>Aug 21, 2019</h4></center> <!-- date -->
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<center><h4>Aug 27, 2019</h4></center> <!-- date -->
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<br>
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<p>
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<!-- !split --><br><br><br><br><br><br><br><br><br><br>
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@@ -1373,10 +1373,15 @@ The examples we have looked at so far are cases where we normally can
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invert the matrix \( \boldsymbol{X}^T\boldsymbol{X} \). Using a polynomial expansion as we
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did both for the masses and the fitting of the equation of state,
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leads to row vectors of the design matrix which are essentially
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orthogonal due to the polynomial character of our model. This may
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orthogonal due to the polynomial character of our model. Obtaining the inverse of the design matrix is then often done via a so-called LU, QR or Cholesky decomposition.
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More material to come here.
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<p>
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This may
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however not the be case in general and a standard matrix inversion
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algorithm based on say LU decomposition may lead to singularities. We will see an example of this below when we try to fit
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the coupling constant of the widely used Ising model.
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algorithm based on say LU, QR or Cholesky decomposition may lead to singularities. We will see examples of this below.
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<p>
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There is however a way to partially circumvent this problem and also gain some insight about the ordinary least squares approach.
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<p>
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@@ -1389,6 +1394,9 @@ inversion algorithm. Thereafter we dive into the math of the SVD.
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</div>
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<p>
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<!-- todo: change model here. -->
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<p>
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<!-- !split --><br><br><br><br><br><br><br><br><br><br>
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@@ -974,10 +974,14 @@ The examples we have looked at so far are cases where we normally can
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invert the matrix $\bm{X}^T\bm{X}$. Using a polynomial expansion as we
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did both for the masses and the fitting of the equation of state,
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leads to row vectors of the design matrix which are essentially
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orthogonal due to the polynomial character of our model. This may
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orthogonal due to the polynomial character of our model. Obtaining the inverse of the design matrix is then often done via a so-called LU, QR or Cholesky decomposition.
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More material to come here.
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This may
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however not the be case in general and a standard matrix inversion
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algorithm based on say LU decomposition may lead to singularities. We will see an example of this below when we try to fit
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the coupling constant of the widely used Ising model.
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algorithm based on say LU, QR or Cholesky decomposition may lead to singularities. We will see examples of this below.
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There is however a way to partially circumvent this problem and also gain some insight about the ordinary least squares approach.
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This is given by the _Singular Value Decomposition_ algorithm, perhaps
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@@ -987,6 +991,9 @@ inversion algorithm. Thereafter we dive into the math of the SVD.
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!eblock
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# todo: change model here.
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!split
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===== The Ising model =====
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