diff --git a/doc/pub/week39/html/week39-bs.html b/doc/pub/week39/html/week39-bs.html index 746b595ba..65aa91964 100644 --- a/doc/pub/week39/html/week39-bs.html +++ b/doc/pub/week39/html/week39-bs.html @@ -59,6 +59,7 @@ Automatically generated HTML file from DocOnce source None, 'revisiting-our-logistic-regression-case'), ('The equations to solve', 2, None, 'the-equations-to-solve'), + ('To be added', 2, None, 'to-be-added'), ("Solving using Newton-Raphson's method", 2, None, @@ -223,53 +224,54 @@ MathJax.Hub.Config({
-
@@ -328,7 +330,7 @@ MathJax.Hub.Config({
-
@@ -241,7 +241,7 @@ plt.legend() plt.show()
-Here we have performed a rather data greedy calculation as function of the regularization parameter \( \lambda \). There is no resampling here. The latter can easily be added by employing the function RidgeCV instead of just calling the Ridge function. For RidgeCV we need to passe the array of \( \lambda \) values. +Here we have performed a rather data greedy calculation as function of the regularization parameter \( \lambda \). There is no resampling here. The latter can easily be added by employing the function RidgeCV instead of just calling the Ridge function. For RidgeCV we need to pass the array of \( \lambda \) values. By inspecting the figure we can in turn determine which is the optimal regularization parameter. This becomes however less functional in the long run. @@ -302,7 +302,10 @@ ypredictRidge = gridsearch.predict(X_test) print(f"R2 score: {R2(y_test,ypredictRidge)}")
-By default the grid search function includes cross validation with five folds. The Scikit-Learn documentation contains more information on how to set the different parameters. +By default the grid search function includes cross validation with +five folds. The Scikit-Learn +documentation +contains more information on how to set the different parameters.
If we take out the random noise, running the above codes results in \( \lambda=0 \) yielding the best fit. @@ -317,7 +320,10 @@ An alternative to the above manual grid set up, is to use a random search where the parameters are tuned from a random distribution (uniform below) for a fixed number of iterations. A model is constructed and evaluated for each combination of chosen parameters. -We repeat the previous example but now with a random search. +We repeat the previous example but now with a random search. Note +that values of \( \lambda \) are now limited to be within \( x\in +[0,1] \). This domain may not be the most relevant one for the specific +case under study.
@@ -438,6 +444,17 @@ This defines what is called the Hessian matrix.
+
+We will add here an example which computes the likelihood \( p_i \), sets up the gradient and the Hessian matrix.
+
+
+Make link with linear regression and the Hessian matrix from linear regression.
+
-
-Here we have performed a rather data greedy calculation as function of the regularization parameter \( \lambda \). There is no resampling here. The latter can easily be added by employing the function RidgeCV instead of just calling the Ridge function. For RidgeCV we need to passe the array of \( \lambda \) values.
+Here we have performed a rather data greedy calculation as function of the regularization parameter \( \lambda \). There is no resampling here. The latter can easily be added by employing the function RidgeCV instead of just calling the Ridge function. For RidgeCV we need to pass the array of \( \lambda \) values.
By inspecting the figure we can in turn determine which is the optimal regularization parameter.
This becomes however less functional in the long run.
@@ -386,7 +387,10 @@ ypredictRidge = gridsearch.predict(X_test)
print(f"R2 score: {R2(y_test,ypredictRidge)}")
-By default the grid search function includes cross validation with five folds. The Scikit-Learn documentation contains more information on how to set the different parameters.
+By default the grid search function includes cross validation with
+five folds. The Scikit-Learn
+documentation
+contains more information on how to set the different parameters.
If we take out the random noise, running the above codes results in \( \lambda=0 \) yielding the best fit.
@@ -401,7 +405,10 @@ An alternative to the above manual grid set up, is to use a random
search where the parameters are tuned from a random distribution
(uniform below) for a fixed number of iterations. A model is
constructed and evaluated for each combination of chosen parameters.
-We repeat the previous example but now with a random search.
+We repeat the previous example but now with a random search. Note
+that values of \( \lambda \) are now limited to be within \( x\in
+[0,1] \). This domain may not be the most relevant one for the specific
+case under study.
@@ -516,6 +523,17 @@ This defines what is called the Hessian matrix.
+We will add here an example which computes the likelihood \( p_i \), sets up the gradient and the Hessian matrix.
+
+
+Make link with linear regression and the Hessian matrix from linear regression.
+
+
+
diff --git a/doc/pub/week39/html/week39.html b/doc/pub/week39/html/week39.html
index 6c91bc434..ed2405a4a 100644
--- a/doc/pub/week39/html/week39.html
+++ b/doc/pub/week39/html/week39.html
@@ -84,6 +84,7 @@ div { text-align: justify; text-justify: inter-word; }
None,
'revisiting-our-logistic-regression-case'),
('The equations to solve', 2, None, 'the-equations-to-solve'),
+ ('To be added', 2, None, 'to-be-added'),
("Solving using Newton-Raphson's method",
2,
None,
@@ -244,7 +245,7 @@ MathJax.Hub.Config({
-
-Here we have performed a rather data greedy calculation as function of the regularization parameter \( \lambda \). There is no resampling here. The latter can easily be added by employing the function RidgeCV instead of just calling the Ridge function. For RidgeCV we need to passe the array of \( \lambda \) values.
+Here we have performed a rather data greedy calculation as function of the regularization parameter \( \lambda \). There is no resampling here. The latter can easily be added by employing the function RidgeCV instead of just calling the Ridge function. For RidgeCV we need to pass the array of \( \lambda \) values.
By inspecting the figure we can in turn determine which is the optimal regularization parameter.
This becomes however less functional in the long run.
@@ -391,7 +392,10 @@ ypredictRidge = gridsearchprint(f"R2 score: {R2(y_test,ypredictRidge)}")
-By default the grid search function includes cross validation with five folds. The Scikit-Learn documentation contains more information on how to set the different parameters.
+By default the grid search function includes cross validation with
+five folds. The Scikit-Learn
+documentation
+contains more information on how to set the different parameters.
If we take out the random noise, running the above codes results in \( \lambda=0 \) yielding the best fit.
@@ -406,7 +410,10 @@ An alternative to the above manual grid set up, is to use a random
search where the parameters are tuned from a random distribution
(uniform below) for a fixed number of iterations. A model is
constructed and evaluated for each combination of chosen parameters.
-We repeat the previous example but now with a random search.
+We repeat the previous example but now with a random search. Note
+that values of \( \lambda \) are now limited to be within \( x\in
+[0,1] \). This domain may not be the most relevant one for the specific
+case under study.
@@ -521,6 +528,17 @@ This defines what is called the Hessian matrix.
+We will add here an example which computes the likelihood \( p_i \), sets up the gradient and the Hessian matrix.
+
+
+Make link with linear regression and the Hessian matrix from linear regression.
+
+
+
diff --git a/doc/pub/week39/ipynb/ipynb-week39-src.tar.gz b/doc/pub/week39/ipynb/ipynb-week39-src.tar.gz
index 2d12ed541..4f2bb3bb6 100644
Binary files a/doc/pub/week39/ipynb/ipynb-week39-src.tar.gz and b/doc/pub/week39/ipynb/ipynb-week39-src.tar.gz differ
diff --git a/doc/pub/week39/ipynb/week39.ipynb b/doc/pub/week39/ipynb/week39.ipynb
index 6e9d11a8c..2d9c9b2dd 100644
--- a/doc/pub/week39/ipynb/week39.ipynb
+++ b/doc/pub/week39/ipynb/week39.ipynb
@@ -10,7 +10,7 @@
" \n",
"**Morten Hjorth-Jensen**, Department of Physics, University of Oslo and Department of Physics and Astronomy and National Superconducting Cyclotron Laboratory, Michigan State University\n",
"\n",
- "Date: **Sep 28, 2021**\n",
+ "Date: **Sep 29, 2021**\n",
"\n",
"Copyright 1999-2021, Morten Hjorth-Jensen. Released under CC Attribution-NonCommercial 4.0 license\n",
"\n",
@@ -45,22 +45,12 @@
},
{
"cell_type": "code",
- "execution_count": 11,
- "metadata": {},
- "outputs": [
- {
- "data": {
- "image/png": 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\n",
- "text/plain": [
- "To be added
+
+Solving using Newton-Raphson's method
diff --git a/doc/pub/week39/html/week39-solarized.html b/doc/pub/week39/html/week39-solarized.html
index 7dc0d0002..458978331 100644
--- a/doc/pub/week39/html/week39-solarized.html
+++ b/doc/pub/week39/html/week39-solarized.html
@@ -79,6 +79,7 @@ div { text-align: justify; text-justify: inter-word; }
None,
'revisiting-our-logistic-regression-case'),
('The equations to solve', 2, None, 'the-equations-to-solve'),
+ ('To be added', 2, None, 'to-be-added'),
("Solving using Newton-Raphson's method",
2,
None,
@@ -239,7 +240,7 @@ MathJax.Hub.Config({
Sep 28, 2021
Sep 29, 2021
@@ -325,7 +326,7 @@ plt.legend()
plt.show()
+To be added
+
+
+
Solving using Newton-Raphson's method
Sep 28, 2021
Sep 29, 2021
@@ -330,7 +331,7 @@ plt.legend()
plt.show()
+To be added
+
+
+
Solving using Newton-Raphson's method