small typos
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@@ -52,7 +52,7 @@ The theory behind support vector machines (SVM hereafter) is based on
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the mathematical description of so-called hyperplanes. Let us start
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with a two-dimensional case. This will also allow us to introduce our
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first SVM examples. These will be tailored to the case of two specific
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classes, as displayed in the figure here based on the usage of the petal data.
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classes, as displayed in the figure here based on the usage of the petal data.
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We assume here that our data set can be well separated into two
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domains, where a straight line does the job in the separating the two
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@@ -561,7 +561,10 @@ Below we discuss how to find the optimal values of $\lambda_i$. Before we procee
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Till now, the margin is strictly defined by the support vectors. This defines what is called a hard classifier, that is the margins are well defined.
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Suppose now that classes overlap in feature space, as shown in the
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figure here. One way to deal with this problem before we define the
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figure in the "handwritten notes":"https://github.com/CompPhysics/MachineLearning/tree/master/doc/HandWrittenNotes/2021" for Thursday November 25.
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One way to deal with this problem before we define the
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so-called _kernel approach_, is to allow a kind of slack in the sense
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that we allow some points to be on the wrong side of the margin.
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@@ -658,8 +661,9 @@ space using other basis expansions such as higher-order polynomials,
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wavelets, splines etc.
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If our feature space is not easy to separate, as shown in the figure
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here, we can achieve a better separation by introducing more complex
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basis functions. The ideal would be, as shown in the next figure, to, via a specific transformation to
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in the "handwritten notes":"https://github.com/CompPhysics/MachineLearning/tree/master/doc/HandWrittenNotes/2021" for Thursday November 25.
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, we can achieve a better separation by introducing more complex
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basis functions. The ideal would be to, via a specific transformation to
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obtain a separation between the classes which is almost linear.
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The change of basis, from $x\rightarrow z=\phi(x)$ leads to the same type of equations to be solved, except that
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