Matthieu Bloch
Tuesday November 22, 2022
A space is separable if it contains a countable dense subset.
Separability is the key property to deal with sequences instead of collections
Any separable Hilbert space has an orthonormal basis.
Most useful Hilbert spaces are separable! We won't worry about non-separable Hilbert spaces
Key take away for separable Hilbert spaces
Any separable Hilbert space is isomorphic to \(\ell_2\)
A functional \(F:\calF\to\bbR\) associates real-valued number to an element of a Hilbert space \(\calF\)
A functional \(F:\calF\to\bbR\) is continuous at \(x\in\calF\) if \[ \forall \epsilon>0\exists\delta>0\textsf{ such that } \norm[\calF]{x-y}\leq \delta\Rightarrow \abs{F(x)-F(y)}\leq\epsilon \] If this is true for every \(x\in\calF\), \(F\) is continuous.
A functional \(F\) is linear if \(\forall a,b\in\bbR\) \(\forall x,y\in\calF\) \(F(ax+by) = aF(x)+bF(y)\).
Continuous linear functions are much more constrained than one would imagine
A linear functional \(F:\calF\to\bbR\) is bounded if there exists \(M>0\) such that \[ \forall x\in\calF\quad\abs{F(x)}\leq M\norm[\calF]{x} \]
A linear functional on a Hilbert space that is countinuous at \(0\) is bounded.
Let \(F:\calF\to\bbR\) be a linear functional on an \(n\)-dimensional Hilbert space \(\calF\).
Then there exists \(c\in\calF\) such that \(F(x)=\dotp{x}{c}\) for every \(x\in\calF\)
Linear functional over finite dimensional Hilbert spaces are continuous!
This is not true in infinite dimension
Let \(F:\calF\to\bbR\) be a continuous linear functional on a (possible infinite dimensional) separable Hilbert space \(\calF\).
Then there exists \(c\in\calF\) such that \(F(x)=\dotp{x}{c}\) for every \(x\in\calF\)
If \(\set{\psi_n}_{n\geq 1}\) is an orthobasis for \(\calF\), then we can construct \(c\) above as \[ c\eqdef \sum_{n=1}^\infty F(\psi_n)\psi_n \]
An RKHS is a Hilbert space \(\calH\) of real-valued functions \(f:\bbR^d\to\bbR\) in which the sampling operation \(\calS_\bftau:\calH\to\bbR:f\mapsto f(\bftau)\) is continuous for every \(\bftau\in\bbR^d\).
In other words, for each \(\bftau\in\bbR^d\), there exists \(k_\bftau\in\calH\) s.t. \[ f(\bftau) = {\dotp{f}{k_\bftau}}_\calH\text{ for all } f\in\calH \]
The kernel of an RKHS is \[ k:\bbR^d\times\bbR^d\to\bbR:(\bft,\bftau)\mapsto k_{\bftau}(\bft) \] where \(k_\bftau\) is the element of \(\calH\) that defines the sampling at \(\bftau\).
A (separable) Hilbert space with orthobasis \(\set{\psi_n}_{n\geq 1}\) is an RKHS iff \(\forall \bftau\in\bbR^d\) \(\sum_{n=1}^\infty\abs{\psi_{n}(\tau)}^2<\infty\)
If \(\calH\) is an RKHS, then \[ \min_{f\in\calF}\sum_{i=1}^n\abs{y_i-f(\vecx_i)}^2+\lambda\norm[\calH]{f} \] has solution \[ f = \sum_{i=1}^n\alpha_i k_{\vecx_i}\textsf{ with } \bfalpha = (\matK+\lambda\matI)^{-1}\vecy\qquad \matK=\mat{c}{k(\vecx_i,\vecx_j)}_{1\leq i,j\leq n} \]