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KL divergence is not distance since it is asymmetric |
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[[File:Old Faithful Geyser KDE with plugin bandwidth.png|thumb|250px|alt=Old Faithful Geyser data kernel density estimate with plug-in bandwidth matrix.|Old Faithful Geyser data kernel density estimate with plug-in bandwidth matrix.]]
The [https://cran.r-project.org/web/packages/ks/index.html ks package]<ref>{{Cite journal| author1=Duong, T. | title=ks: Kernel density estimation and kernel discriminant analysis in R | journal=Journal of Statistical Software | year=2007 | volume=21 | issue = 7
272 records with two measurements each: the duration time of an eruption (minutes) and the
waiting time until the next eruption (minutes) of the [[Old Faithful Geyser]] in Yellowstone National Park, USA.
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== Objective and data-driven kernel selection ==
[[File:Empirical Characteristic Function.jpg|alt=An x-shaped region of empirical characteristic function in Fourier space.|thumb|Demonstration of the filter function <math>I_{\vec{A}}(\vec{t})</math>. The square of the empirical distribution function <math>|\hat{\varphi}|^2</math> from ''N''=10,000 samples of the ‘transition distribution’ discussed in Section 3.2 (and shown in Fig. 4), for <math>|\hat{\varphi}|^2 \ge 4(N-1)N^{-2}</math>. There are two color schemes present in this figure. The predominantly dark, multicolored colored ‘X-shaped’ region in the center corresponds to values of <math>|\hat{\varphi}|^2</math> for the lowest contiguous hypervolume (the area containing the origin); the colorbar at right applies to colors in this region. The lightly-colored, monotone areas away from the first contiguous hypervolume correspond to additional contiguous hypervolumes (areas) with <math>|\hat{\varphi}|^2 \ge 4(N-1)N^{-2}</math>. The colors of these areas are arbitrary and only serve to visually differentiate nearby contiguous areas from one another.]]
Recent research has shown that the kernel and its bandwidth can both be optimally and objectively chosen from the input data itself without making any assumptions about the form of the distribution.<ref name=":0">{{Cite journal|last = Bernacchia|first = Alberto|last2 = Pigolotti|first2 = Simone|date = 2011-06-01|title = Self-consistent method for density estimation|journal = Journal of the Royal Statistical Society, Series B|language = en|volume = 73|issue = 3|pages = 407–422|doi = 10.1111/j.1467-9868.2011.00772.x|issn = 1467-9868|arxiv = 0908.3856}}</ref> The resulting kernel density estimate converges rapidly to the true probability distribution as samples are added: at a rate close to the <math>n^{-1}</math> expected for parametric estimators.<ref name=":0" /><ref name=":1">{{Cite journal|last = O’Brien|first = Travis A.|last2 = Collins|first2 = William D.|last3 = Rauscher|first3 = Sara A.|last4 = Ringler|first4 = Todd D.|date = 2014-11-01|title = Reducing the computational cost of the ECF using a nuFFT: A fast and objective probability density estimation method
<math>\hat{\psi_h}(\vec{t}) \equiv \frac{N}{2(N-1)} \left[ 1 + \sqrt{1 - \frac{4(N-1)}{N^2 |\hat{\varphi}(\vec{t})|^2}} I_{\vec{A}}(\vec{t}) \right]</math> <ref name=":22"/>
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