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		<id>https://en.formulasearchengine.com/index.php?title=Expectation_hypothesis&amp;diff=26584</id>
		<title>Expectation hypothesis</title>
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		<summary type="html">&lt;p&gt;107.19.188.116: &lt;/p&gt;
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&lt;div&gt;The &#039;&#039;&#039;wavelet transform modulus maxima (WTMM)&#039;&#039;&#039; is a method for detecting the [[fractal dimension]] of a signal.&lt;br /&gt;
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More than this, the WTMM is capable of partitioning the time and scale domain of a signal into fractal dimension regions, and the method is sometimes referred to as a &amp;quot;mathematical microscope&amp;quot; due to its ability to inspect the multi-scale dimensional characteristics of a signal and possibly inform about the sources of these characteristics.&lt;br /&gt;
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The WTMM method uses [[continuous wavelet transform]] rather than [[Fourier transform]]s to detect singularities [[Mathematical singularity|singularity]] – that is discontinuities, areas in the signal that are not continuous at a particular derivative.&lt;br /&gt;
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In particular, this method is useful when analyzing [[multifractal]] signals, that is, signals having multiple fractal dimensions.&lt;br /&gt;
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== Description ==&lt;br /&gt;
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Consider a signal that can be represented by the following equation:&lt;br /&gt;
&lt;br /&gt;
: &amp;lt;math&amp;gt;f(t) = a_0 + a_1 (t - t_i) + a_2(t - t_i)^2 + \cdots + a_h(t - t_i)^{h_i} \, &amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where &amp;lt;math&amp;gt; t &amp;lt;/math&amp;gt; is close to &amp;lt;math&amp;gt; t_i &amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt; h_i &amp;lt;/math&amp;gt; is a non-integer quantifying the local singularity.  (Compare this to a [[Taylor series]], where in practice only a limited number of low-order terms are used to approximate a continuous function.)&lt;br /&gt;
&lt;br /&gt;
Generally, a [[continuous wavelet transform]] decomposes a signal as a function of time, rather than assuming the signal is stationary (For example, the Fourier transform).   Any continuous wavelet can be used, though the first derivative of the [[Gaussian distribution]] and the [[Mexican hat wavelet]] (2nd derivative of Gaussian) are common.  Choice of wavelet may depend on characteristics of the signal being investigated.&lt;br /&gt;
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Below we see one possible wavelet basis given by the first derivative of the Gaussian:&lt;br /&gt;
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: &amp;lt;math&amp;gt;G&#039; (t,a,b) = \frac{a}{(2\pi)^{-1/2}}(t - b) e^{\left(\frac{-(t-b)^2}{2a^2}\right)} \,&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Once a &amp;quot;mother wavelet&amp;quot; is chosen, the continuous wavelet transform is carried out as a continuous, [[square-integrable function]] that can be scaled and translated.  Let &amp;lt;math&amp;gt;a &amp;gt; 0&amp;lt;/math&amp;gt; be the scaling constant and &amp;lt;math&amp;gt;b\in\mathbb{R}&amp;lt;/math&amp;gt; be the translation of the wavelet along the signal:&lt;br /&gt;
&lt;br /&gt;
: &amp;lt;math&amp;gt;X_w(a,b)=\frac{1}{\sqrt{a}} \int_{-\infty}^\infty x(t)\psi^\ast \left(\frac{t-b}{a}\right)\, dt&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where &amp;lt;math&amp;gt;\psi(t)&amp;lt;/math&amp;gt;  is a continuous function in both the time domain and the frequency domain called the mother wavelet and &amp;lt;math&amp;gt;^{\ast}&amp;lt;/math&amp;gt; represents the operation of [[complex conjugate]].&lt;br /&gt;
&lt;br /&gt;
By calculating &amp;lt;math&amp;gt;X_w(a,b) &amp;lt;/math&amp;gt; for subsequent wavelets that are derivatives of the mother wavelet, singularities can be identified.  Successive derivative wavelets remove the contribution of lower order terms in the signal, allowing the maximum &amp;lt;math&amp;gt;h_i&amp;lt;/math&amp;gt; to be detected.  (Recall that when taking derivatives, lower order terms become 0.)  This is the &amp;quot;modulus maxima&amp;quot;.&lt;br /&gt;
&lt;br /&gt;
Thus, this method identifies the singularity spectrum by convolving the signal with a wavelet at different scales and time offsets.&lt;br /&gt;
&lt;br /&gt;
The WTMM is then capable of producing{{Vague|date=October 2013}} a &amp;quot;skeleton&amp;quot; that partitions the scale and time space by fractal dimension.&lt;br /&gt;
&lt;br /&gt;
== History ==&lt;br /&gt;
&lt;br /&gt;
The WTMM was developed out of the larger field of continuous wavelet transforms, which arose in the 1980s, and its contemporary fractal dimension methods.&lt;br /&gt;
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At its essence, it is a combination of fractal dimension &amp;quot;box counting&amp;quot; methods and continuous wavelet transforms, where wavelets at various scales are used instead of boxes.&lt;br /&gt;
&lt;br /&gt;
WTMM was originally developed by Mallat and Hwang in 1992 and used for image processing. [http://ieeexplore.ieee.org/stamp/stamp.jsp?tp=&amp;amp;arnumber=119727&amp;amp;isnumber=3425]&lt;br /&gt;
&lt;br /&gt;
Bacry, Muzy, and Arneodo were early users of this methodology. [http://prl.aps.org/abstract/PRL/v67/i25/p3515_1][http://pre.aps.org/abstract/PRE/v47/i2/p875_1] It has subsequently been used in fields related to signal processing.&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&lt;br /&gt;
* Alain Arneodo et al. (2008), [[Scholarpedia]], 3(3):4103. [http://www.scholarpedia.org/article/Wavelet-based_multifractal_analysis]&lt;br /&gt;
&lt;br /&gt;
* &#039;&#039;A Wavelet Tour of Signal Processing&#039;&#039;, by Stéphane Mallat; ISBN :012466606X {{Please check ISBN|reason=Invalid length.}}; Academic Press, 1999 [http://www.ceremade.dauphine.fr/~peyre/wavelet-tour/]&lt;br /&gt;
&lt;br /&gt;
* Mallat, S.; Hwang, W.L.;, &amp;quot;Singularity detection and processing with wavelets,&amp;quot; &#039;&#039;IEEE Transactions on Information Theory&#039;&#039;, volume 38, number 2, pages 617–643, Mar 1992 {{doi|10.1109/18.119727}} [http://ieeexplore.ieee.org/stamp/stamp.jsp?tp=&amp;amp;arnumber=119727&amp;amp;isnumber=3425]&lt;br /&gt;
&lt;br /&gt;
* Arneodo on Wavelets [http://www.iscpif.fr/tiki-index.php?page=CSSS&#039;08+Arneodo&amp;amp;highlight=towards]&lt;br /&gt;
&lt;br /&gt;
* &amp;quot;Wavelets and multifractal formalism for singular signals : application to turbulence data&amp;quot;, J.F. Muzy, E. Bacry and A. Arneodo, &#039;&#039;Physical Review Letters&#039;&#039; 67, 3515 (1991). [http://prl.aps.org/abstract/PRL/v67/i25/p3515_1]&lt;br /&gt;
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* &amp;quot;Multifractal formalism for fractal signals: the structure fonction approach versus the wavelet transform modulus maxima method&amp;quot;, J.F. Muzy, E. Bacry and A. Arneodo, &#039;&#039;Phys. Rev. E&#039;&#039; 47, 875 [http://pre.aps.org/abstract/PRE/v47/i2/p875_1]&lt;br /&gt;
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[[Category:Wavelets| ]]&lt;/div&gt;</summary>
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