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		<id>https://en.formulasearchengine.com/index.php?title=Perfectoid&amp;diff=29384&amp;oldid=prev</id>
		<title>en&gt;David Eppstein: {{abstract-algebra-stub}}</title>
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		<updated>2013-10-03T21:30:50Z</updated>

		<summary type="html">&lt;p&gt;{{abstract-algebra-stub}}&lt;/p&gt;
&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;{{technical|date=July 2013}}&lt;br /&gt;
&lt;br /&gt;
In the mathematical [[theory of probability]], &amp;#039;&amp;#039;&amp;#039;Brownian meander&amp;#039;&amp;#039;&amp;#039; &amp;lt;math&amp;gt;W^+ = \{ W_t^+, t \in [0,1] \}&amp;lt;/math&amp;gt; is a continuous non-homogenous [[Markov process]] defined as follows:&lt;br /&gt;
&lt;br /&gt;
Let &amp;lt;math&amp;gt;W = \{ W_t, t \geq 0 \}&amp;lt;/math&amp;gt; be a standard one-dimensional [[Wiener process|Brownian motion]], &amp;lt;math&amp;gt; \tau := \sup \{ t \in [0,1] : W_t = 0 \} &amp;lt;/math&amp;gt; the last time before &amp;#039;&amp;#039;t&amp;#039;&amp;#039;&amp;amp;nbsp;=&amp;amp;nbsp;1 when &amp;lt;math&amp;gt;W&amp;lt;/math&amp;gt; visits &amp;lt;math&amp;gt;\{ 0 \}&amp;lt;/math&amp;gt;. Then &lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;W^+_t := \frac{1}{\sqrt{1 - \tau}} | W_{\tau + t (1-\tau)} |, \quad t \in [0,1].&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The [[transition density]] &amp;lt;math&amp;gt;p(s,x,t,y) \, dy := P(W^+_t \in dy \mid W^+_s = x)&amp;lt;/math&amp;gt; of Brownian meander is described as follows: &lt;br /&gt;
&lt;br /&gt;
For &amp;lt;math&amp;gt;0 &amp;lt; s &amp;lt; t \leq 1&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;x, y &amp;gt; 0&amp;lt;/math&amp;gt;, and writing&lt;br /&gt;
&lt;br /&gt;
: &amp;lt;math&amp;gt;\phi_t(x):= \frac{\exp \{ -x^2/(2t) \}}{\sqrt{2 \pi t}} \quad \text{and} \quad \Phi_t(x,y):= \int^y_x\phi_t(w) \, dw,&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
we have&lt;br /&gt;
&lt;br /&gt;
:&amp;lt;math&amp;gt;&lt;br /&gt;
\begin{align}&lt;br /&gt;
p(s,x,t,y) \, dy &amp;amp;:= P(W^+_t \in dy  \mid W^+_s = x) \\&lt;br /&gt;
&amp;amp;= \bigl(  \phi_{t-s}(y-x) - \phi_{t-s}(y+x) \bigl)  \frac{\Phi_{1-t}(0,y)}{\Phi_{1-s}(0,x)} \, dy&lt;br /&gt;
\end{align}&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
and&lt;br /&gt;
&lt;br /&gt;
: &amp;lt;math&amp;gt;&lt;br /&gt;
p(0,0,t,y) \, dy := P(W^+_t \in dy ) = 2\sqrt{2 \pi} \frac{y}{t}\phi_t(y)\Phi_{1-t}(0,y) \, dy.&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
In particular, &lt;br /&gt;
&lt;br /&gt;
: &amp;lt;math&amp;gt;P(W^+_1 \in dy ) = y \exp \{ -y^2/2 \} \, dy, \quad y &amp;gt; 0,&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
i.e &amp;lt;math&amp;gt; W^+_1 &amp;lt;/math&amp;gt; has the [[Rayleigh distribution]] with parameter 1, the same distribution as &amp;lt;math&amp;gt;\sqrt{2 \mathbf{e}}&amp;lt;/math&amp;gt;, where &amp;lt;math&amp;gt;\mathbf{e}&amp;lt;/math&amp;gt; is an [[Exponential distribution|exponential random variable]] with parameter 1.&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&lt;br /&gt;
* {{Cite journal |author=Durett, Richard; Iglehart, Donald; Miller, Douglas |year= 1977|title= Weak convergence to Brownian meander and Brownian excursion | journal = The Annals of Probability | volume = 5 | issue = 1| pages = 117–129 |&lt;br /&gt;
url = http://projecteuclid.org/DPubS?service=UI&amp;amp;version=1.0&amp;amp;verb=Display&amp;amp;handle=euclid.aop/1176995895}}&lt;br /&gt;
* {{Cite book |author=Revuz, Daniel; Yor, Marc |title=Continuous Martingales and Brownian Motion |edition=2nd  |isbn=3-540-57622-3 |publisher=Springer-Verlag |location=New York |year=1999}}&lt;br /&gt;
&lt;br /&gt;
{{Stochastic processes}}&lt;br /&gt;
&lt;br /&gt;
[[Category:Stochastic processes]]&lt;br /&gt;
[[Category:Markov processes]]&lt;/div&gt;</summary>
		<author><name>en&gt;David Eppstein</name></author>
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