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<record version="6" id="3029">
 <title>harmonic function</title>
 <name>HarmonicFunction</name>
 <created>2002-06-04 11:11:57</created>
 <modified>2005-03-25 23:47:20</modified>
 <type>Definition</type>
 <creator id="2727" name="mathcam"/>
 <author id="2727" name="mathcam"/>
 <author id="338" name="ariels"/>
 <classification>
	<category scheme="msc" code="31A05"/>
	<category scheme="msc" code="31B05"/>
	<category scheme="msc" code="31C05"/>
	<category scheme="msc" code="30F15"/>
 </classification>
 <related>
	<object name="RadosTheorem"/>
	<object name="SubharmonicAndSuperharmonicFunctions"/>
	<object name="DirichletProblem"/>
	<object name="NeumannProblem"/>
 </related>
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 <content>A twice-differentiable real or complex-valued function $f\colon U\to\mathbb{R}$ or $f\colon U\to\mathbb{C}$, where $U\subseteq\mathbb{R}^n$ is some \PMlinkescapetext{domain}, is called \emph{harmonic} if its Laplacian vanishes on $U$, i.e. if $$\Delta f\equiv 0.$$

Any harmonic function $f\colon\mathbb{R}^n\to\mathbb{R}$ or $f\colon\mathbb{R}^n\to\mathbb{C}$ satisfies Liouville's theorem.   Indeed, a holomorphic function \emph{is} harmonic, and a real harmonic function $f\colon U\to\mathbb{R}$, where $U\subseteq\mathbb{R}^2$, is locally the real part of a holomorphic function.  In fact, it is enough that a harmonic function $f$ be \PMlinkescapetext{bounded} below (or above) to conclude that it is \PMlinkescapetext{constant}.</content>
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