<?xml version="1.0" encoding="UTF-8"?>

<record version="4" id="741">
 <title>superfluid</title>
 <name>Superfluid2</name>
 <created>2009-05-09 09:38:02</created>
 <modified>2009-05-09 10:02:17</modified>
 <type>Definition</type>
 <creator id="441" name="bci1"/>
 <modifier id="441" name="bci1"/>
 <author id="441" name="bci1"/>
 <classification>
	<category scheme="msc" code="02."/>
	<category scheme="msc" code="03."/>
	<category scheme="msc" code="03.65.Fd"/>
 </classification>
 <defines>
	<concept>supefluid $^3$He</concept>
	<concept>Cooper (electron) pairs</concept>
	<concept>long-range coupling</concept>
	<concept>superconductivity</concept>
	<concept>coupled boson systems</concept>
	<concept>quantum statistical theories</concept>
	<concept>quantum statistical mechanics</concept>
 </defines>
 <preamble></preamble>
 <content>A {\em superfluid} is described as a macroscopically coherent quantum system $S_F$ that exhibits `unusual' properties such as negligible losses or no resistance to flows. Therefore, it is defined as a phase that exhibits most unusual effects, previously considered to be anomalous from a thermodynamic viewpoint, that can be however explained in terms of quantum statistical theory/quantum statistical mechanics and long-range coherence of coupled boson systems. As an example, in a superconductor the long-ranged coupling of Cooper electron pairs form a superfluid that sustains very high electric currents without any significant heating of the metal.  Liquid $^3$He is another example of a superfluid where the liquid flow can take place upwards in the absence of externally applied pressure and no apparent resistance to flow--no viscosity.</content>
</record>
