<?xml version="1.0" encoding="UTF-8"?>
<collection xmlns="http://www.loc.gov/MARC21/slim">
 <record>
  <leader>     caa a22        4500</leader>
  <controlfield tag="001">467892962</controlfield>
  <controlfield tag="003">CHVBK</controlfield>
  <controlfield tag="005">20180406152754.0</controlfield>
  <controlfield tag="007">cr unu---uuuuu</controlfield>
  <controlfield tag="008">170328e20061101xx      s     000 0 eng  </controlfield>
  <datafield tag="024" ind1="7" ind2="0">
   <subfield code="a">10.1007/s10955-006-9161-4</subfield>
   <subfield code="2">doi</subfield>
  </datafield>
  <datafield tag="035" ind1=" " ind2=" ">
   <subfield code="a">(NATIONALLICENCE)springer-10.1007/s10955-006-9161-4</subfield>
  </datafield>
  <datafield tag="245" ind1="0" ind2="0">
   <subfield code="a">Fluctuations of Power Injection in Randomly Driven Granular Gases</subfield>
   <subfield code="h">[Elektronische Daten]</subfield>
   <subfield code="c">[Paolo Visco, Andrea Puglisi, Alain Barrat, Emmanuel Trizac, Frédéric van Wijland]</subfield>
  </datafield>
  <datafield tag="520" ind1="3" ind2=" ">
   <subfield code="a">We investigate the large deviation function π∞(w) for the fluctuations of the power W(t) = wt, integrated over a time t, injected by a homogeneous random driving into a granular gas, in the infinite time limit. Our analytical study starts from a generalized Liouville equation and exploits a Molecular Chaos-like assumption. We obtain an equation for the generating function of the cumulants μ(λ) which appears as a generalization of the inelastic Boltzmann equation and has a clear physical interpretation. Reasonable assumptions are used to obtain μ(λ) in a closed analytical form. A Legendre transform is sufficient to get the large deviation function π∞(w). Our main result, apart from an estimate of all the cumulants of W(t) at large times t, is that π∞ has no negative branch. This immediately results in the inapplicability of the Gallavotti-Cohen Fluctuation Relation (GCFR), that in previous studies had been suggested to be valid for injected power in driven granular gases. We also present numerical results, in order to discuss the finite time behavior of the fluctuations of W (t) . We discover that their probability density function converges extremely slowly to its asymptotic scaling form: the third cumulant saturates after a characteristic time τ larger than ∼50 mean free times and the higher order cumulants evolve even slower. The asymptotic value is in good agreement with our theory. Remarkably, a numerical check of the GCFR is feasible only at small times (at most τ/10), since negative events disappear at larger times. At such small times this check leads to the misleading conclusion that GCFR is satisfied for π∞(w). We offer an explanation for this remarkable apparent verification. In the inelastic Maxwell model, where a better statistics can be achieved, we are able to numerically observe the &quot;failure” of GCFR.</subfield>
  </datafield>
  <datafield tag="540" ind1=" " ind2=" ">
   <subfield code="a">Springer Science + Business Media, Inc., 2006</subfield>
  </datafield>
  <datafield tag="690" ind1=" " ind2="7">
   <subfield code="a">Granular gases</subfield>
   <subfield code="2">nationallicence</subfield>
  </datafield>
  <datafield tag="690" ind1=" " ind2="7">
   <subfield code="a">nonequilibrium steady-states</subfield>
   <subfield code="2">nationallicence</subfield>
  </datafield>
  <datafield tag="690" ind1=" " ind2="7">
   <subfield code="a">large deviation</subfield>
   <subfield code="2">nationallicence</subfield>
  </datafield>
  <datafield tag="690" ind1=" " ind2="7">
   <subfield code="a">fluctuation-dissipation</subfield>
   <subfield code="2">nationallicence</subfield>
  </datafield>
  <datafield tag="700" ind1="1" ind2=" ">
   <subfield code="a">Visco</subfield>
   <subfield code="D">Paolo</subfield>
   <subfield code="u">Laboratoire de Physique Théorique (CNRS UMR 8627), Bâtiment 210, Université Paris-Sud, 91405, Orsay cedex, France</subfield>
   <subfield code="4">aut</subfield>
  </datafield>
  <datafield tag="700" ind1="1" ind2=" ">
   <subfield code="a">Puglisi</subfield>
   <subfield code="D">Andrea</subfield>
   <subfield code="u">Laboratoire de Physique Théorique (CNRS UMR 8627), Bâtiment 210, Université Paris-Sud, 91405, Orsay cedex, France</subfield>
   <subfield code="4">aut</subfield>
  </datafield>
  <datafield tag="700" ind1="1" ind2=" ">
   <subfield code="a">Barrat</subfield>
   <subfield code="D">Alain</subfield>
   <subfield code="u">Laboratoire de Physique Théorique (CNRS UMR 8627), Bâtiment 210, Université Paris-Sud, 91405, Orsay cedex, France</subfield>
   <subfield code="4">aut</subfield>
  </datafield>
  <datafield tag="700" ind1="1" ind2=" ">
   <subfield code="a">Trizac</subfield>
   <subfield code="D">Emmanuel</subfield>
   <subfield code="u">Laboratoire de Physique Théorique et Modèles Statistiques (CNRS UMR 8626), Bâtiment 100, Université Paris-Sud, 91405, Orsay cedex, France</subfield>
   <subfield code="4">aut</subfield>
  </datafield>
  <datafield tag="700" ind1="1" ind2=" ">
   <subfield code="a">van Wijland</subfield>
   <subfield code="D">Frédéric</subfield>
   <subfield code="u">Laboratoire de Physique Théorique (CNRS UMR 8627), Bâtiment 210, Université Paris-Sud, 91405, Orsay cedex, France</subfield>
   <subfield code="4">aut</subfield>
  </datafield>
  <datafield tag="773" ind1="0" ind2=" ">
   <subfield code="t">Journal of Statistical Physics</subfield>
   <subfield code="d">Kluwer Academic Publishers-Plenum Publishers; http://www.springer-ny.com</subfield>
   <subfield code="g">125/3(2006-11-01), 533-568</subfield>
   <subfield code="x">0022-4715</subfield>
   <subfield code="q">125:3&lt;533</subfield>
   <subfield code="1">2006</subfield>
   <subfield code="2">125</subfield>
   <subfield code="o">10955</subfield>
  </datafield>
  <datafield tag="856" ind1="4" ind2="0">
   <subfield code="u">https://doi.org/10.1007/s10955-006-9161-4</subfield>
   <subfield code="q">text/html</subfield>
   <subfield code="z">Onlinezugriff via DOI</subfield>
  </datafield>
  <datafield tag="908" ind1=" " ind2=" ">
   <subfield code="D">1</subfield>
   <subfield code="a">research-article</subfield>
   <subfield code="2">jats</subfield>
  </datafield>
  <datafield tag="950" ind1=" " ind2=" ">
   <subfield code="B">NATIONALLICENCE</subfield>
   <subfield code="P">856</subfield>
   <subfield code="E">40</subfield>
   <subfield code="u">https://doi.org/10.1007/s10955-006-9161-4</subfield>
   <subfield code="q">text/html</subfield>
   <subfield code="z">Onlinezugriff via DOI</subfield>
  </datafield>
  <datafield tag="950" ind1=" " ind2=" ">
   <subfield code="B">NATIONALLICENCE</subfield>
   <subfield code="P">700</subfield>
   <subfield code="E">1-</subfield>
   <subfield code="a">Visco</subfield>
   <subfield code="D">Paolo</subfield>
   <subfield code="u">Laboratoire de Physique Théorique (CNRS UMR 8627), Bâtiment 210, Université Paris-Sud, 91405, Orsay cedex, France</subfield>
   <subfield code="4">aut</subfield>
  </datafield>
  <datafield tag="950" ind1=" " ind2=" ">
   <subfield code="B">NATIONALLICENCE</subfield>
   <subfield code="P">700</subfield>
   <subfield code="E">1-</subfield>
   <subfield code="a">Puglisi</subfield>
   <subfield code="D">Andrea</subfield>
   <subfield code="u">Laboratoire de Physique Théorique (CNRS UMR 8627), Bâtiment 210, Université Paris-Sud, 91405, Orsay cedex, France</subfield>
   <subfield code="4">aut</subfield>
  </datafield>
  <datafield tag="950" ind1=" " ind2=" ">
   <subfield code="B">NATIONALLICENCE</subfield>
   <subfield code="P">700</subfield>
   <subfield code="E">1-</subfield>
   <subfield code="a">Barrat</subfield>
   <subfield code="D">Alain</subfield>
   <subfield code="u">Laboratoire de Physique Théorique (CNRS UMR 8627), Bâtiment 210, Université Paris-Sud, 91405, Orsay cedex, France</subfield>
   <subfield code="4">aut</subfield>
  </datafield>
  <datafield tag="950" ind1=" " ind2=" ">
   <subfield code="B">NATIONALLICENCE</subfield>
   <subfield code="P">700</subfield>
   <subfield code="E">1-</subfield>
   <subfield code="a">Trizac</subfield>
   <subfield code="D">Emmanuel</subfield>
   <subfield code="u">Laboratoire de Physique Théorique et Modèles Statistiques (CNRS UMR 8626), Bâtiment 100, Université Paris-Sud, 91405, Orsay cedex, France</subfield>
   <subfield code="4">aut</subfield>
  </datafield>
  <datafield tag="950" ind1=" " ind2=" ">
   <subfield code="B">NATIONALLICENCE</subfield>
   <subfield code="P">700</subfield>
   <subfield code="E">1-</subfield>
   <subfield code="a">van Wijland</subfield>
   <subfield code="D">Frédéric</subfield>
   <subfield code="u">Laboratoire de Physique Théorique (CNRS UMR 8627), Bâtiment 210, Université Paris-Sud, 91405, Orsay cedex, France</subfield>
   <subfield code="4">aut</subfield>
  </datafield>
  <datafield tag="950" ind1=" " ind2=" ">
   <subfield code="B">NATIONALLICENCE</subfield>
   <subfield code="P">773</subfield>
   <subfield code="E">0-</subfield>
   <subfield code="t">Journal of Statistical Physics</subfield>
   <subfield code="d">Kluwer Academic Publishers-Plenum Publishers; http://www.springer-ny.com</subfield>
   <subfield code="g">125/3(2006-11-01), 533-568</subfield>
   <subfield code="x">0022-4715</subfield>
   <subfield code="q">125:3&lt;533</subfield>
   <subfield code="1">2006</subfield>
   <subfield code="2">125</subfield>
   <subfield code="o">10955</subfield>
  </datafield>
  <datafield tag="900" ind1=" " ind2="7">
   <subfield code="a">Metadata rights reserved</subfield>
   <subfield code="b">Springer special CC-BY-NC licence</subfield>
   <subfield code="2">nationallicence</subfield>
  </datafield>
  <datafield tag="898" ind1=" " ind2=" ">
   <subfield code="a">BK010053</subfield>
   <subfield code="b">XK010053</subfield>
   <subfield code="c">XK010000</subfield>
  </datafield>
  <datafield tag="949" ind1=" " ind2=" ">
   <subfield code="B">NATIONALLICENCE</subfield>
   <subfield code="F">NATIONALLICENCE</subfield>
   <subfield code="b">NL-springer</subfield>
  </datafield>
 </record>
</collection>
