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	<title>Quantum thermodynamics - Revision history</title>
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		<title>wikademia&gt;Eme: by http://en.wikipedia.org/w/index.php?title=Quantum_thermodynamics&amp;action=history</title>
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		<summary type="html">&lt;p&gt;by http://en.wikipedia.org/w/index.php?title=Quantum_thermodynamics&amp;amp;action=history&lt;/p&gt;
&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;&amp;#039;&amp;#039;&amp;#039;Quantum thermodynamics&amp;#039;&amp;#039;&amp;#039; is a topic in theoretical physics that concerns the combination of classical [[thermodynamics]] and [[quantum mechanics]] into a coherent whole. It studies, for example, how a quantum mechanical system interacts with a macroscopic system in [[thermodynamic equilibrium]], such as a [[heat bath]]. A important question in quantum thermodynamics is the extent to which the [[laws of thermodynamics]] continue to hold as one progresses from quantum systems with a macroscopic number of degrees of freedom, which are well-described by [[quantum statistical mechanics]], to quantum systems with few degrees of freedom, which are well described by quantum mechanics itself.&lt;br /&gt;
&lt;br /&gt;
==History==&lt;br /&gt;
The first attempt to combine thermodynamics with the hypothesis of a quantized state was in 1901 when [[Max Planck]] outlined the &amp;quot;quantum hypothesis&amp;quot;, i.e. that the energy of atomic systems can be quantized, and studied the effects of quantization on the radiation spectrum of a [[blackbody]] in [[thermal equilibrium]]&amp;lt;ref&amp;gt;Planck, Max. (1901). &amp;quot;&amp;#039;&amp;#039;[http://dbhs.wvusd.k12.ca.us/webdocs/Chem-History/Planck-1901/Planck-1901.html On the Law of Distribution of Energy in the Normal Spectrum]&amp;#039;&amp;#039;&amp;quot;. [[Annalen der Physik]], vol. 4, p. 553 ff.&amp;lt;/ref&amp;gt;. See the [[history of quantum mechanics]] for more details.&lt;br /&gt;
&lt;br /&gt;
==Approaches==&lt;br /&gt;
&lt;br /&gt;
===Coupling to a macroscopic system===&lt;br /&gt;
One approach to quantum thermodynamics is to couple a small quantum system to a macroscopic system  and investigate consequences of their interaction. There are two general methods for studying such systems. The &amp;quot;Hamiltonian&amp;quot;&amp;quot; method is to treat the small and macroscopic systems as a composite quantum system and study its [[ergodic]] properties&amp;lt;ref&amp;gt;W. Jaksic, C.-A. Pillet: “On a model for quantum friction I: Fermi’s golden&lt;br /&gt;
rule and dynamics at zero temperature”, Annales Henri Poincar ́ Physique Theorique 62 (1995), p. 47-68.&amp;lt;/ref&amp;gt;&amp;lt;ref&amp;gt;W. Jaksic, C.-A. Pillet: “On a model for quantum friction II: Fermi’s golden rule and dynamics at positive temperature”, Communications in Mathematical Physics 176 (1996), p. 619-644.&amp;lt;/ref&amp;gt;&amp;lt;ref&amp;gt; W. Jaksic, C.-A. Pillet: “On a model for quantum friction III: Ergodic properties of the spin-boson system”, Communications in Mathematical Physics 178 (1996), p. 627-651.&amp;lt;/ref&amp;gt;. The [[Liouvillian]] operator associated with the composite system contains in its spectrum the ergodic behavior of the system, which provides a window into the thermodynamic aspects of the system.&lt;br /&gt;
&lt;br /&gt;
The &amp;quot;Markovian&amp;quot; method is to model the macroscopic system as producing an effective stochastic force acting upon the small quantum system&amp;lt;ref&amp;gt; S. Attal, Y. Pautrat: From Repeated to Continuous Quantum Interactions. Annales Henri Poincare (Physique Theorique) 7 (2006), p.59-104.&amp;lt;/ref&amp;gt;. For instance, a small quantum system coupled to a [[heat bath]] can be modeled using a quantum [[Langevin equation]]&amp;lt;ref&amp;gt;S. Attal, and A. Joye, &amp;quot;The Langevin Equation for a Quantum Heat Bath&amp;quot; , Journal of Functional Analysis , 247, (2007), p. 253-288.&amp;lt;/ref&amp;gt;. Such coupling can lead to [[quantum decoherence]]. The Markovian method is also sometimes called a [[quantum noise]] approach&amp;lt;ref&amp;gt;A.C. Gardiner, and P. Zoller, &amp;quot;Quantum Noise: A Handbook of Markovian and Non-Markovian Quantum Stochastic Methods with Applications to Quantum Optics&amp;quot;, Springer, 2004 &amp;lt;/ref&amp;gt; because it can be thought of as perturbing the [[Schroedinger equation]] for the small quantum system with a quantum noise term.&lt;br /&gt;
&lt;br /&gt;
===Keenan model===&lt;br /&gt;
The theory of quantum statistical mechanics (QSM) is very successful in explaining many physical phenomena and provides for a basis to understand thermodynamics&amp;lt;ref&amp;gt;C. Kittel, &amp;quot;Elementary Statistical Physics&amp;quot;, John Wiley and Sons, 1958, chapters 10 and 23.&amp;lt;/ref&amp;gt;. But the Keenan approach to quantum thermodynamics at MIT (named for physicist [[Joseph Henry Keenan]]) recognizes that the postulates underlying QSM are problematic to justify in a rigorous manner starting from only quantum mechanics. The approach seeks to redress this problem by creating a formalism that contains elements of both quantum mechanics and thermodynamics at the microscopic level. The [[density operator]] describing a [[statistical ensemble]] in QSM is reinterpreted as a quantum state operator obeying a nonlinear evolution equation that contains a dissipation term&amp;lt;ref&amp;gt;G.N. Hatsopoulos and E.P Gyftopoulos, A unified quantum theory of mechanics and thermodynamics. Part I. Postulates , Foundations of Physics, Vol. 6, 15 (1976)&amp;lt;/ref&amp;gt;&amp;lt;ref&amp;gt;G.N. Hatsopoulos and E.P Gyftopoulos, A unified quantum theory of mechanics and thermodynamics. Part IIa. Available energy, Foundations of Physics, Vol. 6, 127 (1976).&amp;lt;/ref&amp;gt;&amp;lt;ref&amp;gt;G.N. Hatsopoulos and E.P Gyftopoulos, A unified quantum theory of mechanics and thermodynamics. Part IIb. Stable equilibrium states, Foundations of Physics, Vol. 6, 439 (1976).&amp;lt;/ref&amp;gt;&amp;lt;ref&amp;gt;G.N. Hatsopoulos and E.P Gyftopoulos, A unified quantum theory of mechanics and thermodynamics. Part III. Irreducible quantal dispersions , Foundations of Physics, Vol. 6, 561 (1976).&amp;lt;/ref&amp;gt;. Both quantum mechanics and QSM can be shown to be special cases of this formalism. The Keenan approach has not yet seen adoption by the mainstream physics community&amp;lt;ref&amp;gt;G.P. Beretta, &amp;quot;What Is Quantum Thermodynamics?&amp;quot;, &amp;lt;http://www.ing.unibs.it/~beretta/www.quantumthermodynamics.org/WebSite1.pdf&amp;gt;, 1 Dec. 2011.&amp;lt;/ref&amp;gt;&amp;lt;ref&amp;gt;J. Maddox, Nature, 316, p. 11 (1985).&amp;lt;/ref&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
==See also==&lt;br /&gt;
* [[Quantum decoherence]]&lt;br /&gt;
{{portal|Physics}}&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
&amp;lt;div class=&amp;quot;references-small&amp;quot;&amp;gt;&lt;br /&gt;
&amp;lt;references /&amp;gt;&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==Further reading==&lt;br /&gt;
&amp;lt;div class=&amp;quot;references-small&amp;quot;&amp;gt;&lt;br /&gt;
#{{cite book | author=Gemmer, J., Michel, M., Mahler, G. | title= Quantum Thermodynamics – Emergence of Thermodynamic Behavior Within Composite Quantum Systems | publisher=Springer | year=2005 | isbn=3-540-22911-6}}&lt;br /&gt;
#{{cite book | author=Rudakov, E.S. | title= Molecular, Quantum and Evolution Thermodynamics: Development and Specialization of the Gibbs Method.  | publisher=Donetsk State University Press | year=1998 | isbn=966-02-0708-5}}&lt;br /&gt;
&amp;lt;/div&amp;gt;&lt;br /&gt;
&lt;br /&gt;
==External links==&lt;br /&gt;
*[http://staff.science.uva.nl/~nieuwenh/QL2L.html Quantum Thermodynamics and the Gibbs Paradox]&lt;br /&gt;
*[http://www.chaos.org.uk/~eddy/physics/heat.html Quantum Thermodynamics]&lt;br /&gt;
*[http://www.fh.huji.ac.il/~ronnie/Papers/geva92.pdf On the Classical Limit of Quantum Thermodynamics in Finite Time] [PDF-format]&lt;br /&gt;
*[http://www.quantumthermodynamics.org Quantum Thermodynamics] - list of articles related to the Keenan approach&lt;br /&gt;
*[http://arxiv.org/ftp/quant-ph/papers/0502/0502150.pdf Quantum thermodynamics and Brownain motion]&lt;br /&gt;
&lt;br /&gt;
[[Category:thermodynamics]]&lt;/div&gt;</summary>
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