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src/intro.tex
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@ -1,13 +1,13 @@
\chapter{Introduction}%
\label{chap:intro}
Traditionally~\cite{Weiss2012,Rivas2012,Breuer2002Jun}, open quantum
systems have stood for a departure form unitary dynamics. Usually a
\emph{small} system with considerably less degrees than the bath it is
coupled to is considered. The main focus however lies on the small
system, whose time development is computed, ideally eliminating the
bath degrees of freedom through various means. As a result, the system
state does not follow the usual unitary time development generated by
the Schr\"odinger equation.
Traditionally, open quantum systems have stood for a departure from
unitary dynamics~\cite{Weiss2012,Rivas2012,Breuer2002Jun}. Usually a
small system is coupled to a large bath with considerably more degrees
of freedom. The main focus, however, lies on the small system, whose
time development is computed, ideally eliminating the bath degrees of
freedom through various means. % As a result, the system state does not
% follow the usual unitary time development generated by the
% Schr\"odinger equation.
The field of quantum thermodynamics has attracted much recent interest
recently~\cite{Talkner2020Oct,Rivas2019Oct,Riechers2021Apr,Vinjanampathy2016Oct,Binder2018,Kurizki2021Dec,Mukherjee2020Jan,Xu2022Mar}.
@ -16,8 +16,8 @@ extending the standard phenomenological thermodynamic notions to
microscopic open systems. This setting may make it possible to
formulate rigorous microscopic definitions of thermodynamic quantities
such as internal energy, heat and work that are consistent with the
well-known laws of thermodynamics. There is no consensus on this
matter yet, as is demonstrated by the plethora of proposals and
well-known laws of thermodynamics. Currently, there is no consensus on
this matter yet, as is demonstrated by the plethora of proposals and
discussions in
\cite{Rivas2019Oct,Talkner2020Oct,Motz2018Nov,Wiedmann2020Mar,Senior2020Feb,Kato2015Aug,Kato2016Dec,Strasberg2021Aug,Talkner2016Aug,Bera2021Feb,Bera2021Jun,Esposito2015Dec}.