The Landauer-Büttiker theory of mesoscopic conductors was recently extended to nanoelectromechanical systems. In this extension, the adiabatic reaction forces exerted by the electronic degrees of freedom on the mechanical modes were expressed in terms of the electronic S matrix and its first nonadiabatic correction, the A matrix. Here, we provide a more natural and efficient derivation of these results within the setting and solely with the methods of scattering theory. Our derivation is based on a generic model of a slow classical degree of freedom coupled to a quantum-mechanical scattering system, extending previous work on adiabatic reaction forces for closed quantum systems
In molecular dynamics applications there is a growing interest in mixed quantum-classical models. Th...
We shall revisit the conventional adiabatic or Markov approximation, which — contrary to the semicla...
The first proof of the quantum adiabatic theorem was given as early as 1928. Today, this theorem is ...
The Landauer-Buttiker theory of mesoscopic conductors was recently extended to nanoelectromechanical...
Nanoelectromechanical systems are characterized by an intimate connection between electronic and me...
Nanoelectromechanical systems are characterized by an intimate connection between electronic and mec...
In these lecture notes, partly based on a course taught at the Karpacz Winter School in March 2014, ...
The theory of near-adiabatic collisions is formulated in a fully quantum-mechanical form, correctly ...
The extension of the scheme of mesoscopic non-equilibrium thermodynamics developed for quantum mecha...
We develop a scattering theory of current-induced forces exerted by the conduction electrons of a ge...
The conventional quantum-mechanical formulation of near-adiabatic collision theory is known to have ...
Abstract The influence of a fast system on the hamiltonian dynamics of a slow system coupled to it i...
1\. Introduction 2\. Scattering theory 3\. Scattering theory of adiabatic reaction forces 4\. Relati...
When parameters are varied periodically, charge can be pumped through a mesoscopic conductor without...
Simulating chemical dynamics going beyond the adiabatic approximation can be challenging. Due to the...
In molecular dynamics applications there is a growing interest in mixed quantum-classical models. Th...
We shall revisit the conventional adiabatic or Markov approximation, which — contrary to the semicla...
The first proof of the quantum adiabatic theorem was given as early as 1928. Today, this theorem is ...
The Landauer-Buttiker theory of mesoscopic conductors was recently extended to nanoelectromechanical...
Nanoelectromechanical systems are characterized by an intimate connection between electronic and me...
Nanoelectromechanical systems are characterized by an intimate connection between electronic and mec...
In these lecture notes, partly based on a course taught at the Karpacz Winter School in March 2014, ...
The theory of near-adiabatic collisions is formulated in a fully quantum-mechanical form, correctly ...
The extension of the scheme of mesoscopic non-equilibrium thermodynamics developed for quantum mecha...
We develop a scattering theory of current-induced forces exerted by the conduction electrons of a ge...
The conventional quantum-mechanical formulation of near-adiabatic collision theory is known to have ...
Abstract The influence of a fast system on the hamiltonian dynamics of a slow system coupled to it i...
1\. Introduction 2\. Scattering theory 3\. Scattering theory of adiabatic reaction forces 4\. Relati...
When parameters are varied periodically, charge can be pumped through a mesoscopic conductor without...
Simulating chemical dynamics going beyond the adiabatic approximation can be challenging. Due to the...
In molecular dynamics applications there is a growing interest in mixed quantum-classical models. Th...
We shall revisit the conventional adiabatic or Markov approximation, which — contrary to the semicla...
The first proof of the quantum adiabatic theorem was given as early as 1928. Today, this theorem is ...