Abstract:Electronic and vibrational degrees of freedom in atom-cluster collisions are treated simultaneously and self-consistently by combining time-dependent density functional theory with classical molecular dynamics. The gradual change of the excitation mechanisms (electronic and vibrational) as well as the related relaxation phenomena (phase transitions and fragmentation) are studied in a common framework as a function of the impact energy (eV. . . MeV). Cluster "transparency" characterized by practically undisturb… Show more
“…It has been successfully applied so far to very different non-adiabatic processes, like atom-cluster collisions [60], ion-fullerene collisions [61], laser induced excitation and fragmentation of molecules [54] or fragmentation and isomerization of organic molecules in laser fields [62]. However, a realistic description of ionization with the NA-QMD theory 2 is still an open problem.…”
We propose a novel method to describe realistically ionization processes with absorbing boundary conditions in basis expansion within the formalism of the so-called Non-Adiabatic Quantum Molecular Dynamics. This theory couples self-consistently a classical description of the nuclei with a quantum mechanical treatment of the electrons in atomic many-body systems. In this paper we extend the formalism by introducing absorbing boundary conditions via an imaginary potential.It is shown how this potential can be constructed in time-dependent density functional theory in basis expansion. The approach is first tested on the hydrogen atom and the pre-aligned hydrogen molecular ion H + 2 in intense laser fields where reference calculations are available. It is then applied to study the ionization of non-aligned H + 2 and H 2 . Striking differences in the orientation dependence between both molecules are found. Surprisingly, enhanced ionization is predicted for perpendicularly aligned molecules.
“…It has been successfully applied so far to very different non-adiabatic processes, like atom-cluster collisions [60], ion-fullerene collisions [61], laser induced excitation and fragmentation of molecules [54] or fragmentation and isomerization of organic molecules in laser fields [62]. However, a realistic description of ionization with the NA-QMD theory 2 is still an open problem.…”
We propose a novel method to describe realistically ionization processes with absorbing boundary conditions in basis expansion within the formalism of the so-called Non-Adiabatic Quantum Molecular Dynamics. This theory couples self-consistently a classical description of the nuclei with a quantum mechanical treatment of the electrons in atomic many-body systems. In this paper we extend the formalism by introducing absorbing boundary conditions via an imaginary potential.It is shown how this potential can be constructed in time-dependent density functional theory in basis expansion. The approach is first tested on the hydrogen atom and the pre-aligned hydrogen molecular ion H + 2 in intense laser fields where reference calculations are available. It is then applied to study the ionization of non-aligned H + 2 and H 2 . Striking differences in the orientation dependence between both molecules are found. Surprisingly, enhanced ionization is predicted for perpendicularly aligned molecules.
“…The relevant KS equations are either solved on a grid (for a review see [41]) or in a finite-basis expansion of the time-dependent KS orbitals [42]. The latter formalism has been successfully applied to collisions between ions and sodium clusters followed by electron transfer [43] and fragmentation processes [44].…”
Section: Fragmentation Of Atomic Clusters In Collisions With Ionsmentioning
Scattering processes leading to excitation or fragmentation of atomic or molecular systems are a source of information on various physical effects associated with the mutual Coulomb interaction of such many-particle systems. This chapter focuses on the discussion of a quantum-mechanical system (the electrons of the target) influenced by a classical environment (the projectile) that provides the energy that disturbs the electronic system [1]. The classical environment can, for instance, be realized by an intense laser field or an ion beam that imposes its time-dependence on the electronic subsystem and defines a typical timescale for the scattering process -femtoseconds for an electronic system exposed to a laser beam and attoseconds for heavy-particle collisions.2.From a theoretical point of view it is the time-dependent many-electron problem that has to be solved for different external potentials representing the interaction with the classical environment. In practice, one often has to be content with a single-particle approximation providing effective singleparticle equations that can be solved for any active electron at the price, however, that the true two-particle character of the electron-electron interaction has to be neglected.It is the power of density functional theory (DFT) to provide a mathmatical framework that allows one to exactly map the many-electron system onto a set of effective single-particle equations. This chapter gives an outline of the basic concepts behind time-dependent DFT based on a series of review articles [2][3][4] that document the activity in this field. For a comprehensive introduction to stationary DFT the monograph of Dreizler and Gross is specially recommended [5].Although there is hardly an alternative to time-dependent DFT for a theoretical investigation of systems with many active electrons it is not always clear how to extract observables of the system to establish contact with experimental results. The second part of this chapter addresses this problem and gives an idea of its complexity.A few applications of DFT for typical collisional situations are summarized at the end of this chapter. Atomic units are used.
“…[8]. It has later been applied to various collision problems: ion-fullerene collisions [9], atom-sodium cluster collisions [10], charge transfer in atom-cluster collisions [11,12], the stopping power of protons or antiprotons in clusters [13,14] or insulators [15], the excitation and ionization of molecules such as ethylene due to proton collisions [16], or the interaction of protons or heavier ions with carbon nanostructures or graphitic sheets [17,18]. It may also be used to study laser-induced molecular or cluster dynamics in the high-field (but still not relativistic) regime; some examples are Refs.…”
We have employed non-adiabatic molecular dynamics based on time-dependent density-functional theory to characterize the scattering behaviour of a proton with the Li 4 cluster. This technique assumes a classical approximation for the nuclei, effectively coupled to the quantum electronic system. This time-dependent theoretical framework accounts, by construction, for possible charge transfer and ionization processes, as well as electronic excitations, which may play a role in the non-adiabatic regime. We have varied the in- forming a LiH molecule. This theoretical formalism proves to be a powerful, effective and predictive tool for the analysis of non-adiabatic processes at the nanoscale.
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