Coulomb Dissociation of Nanoparticles Grazing along Organic Surfaces

2012 ◽  
Vol 67 (5) ◽  
pp. 296-302
Author(s):  
Viacheslav V. Komarov ◽  
Anna M. Popova ◽  
Lothar Schmidt ◽  
Hartmut Jungclas

A Coulomb dissociation model is presented for molecular nanoparticles, e.g. nanoclusters consisting of identical atoms or small molecules. These nanoparticles graze with velocities less than the Bohr velocity (108 cm=s) along an organic surface at atomic distances. The surface molecules contain IR-antennas, which consist of periodically located identical diatomic valence bonds with significant dipole momenta, e.g. hydrocarbon chains like (CH2)n. Here, we analyse the Coulomb interaction of these surface molecules with grazing nanoparticles, which do not contain any IR-antennas, e.g. fullerene molecules. Provided that the grazing velocity is in the range of 105 - 107 cm=s and the minimum distance of the grazing nanoparticles to the surface is approximately 2 Å , the IR-antennas of the interacting surface molecules will collect vibrational energy quanta, the so-called excimols. The number of excimols accumulated during the interaction time of at least 1 ps increases with the number of dipoles in the IR-antennas. Excimol energy can be transmitted back to the grazing nanoparticle by a ps-photon flux, which is estimated intense enough to induce multi-ionization of nanoparticle constituents. The resulting charges inside the nanoparticles cause high Coulomb repulsion forces, which will be able to promptly dissociate them.

1990 ◽  
Vol 94 (18) ◽  
pp. 6959-6962 ◽  
Author(s):  
Alessandro. Lami ◽  
Giovanni. Villani

1986 ◽  
Vol 39 (5) ◽  
pp. 749 ◽  
Author(s):  
G Doherty ◽  
MJ Hamilton ◽  
PG Burton ◽  
EI von Nagy-Felsobuki

A combination of known methods have been spliced together in order to calculate accurate vibrational energies and wavefunctions. The algorithm is based on the Rayleigh-Ritz variational procedure in which the trial wavefunction is a linear combination of configuration products of one-dimensional basis functions. The Hamiltonian is that due to Carney and Porter (1976). The kernel of the algorithm consists o( the one-dimensional basis functions, which are the finite element solutions of the associated one-dimensional problems.


1963 ◽  
Vol 157 (968) ◽  
pp. 293-300 ◽  

Although the system in which photosynthesis occurs is exceedingly complex there is no reason to suppose that the primary processes involve any principles not already encountered in the photochemistry of other large organic molecules. It will therefore be useful to consider such processes with reference to chlorophyll as a particular case. In many ways the luminescent and photochemical properties of large conjugated organic molecules in the condensed phase are simpler than those of small molecules or molecules in the gas phase. This apparent paradox is a result of the rapid dissipation of excess vibrational energy and the rapid inter-conversion between electronic states which occurs in such systems. An additional simplification is introduced when only processes relevant to photosynthesis need to be considered since irreversible photochemical reactions are then unimportant. Most of the detailed information which is available refers to dilute solutions where the solute molecules are monomeric, though they may be complexed with the solvent, and it will be convenient to consider such systems first.


1983 ◽  
Vol 79 (9) ◽  
pp. 4247-4260 ◽  
Author(s):  
John S. Hutchinson ◽  
William P. Reinhardt ◽  
James T. Hynes

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