2002
DOI: 10.1073/pnas.142253999
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Beyond the Rayleigh instability limit for multicharged finite systems: From fission to Coulomb explosion

Abstract: We address the stability of multicharged finite systems driven by Coulomb forces beyond the Rayleigh instability limit. Our exploration of the nuclear dynamics of heavily charged Morse clusters enabled us to vary the range of the pair potential and of the fissibility parameter, which results in distinct fragmentation patterns and in the angular distributions of the fragments. The Rayleigh instability limit separates between nearly binary (or tertiary) spatially unisotropic fission and spatially isotropic Coulo… Show more

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Cited by 78 publications
(66 citation statements)
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“…In the case of multiply charged clusters, the two competing processes for dissociation are the evaporation of a neutral atom or molecule and the ejection of charged subunits. The latter occurs through a fission process in which the cluster dissociates into two or three charged fragments that then separate due to coulombic repulsion [41]. The competing processes of evaporation and fission have been described by various liquid-drop models for clusters as diverse as atomic nuclei [42], multiply charged metal clusters [5,6], and highly charged solvent droplets [2,3].…”
Section: Nih-pa Author Manuscriptmentioning
confidence: 99%
“…In the case of multiply charged clusters, the two competing processes for dissociation are the evaporation of a neutral atom or molecule and the ejection of charged subunits. The latter occurs through a fission process in which the cluster dissociates into two or three charged fragments that then separate due to coulombic repulsion [41]. The competing processes of evaporation and fission have been described by various liquid-drop models for clusters as diverse as atomic nuclei [42], multiply charged metal clusters [5,6], and highly charged solvent droplets [2,3].…”
Section: Nih-pa Author Manuscriptmentioning
confidence: 99%
“…In the following, we can introduce the 'recorded cluster size' as the sum of the fragment cluster sizes before unimolecular evaporation has occurred (see Figure 4a). The possible difference in produced and observed sizes is due to neutral fragment formation during break-up, as is predicted by classical molecular dynamics calculations on Morse clusters, 42 or the fast 'boiling off' of monomers 26 before break-up.…”
Section: Breakup Into Protonated Fragmentsmentioning
confidence: 90%
“…These dynamic studies were extended for the adiabatic nuclear dynamics of multicharged atomic and molecular clusters (129,130), which manifest unique fragmentation patterns, such as cluster fission and Coulomb explosion. We addressed (130) unifying features of fragmentation channels driven by Coulomb instabilities in clusters, nuclei, droplets, and spectral molasses, demonstrating that the Rayleigh stability limit X = E(Coulomb)/2E(surface) = 1 separates between spatially anisotropic fission (X < 1) and spatially isotropic Coulomb explosion (X > 1).…”
Section: From Dynamics Of Large Finite Systems To Ultracold Cloudsmentioning
confidence: 99%