1966
DOI: 10.1016/0031-9163(66)90400-8
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Minimum moment required to bind a charged particle to an extended dipole

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Cited by 96 publications
(25 citation statements)
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“…30 Indeed, it has been shown that such a potential with a dipole moment greater than 1.625 D possesses an infinite number of bound anionic states within the Born-Oppenheimer ͑BO͒ approximation. [29][30][31][32][33] Jordan and Luken demonstrated that the loosely bound electron in a dipole-bound state occupies a diffuse orbital localized mainly on the positive side of the molecular dipole. 34 The role of non-BO coupling has been studied by Garrett, who concluded that such couplings are negligible for dipole-bound states with electron binding energies (E bind ) much larger than molecular rotational constants.…”
Section: B Dipole-bound Anionsmentioning
confidence: 99%
“…30 Indeed, it has been shown that such a potential with a dipole moment greater than 1.625 D possesses an infinite number of bound anionic states within the Born-Oppenheimer ͑BO͒ approximation. [29][30][31][32][33] Jordan and Luken demonstrated that the loosely bound electron in a dipole-bound state occupies a diffuse orbital localized mainly on the positive side of the molecular dipole. 34 The role of non-BO coupling has been studied by Garrett, who concluded that such couplings are negligible for dipole-bound states with electron binding energies (E bind ) much larger than molecular rotational constants.…”
Section: B Dipole-bound Anionsmentioning
confidence: 99%
“…Long-range dipolar binding plays an important role. Theoretically, a point dipole will bind an electron (and hence, alternatively, a positron) if its dipole moment is larger than a certain critical value, namely 1.625 D (39,40,41,42,43). The same is true of an extended structureless dipole (44), and of a point dipole surrounded by any charge distribution which is spherically symmetrical and overall neutral (42).…”
Section: Aamentioning
confidence: 90%
“…and 0 ϭ1.5 a.u. and the energetic splitting: energy in BOA E BO , second-order diagonal correction E (2)DK , second-order NA correction E (2)NA , total energy in second order E BO ϩE (2) , total energy in higher orders ͑only even orders are shown͒, and energy in the x-diabatic approximation, with the coupling between X and r treated exactly. We have seen that basis functions 5 and 6 hardly contribute to the exact wave function, while in BO approximation they should dominate in the tunneling region.…”
Section: ͑12͒mentioning
confidence: 99%