1997
DOI: 10.1209/epl/i1997-00434-8
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Controlled formation of weakly bound atomic negative ions by electron transfer from state-selected Rydberg atoms

Abstract: Reicherts, M.; Roth, T.; Gopalan, A.; Ruf, M.-W.; Hotop, Harmut; Desfrançuois, C.; and Fabrikant, Ilya I., "Controlled formation of weakly bound atomic negative ions by electron transfer from state-selected Rydberg atoms" (1997). Faculty Publications, Department of Physics and Astronomy. 65.

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Cited by 26 publications
(27 citation statements)
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“…In the paper [23], we investigated resonance structures in the electron scattering differential and integral cross sections for tenuously bound atomic systems, E < 0.1 eV in the context of the quenching of Rydberg states by ground state atoms with small EAs [47,48]. In the Au, Pt, and At atoms as well as the C 60 and other fullerene molecules, the meaning of the EAs was in the context of electron attachment to the ground state of neutral complex heavy systems.…”
Section: Resultsmentioning
confidence: 99%
“…In the paper [23], we investigated resonance structures in the electron scattering differential and integral cross sections for tenuously bound atomic systems, E < 0.1 eV in the context of the quenching of Rydberg states by ground state atoms with small EAs [47,48]. In the Au, Pt, and At atoms as well as the C 60 and other fullerene molecules, the meaning of the EAs was in the context of electron attachment to the ground state of neutral complex heavy systems.…”
Section: Resultsmentioning
confidence: 99%
“…, in thermal collisions of Rydberg atoms ( ) nl A with polar and quadrupolar molecules and atoms B possessing low energies of electron affinity. To this end several authors have developed an efficient Rydberg electron transfer (RET) technique for the production of multipolebound anions (see [21][22][23][24] and references therein). RET technique allows one to determine the binding energy, | | e b , of a weakly bound anion using the experimental data for the peak position, n max , in n-dependence of the ion-pair formation cross section and simple semiempirical relation between n max and | | e b obtained in [18].…”
Section: Introductionmentioning
confidence: 99%
“…[7][8][9][10][11][12][13][14][15][16] The excited rare gas atoms can be metastable atoms, optically allowed excited atoms, 16 or even highly excited Rydberg atoms. [17][18][19][20] Most Penning ionization experiments involved the long-lived metastable species He(2 3 S) and He(2 1 S), since the excitation energies E(2 3 S) = 19.8 eV and E(2 1 S) = 20.6 eV are larger than the lowest ionization energies of almost all atoms and molecules except for He and Ne. For the calculations, reliable model potentials are important as they directly impact on the accuracy of estimated collision characteristics such as the total ionization cross sections and their collisional-energy dependence.…”
Section: Introductionmentioning
confidence: 99%