Double-electron capture as a two-step process

Double-electron capture by the impact of heavy projectiles on heliumlike atoms is studied with a two-electron model. The process is here considered a two-step collision, which in the frame of the distorted-wave formalism is related to the second order. This second order is evaluated by using an on-s...

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Autor principal: Gravielle, M.S
Otros Autores: Miraglia, Jorge Esteban
Formato: Capítulo de libro
Lenguaje:Inglés
Publicado: 1992
Acceso en línea:Registro en Scopus
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Registro en la Biblioteca Digital
Aporte de:Registro referencial: Solicitar el recurso aquí
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100 1 |a Gravielle, M.S. 
245 1 0 |a Double-electron capture as a two-step process 
260 |c 1992 
270 1 0 |m Gravielle, M.S.; Instituto de Astronomía y Física Del Espacio, Consejo Nacional de Investigaciones Científicas y Técnicas, 1428 Buenos Aires, Argentina 
504 |a Zourus, T.J.M., Schneider, D., Stolterfoht, N., (1987) Phys. Rev. A, 35, p. 1963 
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504 |a Belkić, Gayet, R., Salin, A., (1979) Phys. Rep., 56, p. 279 
504 |a Mittleman, M., Calculation of thep+H2→H−+2pReaction Cross Section (1965) Physical Review, 137, p. A1 
504 |a Theisen, T.C., McGuire, J.H., (1979) Phys. Rev. A, 20, p. 1406 
504 |a Gayet, R., Rivarola, R.D., Salin, A., (1981) J. Phys. B, 14, p. 2421 
504 |a Ghosh, M., Mandal, C.R., Mukherjee, S.C., (1987) Phys. Rev. A, 35, p. 5259 
504 |a Chatterjee, S.N., Roy, B.N., (1985) J. Phys. B, 18, p. 4283 
504 |a Olson, R.E., (1982) J. Phys. B, 15, p. L163 
504 |a Crothers, D.S.F., McCarroll, R., (1987) J. Phys. B, 20, p. 2835 
504 |a Fritsch, W., Lin, C.D., (1986) J. Phys. B, 19, p. 2683 
504 |a Fritsch, W., Lin, C.D., (1990) Phys. Rev. A, 41, p. 4776 
504 |a Gramlich, K., Grün, N., Scheid, W., (1989) J. Phys. B, 22, p. 2567 
504 |a Miraglia, J.E., Gravielle, M.S., (1987) Abstracts of Contributed Papers to the 15th International Conference on the Physics of Electronic and Atomic Collisions, Brighton, 1987, p. 521. , edited by, J. Geddes, et al., North-Holland, Amsterdam 
504 |a McGuire, J., (private communcation); When using unperturbed Born wave functions in double excitation, Tfi(1) is real and proportional to ZP, and the principal part also being real contributes to the ZP3 terms of the cross section. Since the energy conservation is imaginary, it gives a contribution of the order of ZP4 and is therefore less important than the principal part; Coleman, J.P., (1969) Case Studies in Atomic Collision Physics I, p. 101. , edited by, E. W. McDaniel, M. C. R. McDowell, North-Holland, Amsterdam 
504 |a We note that langle ξn|Wi| χi+> = < ξn| H-E| χi+rangle = < ξn| En-E +Vn| χi+rangle, where En is the energy of the intermediate state ξn. Since we are working on-shell, E=En [see Eq. (2.7)]; Clementi, E., Roetti, C., (1974) At. Data Nucl. Data Tables, 14, p. 177 
504 |a Bunge, A.V., Bunge, C.F., Jáuregui, R., Cisneros, G., (1989) Comput. Chem., 13, p. 201 
504 |a Bunge, C.F., Jáuregui, R., Cisneros, G., (1989) Comput. Chem., 13, p. 277 
504 |a McDaniel, E.W., Flannery, M.R., Ellis, H.W., Eisele, F.L., Pope, W., (1977), U.S. Army Missile Research and Development Command Technical; DuBois, R.D., (1987) Phys. Rev. A, 36, p. 2585 
504 |a Freire, F.L., Jr., (1988) Phys. Rev. A, 37, p. 280. , N. V. de Castro Faria, and A. G. de Pinho 
504 |a McGuire, J.H., Deb, N.C., Aktas, Y., Sil, N.C., (1988) Phys. Rev. A, 38, p. 3333 
504 |a Fritsch, W., Lin, C.D., (1988) Phys. Rev. Lett., 61, p. 690 
504 |a Meng, L., Reinhold, C.O., (private communication); Note that each contribution should be added coherently; Shah, M.B., Gilbody, H.B., (1985) J. Phys. B, 18, p. 899 
504 |a Hippler, R., Datz, S., Miller, P.D., Pepmiller, P.L., Dittner, P.F., (1987) Phys. Rev. A, 35, p. 585 
504 |a Irby, V., (unpublished). Results provided by C. Reinhold in Ref. [26] 
506 |2 openaire  |e Política editorial 
520 3 |a Double-electron capture by the impact of heavy projectiles on heliumlike atoms is studied with a two-electron model. The process is here considered a two-step collision, which in the frame of the distorted-wave formalism is related to the second order. This second order is evaluated by using an on-shell Green function representing one electron in each center, and it is found to be related, after some approximations, to the independent-electron model. In particular, the exact impulse approximation is used to calculate the single-capture T-matrix elements, and the electronic repulsion is included as a dynamic perturbation in first order. A configuration-interaction wave function is employed to describe the ground state of helium for double capture 1s21s2 in a He2+-He collision. For this benchmark, differences with the use of a Hartree-Fock wave function instead are found to be negligible. Thereafter, capture to single excited states for the same system is calculated by using Hartree-Fock and variational electronic wave functions. Also, double capture for multiply charged ions on helium is calculated. Differential cross sections for double-capture He2+-He collisions at 60 keV/amu impact energy are presented and compared with previous experiments. The present theory produces good agreement with the available data. © 1992 The American Physical Society.  |l eng 
593 |a Instituto de Astronomía y Física Del Espacio, Consejo Nacional de Investigaciones Científicas y Técnicas, 1428 Buenos Aires, Argentina 
700 1 |a Miraglia, Jorge Esteban 
773 0 |d 1992  |g v. 45  |h pp. 2965-2973  |k n. 5  |x 10502947  |t Physical Review A 
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