2002
DOI: 10.1103/physrevlett.89.163202
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Double Photoionization and Transfer Ionization of He: Shakeoff Theory Revisited

Abstract: The shakeoff theory of Aberg [Phys. Rev. A 2, 1726 (1970)] is revisited. With the sudden approximation, we calculate the shakeoff probability when one of the electrons in He is ejected with a finite velocity. This theory is used to examine ratios of cross sections for double to single photoionization and transfer ionization to single electron capture. It is also shown that the momentum distribution of the shakeoff electron provides a means to measure the correlation of the ground state wave function directly.

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Cited by 37 publications
(35 citation statements)
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References 19 publications
(23 reference statements)
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“…For instance, such aspects are electron-electron correlation and entanglement [2][3][4], selection rules [5][6][7], ionization mechanisms [8][9][10], scattering and interference effects, and photon energy and polarization [11]. These characteristics dictate the kinetic energy and the emission pattern of the electrons escaping upon ionization of the target.…”
Section: Introductionmentioning
confidence: 99%
“…For instance, such aspects are electron-electron correlation and entanglement [2][3][4], selection rules [5][6][7], ionization mechanisms [8][9][10], scattering and interference effects, and photon energy and polarization [11]. These characteristics dictate the kinetic energy and the emission pattern of the electrons escaping upon ionization of the target.…”
Section: Introductionmentioning
confidence: 99%
“…Such a process, which becomes possible if the atomic target has at least two electrons, is called transfer ionization. During the last decade transfer ionization in collisions of protons with helium atoms has attracted much attention [1][2][3][4][5][6].…”
Section: Introductionmentioning
confidence: 99%
“…(Note that the ψ f in equation (7) are eigenfunctions of the full atomic Hamiltonian H at including electron-electron interaction, in contrast to the final states in equation (6).) From equation (4), however, it immediately follows that…”
mentioning
confidence: 99%
“…shake-off and knock-out). From [6] it is not entirely clear how much of this "overshooting" has to be attributed to a poor choice of the ground state wavefunction (leading to an asymptotic highenergy limit which is somewhat too large) and how much would still be observed using a more accurate initial state. Assuming that this effect persists it would be obvious that again no physical meaning can be ascribed to this definition of shake-off, since shake-off alone would already be larger than the sum of all mechanisms.…”
mentioning
confidence: 99%