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Aca - Departamento de Física - Universidad Técnica Federico Santa ...

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V Encuentro Sud Americano <strong>de</strong> Colisiones Inelásticas en la Materia<br />

Supression of binary and recoil peaks in ionization of H 2 by electron impact<br />

Fojón O A, Stia C R and Rivarola R D<br />

Instituto <strong>de</strong> <strong>Física</strong> Rosario (CONICET-UNR), Pellegrini 250 (2000) Rosario, Argentina<br />

email address corresponding author: fojon@ifir-conicet.gov.ar<br />

We study theoretically the single<br />

ionization of H 2 molecules by fast electron<br />

impact. Our aim is to show that interferences<br />

coming from the coherent emission from the<br />

molecular centers may produce unexpected<br />

consequences in the physical features of the<br />

observables of the reaction.<br />

Interference phenomena have been of<br />

crucial importance in the foundation of quantum<br />

mechanics. Analogies with the Young two-slit<br />

experiment played a fundamental role in the<br />

<strong>de</strong>scription and comprehension of the dual<br />

nature of quantum objects such as electrons. A<br />

fascinating alternative way of observing<br />

interference patterns is provi<strong>de</strong>d by the electron<br />

spectra resulting from the ionization of<br />

molecular diatomic targets. In the sixties, it was<br />

suggested that the coherent emission from these<br />

molecules may give rise to specific oscillations<br />

in the differential cross sections of the ejected<br />

electrons, the two molecular centers acting as the<br />

analogues of the two slits in the Young<br />

experiment [1]. However, this kind of<br />

oscillations was measured for the very first time<br />

with fast krypton ions impacting on H 2 [2]. In<br />

previous works, we have shown that these<br />

interference patterns may be observed also for<br />

electron impact [3-7].<br />

We focus here on electron emission at<br />

high impact energies from fixed-in-space H 2<br />

molecules impacted by fast electrons. We study<br />

transitions at fixed equilibrium internuclear<br />

distance from the ground state of H 2 to the<br />

ground (gera<strong>de</strong>) and first excited (ungera<strong>de</strong>)<br />

state of the H +<br />

2 residual target. We consi<strong>de</strong>r<br />

coplanar geometries in which the inci<strong>de</strong>nt,<br />

scattered and ejected momenta lie all in the same<br />

plane. In addition, we analyze asymmetric<br />

kinematics situations in which one slow and one<br />

fast electron are <strong>de</strong>tected in the final channel.<br />

We employ a first or<strong>de</strong>r mo<strong>de</strong>l obtained<br />

in the framework of a two-effective center<br />

approximation (TEC). The i<strong>de</strong>a exploited in the<br />

TEC mo<strong>de</strong>l is that although electrons in the<br />

ground state of H 2 are shared by both nuclei, the<br />

electronic <strong>de</strong>nsity is peaked at the nuclei<br />

positions. Then, it is argued that ejection occurs<br />

in the neighbourhoods of one nucleus while the<br />

nuclear charge of the other one is screened<br />

completely by the non ionized electron.<br />

Consequently, a unique final effective<br />

continuum function satisfying the correct<br />

asymptotic long range conditions is used to<br />

represent the ejected electron in the final channel<br />

of the reaction. This mo<strong>de</strong>l gives reasonably<br />

good agreement with experiments [8]<br />

constituting thus a good approximation to the<br />

final state of the reaction in which three charged<br />

bodies interact through Coulomb potentials. In<br />

or<strong>de</strong>r to take into account the complexities of<br />

this interaction in an approximate way, one can<br />

take a more elaborated final function such as the<br />

one used in Ref. [9]. This function <strong>de</strong>scribes the<br />

final interactions through a product of three<br />

Coulomb functions associated to the three twobody<br />

pairs present in the final channel. The<br />

approximation obtained using this function for<br />

molecular targets gives an excellent agreement<br />

with experiments [10].<br />

We show here for the first time that un<strong>de</strong>r<br />

<strong>de</strong>finite conditions, <strong>de</strong>structive interferences<br />

coming from the coherent emission from both<br />

molecular centers provoke the supression of the<br />

binary peak in the multiple differential cross<br />

sections corresponding to transitions leading to<br />

final ground state of H 2 + . This is a surprising<br />

result as is well known that ejection is classically<br />

more likely to be produced in the binary region.<br />

Moreover, this finding is shocking as so far and<br />

up to our knowledge the presence of the binary<br />

peak was assumed for every ionization reaction<br />

with either atomic or molecular targets [11].<br />

57 Valparaíso, Chile

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