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DESIREE
RESEARCH
FAST COLLISIONS
ION-FULLERENE COLLISIONS
CLUSTERS OF FULLERENES
DESIREE
MODELLING OF ELECTRON TRANSFER
PEOPLE
OPEN POSITIONS
RECENT PUBLICATIONS
RECENT THESES
LINKS
CONTACT
Electron transfer in fast ion-atom collisions
Electron transfer is defined as the transfer of electrons from the target to the colliding projectile. If the projectile speed is low compared to the speed of the bound electrons in the target, the electrons have sufficient time to arrange themselves according to the changing positions of the nuclei. We study fast collisions, where the speed of the projectile is much higher than the speed of the elecrons. In these collisions the probability to transfer an electron from the target to the projectile is extremely low, as the active electron has to undergo a large momentum and energy change within the short collision time. The cross section can be as small as 10-27cm². That makes the investigation of these processes extremely difficult. |
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| The CRYRING facility at MSL (left figure) and the gas-jet target (right fig.) | |
With the CRYRING facility at the Manne Siegbahn Laboratory we have access to unique experimental conditions where the high beam currents make the study of these processes feasible. In combination with a COLTRIMS setup at the internal gas-jet target we can study fast electron transfer collisions with high luminosity and with high resolution.
The investigation of the final momentum space and the projectile scattering angle provides a fundamental and detailed insight into the dynamics of these collisions, and even different electron transfer mechanisms can be separated. In addition, these experiments provide a sensitive test of different theoretical modells.
The reactions, we are focussing on, are:
How COLTRIMS works:
COLTRIMS (COLd Target Recoil Ion Momentum Spectroscopy) is an imaging technique to measure the fragmentation of a few body system. The ionized target fragments from an atomic or molecular collision are projected by an electric field onto a position sensitive detector. From the measured time-of-flight of the particles and their position of impact on the detector the three dimensional momentum vector is obtained. Cooling of the the target atoms before the fragmentation by supersonic expansion makes a high momentum resolution achievable.