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Resonant Transfer Excitation : Interference Effects [Book Chapter]

Conference · · Recombination of Atomic Ions
 [1];  [2];  [3];  [4];  [5];  [5];  [6];  [6];  [6]
  1. University of North Carolina, Chapel Hill, NC (United States)
  2. University of North Carolina, Chapel Hill, NC (United States); Universite Paul Sabatier, Toulouse (France)
  3. Oak Ridge National Laboratory (ORNL), Oak Ridge, TN (United States); Lawrence Livermore National Laboratory (LLNL), Livermore, CA (United States)
  4. Oak Ridge National Laboratory (ORNL), Oak Ridge, TN (United States); University of Missouri, Rolla, MO (United States)
  5. Oak Ridge National Laboratory (ORNL), Oak Ridge, TN (United States); Kansas State University, Manhattan, KS (United States)
  6. Oak Ridge National Laboratory (ORNL), Oak Ridge, TN (United States)
Interference effects in RTE (Resonant Transfer Excitation) can be studied for low Z projectiles via Auger electrons emitted from highly ionized fast moving projectile ions following collisions with low Z targets. RTE in ion-atom collisions is closely related to dielectronic recombination’. In the latter case which is of practical interest to the fusion power program an electron with the proper velocity incident on a highly charged ion is resonantly captured and simultaneously interacts with an inner shell electron to excite it, thus forming a doubly excited state which may decay predominantly by x-ray emission for higher Z ions or by Auger electron decay for lower Z ions. The resonant velocity is that of the Auger electron emitted by the ion in the doubly excited state. In RTE the electrons to be captured are in low Z atomic (typically He) or molecular (typically H2) targets and the ions are produced by accelerators in highly charged states with the appropriate resonant velocity. The resonance is much broadened by the velocity distribution of the target electrons. Thus the resonance width as a function of projectile energy is determined by folding the Compton profile of the target electrons with the dielectronic recombination cross sections. This results in a formula valid when the impulse approximation applies:
Research Organization:
Oak Ridge National Laboratory (ORNL), Oak Ridge, TN (United States)
Sponsoring Organization:
USDOE Office of Science (SC), Basic Energy Sciences (BES). Chemical Sciences, Geosciences & Biosciences Division (CSGB)
DOE Contract Number:
AC05-84OR21400; FG05-87ER40361
OSTI ID:
10122283
Report Number(s):
CONF-9110313--5; ON: DE92007240
Resource Type:
Conference paper
Conference Information:
Journal Name: Recombination of Atomic Ions Journal Volume: 296
Country of Publication:
United States
Language:
English

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