Ab initio calculations of energy transfer and non-additivity in the He-Ne laser system
Eur. Phys. J. D 7, 181–189 (1999) • 1999
معلومات البحث
المؤلفون
A.S. Shalabi1, M.M. Assem1, S. Abd El-Aal1, M.A. Kamel2, and M.M. Abd El-Rahman2
الكلمات المفتاحية
Not Available
المجلة العلمية
Eur. Phys. J. D 7, 181–189 (1999)
الناشر
Not Available
المجلد
Not Available
العدد
Not Available
الصفحات
Not Available
publication.type
International
رابط البحث
Not Available
المواد المرفقة
Not Available
الملخص
Ab initio calculations were performed for several suggested mechanisms of energy transfer between
helium metastable particles and neon. Optimized geometries and excited-state energies were calculated
for neon excited-state complexes and the convergence properties of the non-additive contributions to
the interaction energies were examined. The most probable excitation-transfer mechanism was found to be
Hem2
(a3Σ+
u )+Ne → (He2Ne)
∗
r
→ Ne(2p53s)+2He based on an energy difference of 0.0674 eV between the
triplet excited state of Hem2
and the singlet excited state of (HeNeHe)
∗
r. No theoretical evidence was found
for the production of neon singlet excited-state complexes other than 20.0858 to 20.4875 eV by the considered
two-, three- and four-body models of energy transfer processes. The energy curves of the reactions
involving the excited-state complexes (HeNeHe)
∗
r and (HeNe)
∗
r are provided and compared with the previously
reported experimental results on the reaction Hem2
(a3Σ+
u )+Ne → (He2Ne)
∗
r
→ Ne(2p53s)+2He. The
relation between the probability of energy transfer and laser activity is discussed. The non-additive contribution
to the total interaction energy of the nominated (HeNeHe)
∗
r intermediate complex was found to be
negligible, pointing to the possibility of constructing model potentials and simulation of larger systems.
helium metastable particles and neon. Optimized geometries and excited-state energies were calculated
for neon excited-state complexes and the convergence properties of the non-additive contributions to
the interaction energies were examined. The most probable excitation-transfer mechanism was found to be
Hem2
(a3Σ+
u )+Ne → (He2Ne)
∗
r
→ Ne(2p53s)+2He based on an energy difference of 0.0674 eV between the
triplet excited state of Hem2
and the singlet excited state of (HeNeHe)
∗
r. No theoretical evidence was found
for the production of neon singlet excited-state complexes other than 20.0858 to 20.4875 eV by the considered
two-, three- and four-body models of energy transfer processes. The energy curves of the reactions
involving the excited-state complexes (HeNeHe)
∗
r and (HeNe)
∗
r are provided and compared with the previously
reported experimental results on the reaction Hem2
(a3Σ+
u )+Ne → (He2Ne)
∗
r
→ Ne(2p53s)+2He. The
relation between the probability of energy transfer and laser activity is discussed. The non-additive contribution
to the total interaction energy of the nominated (HeNeHe)
∗
r intermediate complex was found to be
negligible, pointing to the possibility of constructing model potentials and simulation of larger systems.
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