Stability of Three-Body Coulomb Systems with J = 1 in the Oscillator Representation | Zendy

M. Dineykhan | Zendy; G. V. Efimov | Zendy

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Stability of Three-Body Coulomb Systems with J = 1 in the Oscillator Representation

Author(s) -

M. Dineykhan,

G. V. Efimov

Publication year - 1996

Publication title -

few-body systems

Language(s) - English

Resource type - Journals

SCImago Journal Rank - 0.478

H-Index - 45

eISSN - 1432-5411

pISSN - 0177-7963

DOI - 10.1007/s006010050041

Subject(s) - coulomb , physics , representation (politics) , angular momentum , stability (learning theory) , spectrum (functional analysis) , energy spectrum , momentum (technical analysis) , atomic physics , quantum mechanics , electron , computer science , machine learning , politics , political science , law , finance , economics

. The oscillator representation is applied to calculate the energy spectrum of three-body Coulomb systems with total angular momentum J. For three-body Coulomb systems with J = 1 and arbitrary masses the region of stability is determined. For the systems (A + A − e −), (pe − C +), (pB − e −), and (D + e − e +), the values of the critical masses of the particles A, B, C, and D are obtained as m A = 2.22m e , m B = 1.49m e , m C = 2.11m e and m D = 4.15m e .

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