Результаты исследований: Научные публикации в периодических изданиях › статья › Рецензирование
Schrödinger-like equation for the relativistic few-electron atom. / Shabaev, V. M.
в: Journal of Physics B: Atomic, Molecular and Optical Physics, Том 26, № 24, 28.12.1993, стр. 4703-4718.Результаты исследований: Научные публикации в периодических изданиях › статья › Рецензирование
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TY - JOUR
T1 - Schrödinger-like equation for the relativistic few-electron atom
AU - Shabaev, V. M.
PY - 1993/12/28
Y1 - 1993/12/28
N2 - The equation for the determination of the energy levels and wavefunctions of quasidegenerate states of the relativistic few-electron atom in the form of the usual eigenvalue problem for an energy operator (‘Schrodinger-like equation1) is constructed consistently from quantum electrodynamics (qed). Two choices of the space Ω2, in which the constructed energy operator H acts, are considered. In the first case Ω2 = Ω2 is the space of the fine structure levels. In the second case Ω2 = Ω2b is the space of all the positive energy states which correspond to the non-relativistic region of the spectrum. The construction of H in the Feynman gauge in the first and second (with the precision up to the terms α2(αZ)2m) orders in a is demonstrated for both choices of Ω . An effective expression for the energy operator Hcti, which gives the energy values within am for high Z and within α2(αZ)2m) for low Z, is proposed.
AB - The equation for the determination of the energy levels and wavefunctions of quasidegenerate states of the relativistic few-electron atom in the form of the usual eigenvalue problem for an energy operator (‘Schrodinger-like equation1) is constructed consistently from quantum electrodynamics (qed). Two choices of the space Ω2, in which the constructed energy operator H acts, are considered. In the first case Ω2 = Ω2 is the space of the fine structure levels. In the second case Ω2 = Ω2b is the space of all the positive energy states which correspond to the non-relativistic region of the spectrum. The construction of H in the Feynman gauge in the first and second (with the precision up to the terms α2(αZ)2m) orders in a is demonstrated for both choices of Ω . An effective expression for the energy operator Hcti, which gives the energy values within am for high Z and within α2(αZ)2m) for low Z, is proposed.
UR - http://www.scopus.com/inward/record.url?scp=0000035945&partnerID=8YFLogxK
U2 - 10.1088/0953-4075/26/24/006
DO - 10.1088/0953-4075/26/24/006
M3 - Article
AN - SCOPUS:0000035945
VL - 26
SP - 4703
EP - 4718
JO - Journal of the European Optical Society Part B: Quantum Optics
JF - Journal of the European Optical Society Part B: Quantum Optics
SN - 0953-4075
IS - 24
ER -
ID: 35708717