The effective operator for atomic level widths due to l(1)(N)(1)l(2)(N2)-> l(1)(1)(N)(+1)l(2)(2)(epsilon l3)(N)(-2) Auger transitions

Merkelis G

首页> 外文期刊>Physica Scripta: An International Journal for Experimental and Theoretical Physics >The effective operator for atomic level widths due to l(1)(N)(1)l(2)(N2)-> l(1)(1)(N)(+1)l(2)(2)(epsilon l3)(N)(-2) Auger transitions

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The effective operator for atomic level widths due to l(1)(N)(1)l(2)(N2)-> l(1)(1)(N)(+1)l(2)(2)(epsilon l3)(N)(-2) Auger transitions

机译：由于l（1）（N）（1）l（2）（N2）-> l（1）（1）（N）（+ 1）l（2）（2）（ epsilon l3）（N）（-2）俄歇过渡

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The effective operator A(Gamma) for the Auger l(1)(N1)l(2)(N2)-> l(1)(N1+1)l(2)(N2-2)epsilon l(3) transitions was determined in the nonrelativistic approximation in the second quantization representation in the case of normal ordering of electron creation and annihilation operators. The matrix element of A 0 yields a partial Auger width of a level. The specific transitions when l(2) = 1, 2 and l(1) > 0 were considered in detail. The general formula for a matrix element of A 0 was derived when a wavefunction with open-shells was presented in normal coupling. Compact expressions for the matrix elements of A(Gamma) in the case l(1)(N1)l(2)(2) when N-1 = 1, 2, 4l(1) + 1 and 4l(1) were obtained. The selection rules for matrix elements of A(Gamma) are discussed by using the quasispin technique.

机译：俄歇l（1）（N1）l（2）（N2）-> l（1）（N1 + 1）l（2）（N2-2）εl（3）跃迁的有效算符A（Gamma）在电子生成和an灭算符的正常排序的情况下，在第二个量化表示形式的非相对论近似中确定。 A 0的矩阵元素会产生电平的部分俄歇宽度。详细考虑了当l（2）= 1、2和l（1）> 0时的特定跃迁。当法向耦合中存在具有开壳的波函数时，得出A 0的矩阵元素的通式。当N-1 = 1、2、4l（1）+ 1和4l（1）时，获得了l（1）（N1）l（2）（2）情况下A（γ）矩阵元素的紧凑表达式。。利用准四边形技术讨论了A（Gamma）矩阵元素的选择规则。

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《Physica Scripta: An International Journal for Experimental and Theoretical Physics》 |2006年第3期|共10页
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Merkelis G;
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正文语种 eng
中图分类物理学;
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SPECTRA;

机译：规格;

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1. The effective operator for atomic level widths due to l(1)(N)(1)l(2)(N2)-> l(1)(1)(N)(+1)l(2)(2)(epsilon l3)(N)(-2) Auger transitions [J] . Merkelis G Physica Scripta: An International Journal for Experimental and Theoretical Physics . 2006,第3期

机译：由于l（1）（N）（1）l（2）（N2）-> l（1）（1）（N）（+ 1）l（2）（2）（ epsilon l3）（N）（-2）俄歇过渡
2. Reexamination of M_(2,3) atomic level widths and L_1M_(2,3) transition energies of elements 69 ≤ Z ≤ 95 [J] . K. Fennane, M. Berset, J.-Cl. Dousse, Physical Review, A. Atomic, molecular, and optical physics . 2013,第5aPta1期

机译：重新检查元素69≤Z≤95的M_（2,3）原子能级宽度和L_1M_（2,3）跃迁能
3. The effect of an external magnetic field on the L3 subshell fluorescence yields and level widths for Ta, W, Tl, Th and U at 59.54 keV photons [J] . D. Demir, Y. Sahin The European physical journal, D. Atomic, molecular, and optical physics . 2007,第1期

机译：外磁场对59.54 keV光子的Ta，W，Tl，Th和U的L3子壳荧光产量和能级宽度的影响
4. Levels width in triple-barrier structures in two-photon transitions [C] . Kapralova A. A., Pashkovskiy A. B. 2011 21th International Crimean Conference Microwave and Telecommunication Technology . 2011

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5. Multiple scale K-epsilon turbulence modeling of the transitional boundary layer for elevated freestream turbulence levels. [D] . Wu, Sheng-Yi. 1995

机译：过渡边界层的多尺度K-ε湍流建模，用于提高自由流湍流水平。
6. Effects of the atomic level shift in the Auger neutralization rates of noble metal surfaces [O] . R.C. Monreal, D. Goebl, D. Primetzhofer, -1

机译：原子能级移动对贵金属表面俄歇中和速率的影响
7. Selection rules for effective intra-atomic and optical transition operators in partly-filled shell ions [O] . Wang Qingsheng 1993

机译：在部分填充的壳离子中有效的原子内和光学跃迁算符的选择规则

The effective operator for atomic level widths due to l(1)(N)(1)l(2)(N2)-> l(1)(1)(N)(+1)l(2)(2)(epsilon l3)(N)(-2) Auger transitions

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