کد مقاله | کد نشریه | سال انتشار | مقاله انگلیسی | نسخه تمام متن |
---|---|---|---|---|
4964500 | 1447810 | 2017 | 27 صفحه PDF | دانلود رایگان |
عنوان انگلیسی مقاله ISI
On the calculation of ÎãSË2ã for electronic excitations in time-dependent density-functional theory
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موضوعات مرتبط
مهندسی و علوم پایه
شیمی
شیمی تئوریک و عملی
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چکیده انگلیسی
Excited states are often treated within the context of time-dependent (TD) density-functional theory (DFT), making it important to be able to assign the excited spin-state symmetry. While there is universal agreement on how ÎãSË2ã, the difference between ãSË2ã for ground and excited states, should be calculated in a wave-function-like formalism such as the Tamm-Dancoff approximation (TDA), confusion persists as to how to determine the spin-state symmetry of excited states in TD-DFT. We try to clarify the origins of this confusion by examining various possibilities for the parameters (Ï1,Ï2) in the formula ÎãSË2ã=[ÎãSËTDA2ã(Xâ)+ÎãSËTDA2ã(Yââ)+Ï1ÎãSËmixed2ã(Xâ,Yââ)]/(Xââ Xâ+Ï2Yââ Yâ), where Xâ is the particle-hole part and Yâ is the hole-particle part of the response theory vector. A first principles derivation leads directly to (Ï1,Ï2)=(+1,â1) which we argue is the best simple formula linking spin with energy, albeit approximately. On the other hand, if the desire is to recover wave-function-like values of ÎãSË2ã, then we argue that the choice (Ï1,Ï2)=(+1,+1) should be made. Additional examples are offered to justify that the choice of Ï1=0 should also be made when seeking wave-function-like values of ÎãSË2ã.
ناشر
Database: Elsevier - ScienceDirect (ساینس دایرکت)
Journal: Computer Physics Communications - Volume 213, April 2017, Pages 72-91
Journal: Computer Physics Communications - Volume 213, April 2017, Pages 72-91
نویسندگان
Hemanadhan Myneni, Mark E. Casida,