Self Consistent Field Equations for H2 And H3
Self Consistent Field Equations for H2 And H3
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In our eReader you can find the full English version of the book. Read Self Consistent Field Equations for H2 And H3 Online - link to read the book on full screen. Our eReader also allows you to upload and read Pdf, Txt, ePub and fb2 books. In the Mini eReder on the page below you can quickly view all pages of the book - Read Book Self Consistent Field Equations for H2 And H3
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)= l/r, j (5. U) W - H - E, where (U. 7) E - (T, H T) - 3K^ 1^(1 +K^TT )(Hp+ 2H^+ Vp+ 2W^) TT permutes a, b, £ cyclically, and K is a constant given by the condition (U. 3) as follows (5. 5) (¥, T) = 3K^ [d+K^TT )(FF)+ 2K(FG)j -1, where the scalar scalar products (FF) and (FG) are given by equations (8. 3) and (8. 5). The Q . , contain three constants N, N, ,N which are determined from the ^ ij a' b' c subsidiary conditions (3. U).
- 9 - 6. Discussion 6. ] How general is the wave function Y ?
T...his point is discussed in section 1 (see the footnote on p. 2 ). T, as given by the self-consistent field method, is the best powwible wave function that can be obtained as one antisjTtimetrized product of one-electron wave functions; these functions are chosen so that the space symmetry of the problem as a whole is taken into account (to this end we use Y, and Y^ or the factor >t ) . An exact result could be obtained either by taking an infinite set of such Y functions, or by letting the individual a, b, c functions depend on the coordinates of all the particles in an arbitrary way.
What to read after Self Consistent Field Equations for H2 And H3?
You can find similar books in the "Read Also" column, or choose other free books by Ernest Bauer to read onlineMoreLess
To quickly assess the difficulty of the text, read a short excerpt:
)= l/r, j (5. U) W - H - E, where (U. 7) E - (T, H T) - 3K^ 1^(1 +K^TT )(Hp+ 2H^+ Vp+ 2W^) TT permutes a, b, £ cyclically, and K is a constant given by the condition (U. 3) as follows (5. 5) (¥, T) = 3K^ [d+K^TT )(FF)+ 2K(FG)j -1, where the scalar scalar products (FF) and (FG) are given by equations (8. 3) and (8. 5). The Q . , contain three constants N, N, ,N which are determined from the ^ ij a' b' c subsidiary conditions (3. U).
- 9 - 6. Discussion 6. ] How general is the wave function Y ?
T...his point is discussed in section 1 (see the footnote on p. 2 ). T, as given by the self-consistent field method, is the best powwible wave function that can be obtained as one antisjTtimetrized product of one-electron wave functions; these functions are chosen so that the space symmetry of the problem as a whole is taken into account (to this end we use Y, and Y^ or the factor >t ) . An exact result could be obtained either by taking an infinite set of such Y functions, or by letting the individual a, b, c functions depend on the coordinates of all the particles in an arbitrary way.
What to read after Self Consistent Field Equations for H2 And H3?
You can find similar books in the "Read Also" column, or choose other free books by Ernest Bauer to read onlineMoreLess
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