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17 Jul 2009: Dulieu, J. Chem. Phys. 122, 204302 (2005)]. R/δ = 0.25 r 200 nm.

9 Nov 2009: ra0. cos θra0. eiφ sin θ. and the symmetry of Ĥ(1), it is clear that only the matrix element = 〈200|Ĥ(1)|210〉 is non-vanishing (and given by = ... H(1)ij =. (0 0. ). Eigenstates: (|200〉 | 210〉)/. 2 with energy linear in E.

28 Oct 2009: and the symmetry of Ĥ(1), it is clear that only the matrix element = 〈200|Ĥ(1)|210〉 is non-vanishing (and given by = 3eEa0).In two-dimensional degenerate subspace spanned ... H(1)ij =. (0 0. )Eigenstates: (|200〉 |210〉)/. 2 with energy linear

9 Nov 2009: 3. –2. –1. 0. 1. 2. 3. 4E /eV. 100 200 300R/pm.

9 Nov 2009: 3. –2. –1. 0. 1. 2. 3. 4E /eV. 100 200 300R/pm.

9 Nov 2009: 3–2–101234E/eV. 100 200 300R/pm. Eu Ry. LCAO Eg RyExact Eg Ry. ##

8 Oct 2009: So the only diagonalization necessary is within the two-dimensional degeneratesubspace spanned by |200〉 and |210〉, i.e. ... Notice that the neweigenstates (|200〉 | 210〉)/. 2 are not eigenstates of the parity operator -- a sketch.

14 Oct 2009: 16.1. PROBLEM SET I 200. for eigenvalues! /2 and! /2 respectively.

3 Nov 2009: REFERENCES. J.S. Bell, "On the Einstein-Podolsky-Rosen Paradox," Physics 1, 195-200 (1964).

22 Jul 2009: That this definition coincides withthe more classical ones follows, for instance, from Meyer (1992, page 200) orSection 9 in Härdle et al.