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Biological Utilisation of Quantum NonLocality
www.tcm.phy.cam.ac.uk/~bdj10/papers/bell.html3 Nov 2009: REFERENCES. J.S. Bell, "On the Einstein-Podolsky-Rosen Paradox," Physics 1, 195-200 (1964). -
dipole_pwave_dresden.dvi
www.tcm.phy.cam.ac.uk/~nrc25/SEMINARS/dipole_pwave_dresden.pdf17 Jul 2009: Dulieu, J. Chem. Phys. 122, 204302 (2005)]. R/δ = 0.25 r 200 nm. -
16.1. PROBLEM SET I 197 Answers: Problem set I ...
www.tcm.phy.cam.ac.uk/~bds10/aqp/ans1.pdf14 Oct 2009: 16.1. PROBLEM SET I 200. for eigenvalues! /2 and! /2 respectively. -
lectures
www.tcm.phy.cam.ac.uk/~bds10/aqp/lec15_compressed.pdf9 Nov 2009: 3. –2. –1. 0. 1. 2. 3. 4E /eV. 100 200 300R/pm. -
lectures
www.tcm.phy.cam.ac.uk/~bds10/aqp/lec15.pdf9 Nov 2009: 3. –2. –1. 0. 1. 2. 3. 4E /eV. 100 200 300R/pm. -
lectures
www.tcm.phy.cam.ac.uk/~bds10/aqp/lec8-10_compressed.pdf9 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. -
Chapter 7 Approximation methods forstationary states 7.1…
www.tcm.phy.cam.ac.uk/~bds10/aqp/handout_approx.pdf8 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. -
Synopsis: Lectures 5-10 5 Charged particle in an electromagnetic ...
www.tcm.phy.cam.ac.uk/~bds10/aqp/lec8-10.pdf28 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 -
Chapter 10 From molecules to solids In the previous ...
www.tcm.phy.cam.ac.uk/~bds10/aqp/handout_molecular.pdf9 Nov 2009: 3–2–101234E/eV. 100 200 300R/pm. Eu Ry. LCAO Eg RyExact Eg Ry. ##
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