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Nonrelativistic Operators for Relativistic Transition Rates

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Figure

Figure 4.1: This diagram illustrates the Hylleras-Undheim-MacDonald theorem [1, 2].The Ei are the exact eigenvalues of H, and the λi are the variational eigenvalues fora N-dimensional basis set.The previous N eigenvalues lie between the new N+1eigenvalues as N increases
Figure 5.1: This diagram shows the energy spectrum for the 1s pseudostates forhighest power 10, for both triangular and linear basis
Figure 5.4:Plot of the deviation of the�Nn=1�Ψ(0)n |pz|Ψ(0)2p��
Figure 5.5: Plot of the analytic Ψ(1)1s and the Ψ(1)1s (for r = 0.1..20) obtained frompseudostates using a triangular basis set with a λ = 14 and a highest power of 6
+2

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