Consider a physical system whose three-dimensional state space is spanned by the orthonormal basis formed by the three kets {le1>, Je2>, Je3>}. In the basis of these three vectors, taken in this order, the Hamiltonian H^ and the two operators B^ and D° are defined by: i 0 H= hwo -i 3 0 0 2 3 7 i 1- 1 2a B= bo 7 1+i 2a 1+i 1-i 6. 2a -3a where wo and bo are constants. Also using this ordered basis, the initial state of the system is given by: (e1| v(0) (e2] #(0)) (e3] v(0) |»(0)) = 3 6.
Consider a physical system whose three-dimensional state space is spanned by the orthonormal basis formed by the three kets {le1>, Je2>, Je3>}. In the basis of these three vectors, taken in this order, the Hamiltonian H^ and the two operators B^ and D° are defined by: i 0 H= hwo -i 3 0 0 2 3 7 i 1- 1 2a B= bo 7 1+i 2a 1+i 1-i 6. 2a -3a where wo and bo are constants. Also using this ordered basis, the initial state of the system is given by: (e1| v(0) (e2] #(0)) (e3] v(0) |»(0)) = 3 6.
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