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quantum physics.
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from a) to h)
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Consider a spin-1 particle placed in a constant uniform magnetic field along the z-axis. The particle is initially in the sta
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Auf- Â =-MABS = -MeBo $(38= Bî) At t=0, particle is in 11,0% (eigenstade of Sse operator) particle is a spinal pandicle, il,tuet RD (a) Energy eigenvalues of Hamiltonian, IH-EI) 20. · |-Mg Bato - e 0 0 0 - E 30 % E = -MeBo to 0 -E+Mg Botil E. E, =-M(d) (32) =4<1,0|82|1,0%(4) all = (CLEAR VIl-pitting, -1) 32 (piesta 1,- exista 1-2) = [ (inte mi) - pi fila, L, -1) 2*2 (E FA(h) lo 52-ti I 22 1-12h o 10-Ft A: - to o 52 til = 0 11 12 13 | 1 0 o 1 о то for => 1, - 50 ; + =0.p0,2=73 1742 + ola -0. 2 >

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