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Time independent H o  o = E o  o Stationary States  m o   m 

Time independent H o  o = E o  o Stationary States  m o   m . Time dependent [H o + V(t)] = i ħ /t.  m   o . Harry Kroto 2004. Time independent H o  o = E o  o Stationary States  m o   m . Time dependent [H o + V(t)] = i ħ /t V(t) = -E e ( t )  e.

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Time independent H o  o = E o  o Stationary States  m o   m 

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  1. Time independent Hoo= Eoo Stationary States mo m Time dependent [Ho + V(t)] = iħ/t m  o Harry Kroto 2004

  2. Time independent Hoo= Eoo Stationary States mo m Time dependent [Ho + V(t)] = iħ/t V(t) = -Ee(t)e m  o Harry Kroto 2004

  3. Time independent Hoo= Eoo Stationary States mo m Time dependent [Ho + V(t)] = iħ/t V(t) = -Ee(t)e Ee (t) = Eeocos2t m  o Harry Kroto 2004

  4. Time independent Hoo= Eoo Stationary States mo m Time dependent [Ho + V(t)] = iħ/t V(t) = -Ee(t)e Ee (t) = Eeocos2t Ee(t) Radiation field m  o Harry Kroto 2004

  5. Time independent Hoo= Eoo Stationary States mo m Time dependent [Ho + V(t)] = iħ/t V(t) = -Ee(t)e Ee (t) = Eeocos2t Ee(t) Radiation field e Electric dipole moment m  o Harry Kroto 2004

  6. Time independent Hoo= Eoo Stationary States mo m Time dependent [Ho + V(t)] = iħ/t V(t) = -Ee(t)e Ee (t) = Eeocos2t Ee(t) Radiation field e Electric dipole moment = mam(t)m m  o Harry Kroto 2004

  7. Time independent Hoo= Eoo Stationary States mo m Time dependent [Ho + V(t)] = iħ/t V(t) = -Ee(t)e Ee (t) = Eeocos2t Ee(t) Radiation field e Electric dipole moment = mam(t)m m  o Harry Kroto 2004

  8. Time independent Hoo= Eoo Stationary States mo m • Time dependent • [Ho + V(t)] = iħ/t • V(t) = -Ee(t)e • Ee (t) = Eeocos2t • Ee(t) Radiation field • e Electric dipole moment • = mam(t)m am(t) indicates how the population of statem varies in time m  o Harry Kroto 2004

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