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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 Hoo= Eoo Stationary States mo m Time dependent [Ho + V(t)] = iħ/t m o Harry Kroto 2004
Time independent Hoo= Eoo Stationary States mo m Time dependent [Ho + V(t)] = iħ/t V(t) = -Ee(t)e m o Harry Kroto 2004
Time independent Hoo= Eoo Stationary States mo m Time dependent [Ho + V(t)] = iħ/t V(t) = -Ee(t)e Ee (t) = Eeocos2t m o Harry Kroto 2004
Time independent Hoo= Eoo Stationary States mo m Time dependent [Ho + V(t)] = iħ/t V(t) = -Ee(t)e Ee (t) = Eeocos2t Ee(t) Radiation field m o Harry Kroto 2004
Time independent Hoo= Eoo Stationary States mo m Time dependent [Ho + V(t)] = iħ/t V(t) = -Ee(t)e Ee (t) = Eeocos2t Ee(t) Radiation field e Electric dipole moment m o Harry Kroto 2004
Time independent Hoo= Eoo Stationary States mo m Time dependent [Ho + V(t)] = iħ/t V(t) = -Ee(t)e Ee (t) = Eeocos2t Ee(t) Radiation field e Electric dipole moment = mam(t)m m o Harry Kroto 2004
Time independent Hoo= Eoo Stationary States mo m Time dependent [Ho + V(t)] = iħ/t V(t) = -Ee(t)e Ee (t) = Eeocos2t Ee(t) Radiation field e Electric dipole moment = mam(t)m m o Harry Kroto 2004
Time independent Hoo= Eoo Stationary States mo m • Time dependent • [Ho + V(t)] = iħ/t • V(t) = -Ee(t)e • Ee (t) = Eeocos2t • Ee(t) Radiation field • e Electric dipole moment • = mam(t)m am(t) indicates how the population of statem varies in time m o Harry Kroto 2004