Time independent Hoo = Eoo Stationary States mo  m

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Presentation transcript:

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

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

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

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

e Electric dipole moment Time independent Hoo = Eoo Stationary States mo  m Time dependent [Ho + V(t)] = iħ/t V(t) = -Ee(t) e Ee (t) = Eeocos 2t Ee(t) Radiation field e Electric dipole moment m  o Harry Kroto 2004

e Electric dipole moment  = mam(t) m Time independent Hoo = Eoo Stationary States mo  m Time dependent [Ho + V(t)] = iħ/t V(t) = -Ee(t) e Ee (t) = Eeocos 2t Ee(t) Radiation field e Electric dipole moment  = mam(t) m m  o Harry Kroto 2004

e Electric dipole moment  = mam(t) m Time independent Hoo = Eoo Stationary States mo  m Time dependent [Ho + V(t)] = iħ/t V(t) = -Ee(t) e Ee (t) = Eeocos 2t Ee(t) Radiation field e Electric dipole moment  = mam(t) m m  o Harry Kroto 2004

e Electric dipole moment = mam(t) m Time independent Hoo = Eoo Stationary States mo  m Time dependent [Ho + V(t)] = iħ/t V(t) = -Ee(t) e Ee (t) = Eeocos 2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