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Published byConrad Dawson Modified over 5 years ago
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If is an orthonormal wavefunction ∫* dτ = 1
∫*H dτ ≥ Eo is either o or an excited state with eigenvalue > Eo ∫* (H – Eo) dτ = ∫* H dτ – Eo∫* dτ = ∫* H dτ – Eo = Σiciφi ∫* (H – Eo) dτ = ∫ (Σici* φi * ) (H – Eo) (Σiciφi) dτ Harry Kroto 2004 2
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Since the φi’s are eigenfunctions of H … ie ∫φi*Hφidτ = Ei
∫* (H – Eo) dτ = ∫ (Σici* φi * ) (H – Eo) (Σiciφi) dτ = Σici* ci (Ei – Eo) All the ci* ci are positive numbers and by definition Ei ≥ Eo ∫* (H – Eo) dτ ≥ 0 ∫*H dτ ≥ Eo Thus the Variation Principle states that no calculated wavefunction can have an eigenvalue greater than the experimentally determined eigenvalue 3
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Herzberg and Monfils obtained 36 113.6
I just got Herzberg and Monfils obtained Kolos and Wolniewicz calculated Herzberg between – 4
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Since the φi’s are eigenfunctions of H … ie
∫* (H – Eo) dτ = ∫ (Σici* φi * ) (H – Eo) (Σiciφi) dτ Since the φi’s are eigenfunctions of H … ie ∫φi*Hφidτ = Ei ∫* (H – Eo) dτ = ∫ (Σici* φi * ) Σi (Ei – Eo) (Σiciφi) dτ = Σici* ci (Ei – Eo) ∫* (H – Eo) dτ ≥ 0 ∫*H dτ ≥ Eo 6
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¾ ( ) = ¾ R 7
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¾ ( ) = ¾ R 8
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Herzberg and Monfils obtained 36 113.6
¾ ( ) = ¾ R I get Herzberg and Monfils obtained Kolos and Wolniewicz calculated Herzberg between – 9
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Men’n” Franck Condon II Harry Kroto 2004 10
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