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Volumn 61, Issue 3, 2000, Pages 355021-3550213

Nuclear octupole correlations and the enhancement of atomic time-reversal violation

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EID: 12944300327     PISSN: 05562813     EISSN: 1089490X     Source Type: Journal    
DOI: 10.1103/PhysRevC.61.035502     Document Type: Article
Times cited : (89)

References (38)
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    • R.P. Feynman, Phys. Rev. 56, 340 (1939); H. Hellmann, Einfuhrung in die Quantumchemie (Franz Deuticke, Leipzig, 1937), p. 285. The usual statement of the theorem is that if a Hamiltonian H(λ) depends on a parameter λ, the energy shift E(λ) for that Hamiltonian satisfies ∂E(λ)/∂λ = 〈ψ(λ)|∂H(λ)/∂λ|ψ(λ)〉. If one performs a unitary transformation so that H(λ) = exp(iλU)H(0)exp(-iλU), uses the theorem and then sets λ to zero, one finds ∂E(0)/∂λ ≡ 0 = i〈[U,H(0)]〉, since there can be no energy shift from a unitary transformation. Our quantity Δ in Eqs. (6) and (21) is given by this relationship.
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    • Feynman, R.P.1
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    • Franz Deuticke, Leipzig
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    • (1937) Einfuhrung in Die Quantumchemie , pp. 285
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* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.