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Volumn 79, Issue 10, 2009, Pages

Incoherent Landau-Zener-Stückelberg transitions in single-molecule magnets

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EID: 64849098701     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.79.104423     Document Type: Article
Times cited : (17)

References (39)
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    • For excited states, such processes are important and have been studied extensively in Mn12. For this, see chapter 10 of Ref. and references therein.
    • For excited states, such processes are important and have been studied extensively in Mn12. For this, see chapter 10 of Ref. and references therein.
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    • More precisely, it is conceivable that ηi could vanish for isolated unequal values of t1 and t2, but this would require a coincidence of the directions nI 1 and nI 2 defined in Eq. 10. Such a coincidence can only happen for a measure-zero set of Ki, μi, t1, and t2. It can therefore be regarded as accidental and for all practical purposes we can say that ηi >0 if t12 ≤0.
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    • We were led to think about the points in this paragraph in a correspondence with Jacques Villain and Wolfgang Wernsdorfer.
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    • Even though we do not need it to find /i ηi, the argument that follows provides still more support for our approach. The exp (-b t 12 2) behavior of |F| max can be understood if we note that the weight of the delta functions in the replacements 3 and 17 should be multiplied by another factor (1-Δ | t12 | /π) because the integrals over Ωi- begin from Δ, not 0. (This is readily seen by performing the integrals from 0 to , and from 0 to Δ, and subtracting.) When we make these changes, and fix c according to Eq. 31, we find S1 + S2 - S3 =b | Δ t12 | 2, with b=2.02 Edm / Eb, or just 2.02 if Edm = Eb. Our numerical fits yield b∼2.1-2.8, which is close enough given the crudeness of our estimates.
    • Even though we do not need it to find /i ηi, the argument that follows provides still more support for our approach. The exp (-b t 12 2) behavior of |F| max can be understood if we note that the weight of the delta functions in the replacements 3 and 17 should be multiplied by another factor (1-Δ | t12 | /π) because the integrals over Ωi- begin from Δ, not 0. (This is readily seen by performing the integrals from 0 to, and from 0 to Δ, and subtracting.) When we make these changes, and fix c according to Eq. 31, we find S1 + S2 - S3 =b | Δ t12 | 2, with b=2.02 Edm / Eb, or just 2.02 if Edm = Eb. Our numerical fits yield b∼2.1-2.8, which is close enough given the crudeness of our estimates.


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