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A comprehensive and lucid review of the entire field of SMMs is given by D. Gatteschi, R. Sessoli, and J. Villain, Molecular Nanomagnets (Oxford University Press, Oxford, 2006).
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C. Sangregorio, T. Ohm, C. Paulsen, R. Sessoli, and D. Gatteschi, Phys. Rev. Lett. 78, 4645 (1997). Many more examples can be found throughout Ref. 10.1103/PhysRevLett.78.4645
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64849109719
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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.
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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.
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The sum of the inverse sixth power of the distance from a Bravais lattice point to all other lattice points is tabulated for the three cubic lattices in Holt, Rinehart, and Winston, New York
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The sum of the inverse sixth power of the distance from a Bravais lattice point to all other lattice points is tabulated for the three cubic lattices in N. W. Ashcroft and N. D. Mermin, Solid State Physics (Holt, Rinehart, and Winston, New York, 1976). See Table 20.2.
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64849091163
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Note that Bn entails the sum of the magnitudes hi and not the magnitude of the vector sum /i hi si.
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Note that Bn entails the sum of the magnitudes hi and not the magnitude of the vector sum /i hi si.
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29
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0003498504
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Academic, New York
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31
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0001176603
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34
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64849110944
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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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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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35
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35348829349
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10.1103/PhysRevB.76.134405
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E. Keçecioǧlu and A. Garg, Phys. Rev. B 76, 134405 (2007). 10.1103/PhysRevB.76.134405
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Keçecioǧlu, E.1
Garg, A.2
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36
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64849098809
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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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We were led to think about the points in this paragraph in a correspondence with Jacques Villain and Wolfgang Wernsdorfer.
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37
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29844444619
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10.1103/PhysRevB.72.214429
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64849095712
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arXiv:0804.1246 (unpublished).
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W. Wernsdorfer, arXiv:0804.1246 (unpublished).
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Wernsdorfer, W.1
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39
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64849115598
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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.
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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.
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