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85038294511
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Classical spin vectors are denoted without a caret
-
Classical spin vectors are denoted without a caret.
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32
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85038305794
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-
order to obtain reliable results for the magnetization (Formula presented) with instanton techniques, one needs anisotropies as large as (Formula presented) in (Formula presented) wheels. These values are larger than, but of the same order of magnitude as, the ones of the clusters synthesized so far
-
In order to obtain reliable results for the magnetization (Formula presented) with instanton techniques, one needs anisotropies as large as (Formula presented) in (Formula presented) wheels. These values are larger than, but of the same order of magnitude as, the ones of the clusters synthesized so far.
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-
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33
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85038307142
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Terms (Formula presented) can be neglected
-
Terms (Formula presented) can be neglected.
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-
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35
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85038272876
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-
(Formula presented) for (Formula presented) holds as long as (Formula presented) independent of the magnitude of (Formula presented)
-
(Formula presented) for (Formula presented) holds as long as (Formula presented) independent of the magnitude of (Formula presented)
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37
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85038317106
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The absolute value of (Formula presented) deviates from (Formula presented) by terms of order (Formula presented) which is beyond the precision of our result, Eq. (35). Hence we compare ED and analytical results only for (Formula presented) for which this shift nearly cancels
-
The absolute value of (Formula presented) deviates from (Formula presented) by terms of order (Formula presented) which is beyond the precision of our result, Eq. (35). Hence we compare ED and analytical results only for (Formula presented) for which this shift nearly cancels.
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41
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85038300234
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Note that the classical value for (Formula presented) at the saddle points of the path integral, φ=π/2 and 3π/2, respectively, coincides with the value derived from the classical vector model in Sec. III, as it should
-
Note that the classical value for (Formula presented) at the saddle points of the path integral, φ=π/2 and 3π/2, respectively, coincides with the value derived from the classical vector model in Sec. III, as it should.
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-
43
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85038267164
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Terms proportional to (Formula presented) in (Formula presented) lead only to small contributions of order (Formula presented) to (Formula presented) This allows us to neglect the term (Formula presented) [Eq. (42)]
-
Terms proportional to (Formula presented) in (Formula presented) lead only to small contributions of order (Formula presented) to (Formula presented) This allows us to neglect the term (Formula presented) [Eq. (42)].
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44
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85038283483
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However, we do not claim that this is an indication that our ansatz, Eq. (26), provides a full microscopic description of the local spin directions
-
However, we do not claim that this is an indication that our ansatz, Eq. (26), provides a full microscopic description of the local spin directions.
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45
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85038346686
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Note that also the anisotropy energy favors a spin configuration as sketched in Fig. 33(c) such that the condition (Formula presented) can be relaxed. Consequently, also for Ga dopants a tunneling scenario is feasible
-
Note that also the anisotropy energy favors a spin configuration as sketched in Fig. 33(c) such that the condition (Formula presented) can be relaxed. Consequently, also for Ga dopants a tunneling scenario is feasible.
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46
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0001252161
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85038295366
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cond-mat/0106579 (unpublished)
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Rumberger, E.7
Hendrikson, D.N.8
Christou, G.9
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