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Instead of using the bulk magnetization M z 2, one may introduce thermal average of the square of the local magnetization along the applied field M z 2. However, this quantity neither gives zero for the low-field limit, nor can be expressed in terms of other measurable bulk quantities. Thus we use M z 2 in the following discussion.
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Instead of using the bulk magnetization M z 2, one may introduce thermal average of the square of the local magnetization along the applied field M z 2. However, this quantity neither gives zero for the low-field limit, nor can be expressed in terms of other measurable bulk quantities. Thus we use M z 2 in the following discussion.
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