Reply to the comment of Chudnovsky & Garanin on ” Spin re - laxation in Mn 12 - acetate ”

نویسنده

  • Michael N. Leuenberger
چکیده

Angular momentum conservation is a physical law that must be obeyed in any closed system. However, it is well known from standard textbooks that in the case of interactions with phonons a part of the total momentum and of the total angular momentum can be absorbed by the whole crystal and is then no longer considered (cf. e.g. the Mössbauer effect[1] and the Umklapp process[2]). Therefore, there is no such general reason why the spin-phonon couplings g 1 (ǫ xx − ǫ yy) ⊗ (S 2 x − S 2 y) + 1 2 g 2 ǫ xy ⊗ {S x , S y } (1) must vanish in the spin-phonon Hamiltonian H sp (see Eq. (6) in Ref. [7]) due to angular momentum conservation as incorrectly claimed in Ref. [3]. Both terms in Eq. (1) were used e.g. in Refs. [4], [5], [6], and [7] to describe phonon-assisted tunneling in Mn 12. Furthermore, such terms were derived in Refs. [8] and [9] many years ago by means of perturbation theory: These authors combined two spin-orbit interactions H SO = λL · S with one orbit-lattice interaction H OL , which yields a third-order term of the form[8] j,k

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تاریخ انتشار 2000