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首页> 外文期刊>Physical review. B, Condensed Matter And Materials Physics >Jahn-Teller effect versus Hund's rule coupling in C_(60)~(N-)
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Jahn-Teller effect versus Hund's rule coupling in C_(60)~(N-)

机译:C_(60)〜(N-)中的Jahn-Teller效应与Hund规则耦合

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We propose variational states for the ground state and the low-energy collective rotator excitations in negatively charged C_(60)~(N-) ions (N= 1,... ,5). The approach includes the linear electron-phonon coupling and the Coulomb interaction on the same level. The electron-phonon coupling is treated within the effective mode approximation which yields the linear t_(1u) directX H_g Jahn-Teller problem whereas the Coulomb interaction gives rise to Hund's rule coupling for N=2,3,4. The Hamiltonian has accidental SO(3) symmetry which allows an elegant formulation in terms of angular momenta. Trial states are constructed from coherent states and using projection operators onto angular momentum subspaces which results in good variational states for the complete parameter range. The evaluation of the corresponding energies is to a large extent analytical. We use the approach for a detailed analysis of the competition between Jahn-Teller effect and Hund's rule coupling, which determines the spin state for N= 2,3,4. We calculate the low-spin-high-spin gap for N= 2,3,4 as a function of the Hund's rule coupling constant J. We find that the experimentally measured gaps suggest a coupling constant in the range J=60-80 meV. Using a finite value for J, we recalculate the ground state energies of the C_(60)~(N-) ions and find that the Jahn-Teller energy gain is partly counterbalanced by the Hund's rule coupling. In particular, the ground state energies for N=2,3,4 are almost equal.
机译:我们提出了带负电的C_(60)〜(N-)离子(N = 1,...,5)中基态和低能集体转子激发的变分态。该方法包括在相同水平上的线性电子-声子耦合和库仑相互作用。电子-声子耦合在有效模态近似范围内处理,从而产生线性t_(1u)directX H_g Jahn-Teller问题,而库仑相互作用产生N = 2,3,4的Hund规则耦合。哈密​​顿量具有偶然的SO(3)对称性,因此可以根据角动量进行优雅的表述。试验状态是从相干状态构造的,并使用投影算符到角动量子空间上,这为整个参数范围提供了良好的变化状态。相应能量的评估在很大程度上是分析性的。我们使用该方法详细分析了Jahn-Teller效应与Hund规则耦合之间的竞争,后者确定了N = 2,3,4的自旋状态。我们计算了N = 2,3,4时的低自旋-高自旋间隙,作为汉德法则耦合常数J的函数。我们发现,实验测量的间隙表明耦合常数在J = 60-80 meV的范围内。使用J的有限值,我们重新计算了C_(60)〜(N-)离子的基态能量,发现Jahn-Teller能量增益被洪德法则耦合部分抵消。特别地,对于N = 2、3、4,基态能量几乎相等。

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