arXivDaily arXiv每日学术速递 周一至周五更新
arXiv 1305.3263cond-mat.str-elcond-mat.mes-hall
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磁性振动分子的非平衡输运

Nonequilibrium transport through magnetic vibrating molecules

P. Roura-Bas, L. Tosi, A. A. Aligia

摘要:

我们计算了通过分子或量子点的非平衡电导,其中相关电子能级的占据与强度$λ$耦合到声子模,也耦合到两个导电引线。该系统由Anderson-Holstein Hamilton描述。我们使用Keldysh形式主义和非交叉近似(NCA)的电子-电子和电子-声子相互作用解决了这个问题。我们得到了一个温和的降低近藤温度$T_K$与$λ$固定重整化能量的局域化水平$\tilde{E_d}$。论述了$\tilde{E_d}$的意义和价值。定域电子的谱密度显示除了宽度为$2 T_K$的近藤峰外,该峰的伴峰移动了声子频率$ ω_0$的倍数。非平衡电导作为偏置电压$V_b$的函数,在小的温度下,也显示在$ω_0$的倍数峰除了中央占主导地位的近藤峰附近的$V_b=0$。

英文摘要:

We calculate the nonequilibrium conductance through a molecule or a quantum dot in which the occupation of the relevant electronic level is coupled with intensity $λ$ to a phonon mode, and also to two conducting leads. The system is described by the Anderson-Holstein Hamiltonian. We solve the problem using the Keldysh formalism and the non-crossing approximation (NCA) for both, the electron-electron and the electron-phonon interactions. We obtain a moderate decrease of the Kondo temperature $T_K$ with $λ$ for fixed renormalized energy of the localized level $\tilde{E_d}$. The meaning and value of $\tilde{E_d}$ are discussed. The spectral density of localized electrons shows in addition to the Kondo peak of width $2 T_K$, satellites of this peak shifted by multiples of the phonon frequency $ ω_0$. The nonequilibrium conductance as a function of bias voltage $V_b$ at small temperatures, also displays peaks at multiples of $ω_0$ in addition to the central dominant Kondo peak near $V_b=0$.

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