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A local moment approach to the gapped Anderson model

机译:差距安德森模型的局部矩方法

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We develop a non-perturbative local moment approach (LMA) for the gapped Anderson impurity model (GAIM), in which a locally correlated orbital is coupled to a host with a gapped density of states. Two distinct phases arise, separated by a level-crossing quantum phase transition: a screened singlet phase, adiabatically connected to the non-interacting limit and as such a generalized Fermi liquid (GFL); and an incompletely screened, doubly degenerate local moment (LM) phase. On opening a gap (delta) in the host, the transition occurs at a critical gap delta(c), the GFL [LM] phase occurring for delta delta(c)] . In agreement with numerical renormalization group (NRG) calculations, the critical delta(c) = 0 at the particle-hole symmetric point of the model, where the LM phase arises immediately on opening the gap. In the generic case by contrast delta(c) > 0, and the resultant LMA phase boundary is in good quantitative agreement with NRG results. Local single-particle dynamics are considered in some detail. The major difference between the two phases resides in bound states within the gap: the GFL phase is found to be characterised by one bound state only, while the LM phase contains two such states straddling the chemical potential. Particular emphasis is naturally given to the strongly correlated, Kondo regime of the model. Here, single-particle dynamics for both phases are found to exhibit universal scaling as a function of scaled frequency omega/omega(m) (0) for fixed gaps delta/omega(0)(m), where omega(0)(m) is the characteristic Kondo scale for the gapless (metallic) AIM; at particle-hole symmetry in particular, the scaling spectra are obtained in closed form. For frequencies |omega|/omega(0)(m) delta/omega(0)(m), the scaling spectra are found generally to reduce to those of the gapless, metallic Anderson model; such that for small gaps delta/omega(0)(m) 1 in particular, the Kondo resonance that is the spectral hallmark of the usual metallic Anderson model persists more or less in its entirety in the GAIM.
机译:我们为有间隙的安德森杂质模型(GAIM)开发了一种非微扰局部矩方法(LMA),其中局部相关的轨道耦合到具有状态间隙密度的宿主。出现了两个不同的相,这些相被跨水平的量子相变分隔开:屏蔽的单重态相,绝热连接至非相互作用极限,因此是广义费米液体(GFL)。以及未完全筛选的双简并局部矩(LM)相位。在宿主中打开缺口(delta)时,过渡发生在临界缺口delta(c)处,GFL [LM]相发生于delta delta(c)]。与数值归一化组(NRG)的计算一致,在模型的粒子-孔对称点处的临界delta(c)= 0,其中LM相在打开间隙时立即出现。在一般情况下,对比度为delta(c)> 0,并且所得的LMA相界与NRG结果具有良好的定量一致性。局部单粒子动力学被详细考虑。两相之间的主要区别在于缝隙内的键合状态:发现GFL相仅以一个键合状态为特征,而LM相包含跨越化学势的两个这样的状态。自然地,模型的高度相关的近藤状态自然会得到特别强调。在这里,对于固定间隙delta / omega(0)(m),发现两个相的单粒子动力学都表现出普遍的缩放比例,该比例是缩放频率omega / omega(m)(0)的函数,其中omega(0)(m )是无间隙(金属)AIM的特征近藤标度;特别是在颗粒-孔对称的情况下,缩放光谱以封闭形式获得。对于|ω| /ω(0)(m)δ/ω(0)(m)的频率,通常发现定标谱减小到无间隙的金属安德森模型的定标谱。因此,特别是对于小间隙delta / omega(0)(m) 1而言,作为常见金属安德森模型的光谱特征的近藤共振在GAIM中或多或少地整体存在。

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