Fabrizio Michele
International School for Advanced Studies (SISSA), Via Bonomea 265, I-34136 Trieste, Italy.
Phys Rev B. 2017 Feb 28;95(7). doi: 10.1103/PhysRevB.95.075156.
We present a simple scheme to evaluate linear response functions including quantum fluctuation corrections on top of the Gutzwiller approximation. The method is derived for a generic multiband lattice Hamiltonian without any assumption about the dynamics of the variational correlation parameters that define the Gutzwiller wavefunction, and which thus behave as genuine dynamical degrees of freedom that add on those of the variational uncorrelated Slater determinant. We apply the method to the standard half-filled single-band Hubbard model. We are able to recover known results, but, as by-product, we also obtain few novel ones. In particular, we show that quantum fluctuations can reproduce almost quantitatively the behaviour of the uniform magnetic susceptibility uncovered by dynamical mean field theory, which, though enhanced by correlations, is found to be smooth across the paramagnetic Mott transition. By contrast, the simple Gutzwiller approximation predicts that susceptibility to diverge at the transition.
我们提出了一种简单的方案来评估线性响应函数,该方案包括在古兹维勒近似基础上的量子涨落修正。该方法是针对一般的多带晶格哈密顿量推导出来的,对于定义古兹维勒波函数的变分相关参数的动力学没有任何假设,因此这些参数表现为真正的动力学自由度,它们附加在变分不相关的斯莱特行列式的自由度之上。我们将该方法应用于标准的半填充单带哈伯德模型。我们能够恢复已知结果,但作为副产品,我们也获得了一些新的结果。特别是我们表明,量子涨落几乎可以定量地再现动态平均场理论所揭示的均匀磁化率的行为,尽管该行为因关联而增强,但发现在顺磁莫特转变过程中是平滑的。相比之下,简单的古兹维勒近似预测磁化率在转变处发散。