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Instantons, colloids and convergence of the 1/N expansion for the homogeneous electron gas

机译:用于均相电子气体的1 / N膨胀的偶然型,胶体和收敛性

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We investigate non-perturbative corrections to the large N expansion of the homogeneous electron gas. These are associated with instanton solutions to the effective action of the plasmon field. We show that, although the large field behavior of that action dominates the quadratic bare Coulomb term, there are no solutions at large field, and consequently none at large density. We argue that solutions would exist at low density if the large N theory had a Wigner crystal (WC) phase. However, we argue that this is not the case. Together with the implied convergence of the large N expansion, this implies that the homogeneous electron gas with N component spins and a Coulomb interaction scaling like 1/N can only have a WC phase below a curve in the plane of N and density, which asymptotes to zero density at infinite N. We argue that for systems with a semi-classical expansion for order parameter dynamics, and a first order quantum transition between fluid and crystal phases, there are instantons associated with the decays of meta-stable fluid and crystal phases in the appropriate regions of the phase diagram. We argue that the crystal will decay into one or more colloidal or bubble phases (Kivelson and Spivak, 2006) rather than directly into the fluid. It is possible that the bubble phases remain stable all the way to the density where the crystal solution disappears. The bubbles of fluid will expand as the density is raised and gradually convert the system into a fluid filled with chunks of crystal. The transition to a translationally invariant phase is likely to be second order. Unfortunately, the HEG does not have a crystal phase at large N, where these semi-classical ideas could be examined in detail. We suggest that the evidence for negative dielectric function at intermediate densities for N = 2 is an indicator of this second order transition. While the infinite N limit does not have a negative dielectric function at any density, it is possible that the closed large
机译:我们研究了非扰动校正对均匀电子气的大N扩展。这些与算法解决方案有关,以实现等离子体领域的有效作用。我们展示了,尽管该行动的大场行为主导了二次裸露的库仑术语,但大场没有解决方案,因此没有大密度。我们认为,如果大N理论具有Wigner晶体(WC)相,则解决方案将以低密度存在。但是,我们认为这不是这种情况。与大n扩展的暗示收敛一起,这意味着具有n个组分旋转的均匀电子气体和诸如1 / n的库仑相互作用缩放只能在n和密度平面下具有Wc相,渐近的曲线在无限N处零密度。我们认为,对于具有顺序参数动态的半传统扩展的系统,以及流体和晶相之间的一阶量子过渡,有与元稳定的流体和晶相的衰减相关联在相图的适当区域。我们认为晶体将腐烂进入一个或多个胶体或泡沫阶段(Kivelson和Spivak,2006),而不是直接进入流体。气泡阶段可能一直保持稳定,以晶体溶液消失的密度。由于密度升高并逐渐将该系统逐渐将系统转化为充满晶体的液体,流体的气泡将膨胀。转换到翻译不变阶段可能是秒顺序。不幸的是,HEG在大的N下没有晶相,其中可以详细检查这些半古典思想。我们建议在N = 2的中间密度下对负介质功能的证据是该二阶转变的指标。虽然无限N限制在任何密度都没有负介质功能,但是闭合的大型可能

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