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Quantum electrodynamical density-functional theory: Bridging quantum optics and electronic-structure theory

机译:量子电动力学密度泛函理论:桥接量子光学和电子结构理论

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摘要

In this work we give a comprehensive derivation of an exact and numerically feasible method to perform ab-initio calculations of quantum particles interacting with a quantized electromagnetic field. We present a hierachy of density-functional-type theories that describe the interaction of charged particles with photons and introduce the appropriate Kohn-Sham schemes. We show how the evolution of a system described by quantum electrodynamics in Coulomb gauge is uniquely determined by its initial state and two reduced quantities. These two fundamental observables, the polarization of the Dirac field and the vector potential of the photon field, can be calculated by solving two coupled, non-linear evolution equations without the need to explicitly determine the (numerically infeasible) many-body wave function of the coupled quantum system. To find reliable approximations to the implicit functionals we present the according Kohn-Sham construction. In the non-relativistic limit this density-functional-type theory of quantum electrodynamics reduces to the density-functional reformulation of the Pauli-Fierz Hamiltonian, which is based on the current density of the electrons and the vector potential of the photon field. By making further approximations, e.g. restricting the allowed modes of the photon field, we derive further density functional-type theories of coupled matter-photon systems for the corresponding approximate Hamiltonians. In the limit of only two sites and one mode we deduce the according effective theory for the two-site Hubbard model coupled to one photonic mode. This model system is used to illustrate the basic ideas of a density-functional reformulation in great detail and we present the exact Kohn-Sham potentials for our coupled matter-photon model system.
机译:在这项工作中,我们给出了一种精确且在数值上可行的方法的综合推导,以执行与量子电磁场相互作用的量子粒子的从头算。我们提出了一种密度泛函型理论,描述了带电粒子与光子的相互作用,并介绍了适当的Kohn-Sham方案。我们展示了如何用库仑规中的量子电动力学描述的系统的演化是由其初始状态和两个减少的量唯一地确定的。这两个基本的可观测值,狄拉克场的极化和光子场的矢量势,可以通过求解两个耦合的非线性演化方程来计算,而无需明确地确定(在数值上不可行的)多体波函数。耦合量子系统。为了找到隐式函数的可靠近似,我们介绍了相应的Kohn-Sham构造。在非相对论的极限中,这种量子电动力学的密度函数式理论简化为泡利-费兹哈密顿量的密度函数重新公式化,其基于电子的电流密度和光子场的矢量势。通过进一步近似,例如限制光子场的允许模式,我们推导了相应的近似哈密顿量的耦合物质-光子系统的进一步的密度泛函型理论。在只有两个位点和一个模式的限制下,我们推论了耦合到一个光子模式的两个位点的哈伯德模型的有效理论。该模型系统用于详细说明密度泛函的基本概念,我们给出了耦合物质-光子模型系统的精确Kohn-Sham势。

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