<oai_dc:dc xmlns:dc="http://purl.org/dc/elements/1.1/" xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/ http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
  <dc:creator>Nilsson, Fredrik</dc:creator>
  <dc:creator>Boehnke, Lewin</dc:creator>
  <dc:creator>Werner, Philipp</dc:creator>
  <dc:creator>Aryasetiawan, Ferdi</dc:creator>
  <dc:date>2017-09-21</dc:date>
  <dc:description xmlns:ns0="xml" ns0:lang="en">We discuss a parameter-free and computationally efficient ab initio simulation  approach for moderately and strongly correlated materials, the multitier self-consistent  GW+EDMFT method. This scheme treats different degrees of freedom, such as high- energy and low-energy bands, or local and nonlocal interactions, within appropriate  levels of approximation, and provides a fully self-consistent description of correlation  and screening effects in the solid. The ab initio input is provided by a one-shot G0W0  calculation, while the strong-correlation effects originating from narrow bands near the  Fermi level are captured by a combined GW plus extended dynamical mean-field  (EDMFT) treatment. We present the formalism and technical details of our  implementation and discuss some general properties of the effective EDMFT impurity  action. In particular, we show that the retarded impurity interactions can have  noncausal features, while the physical observables, such as the screened interactions  of the lattice system, remain causal. As a first application, we present ab initio  simulation results for SrMoO3, which demonstrate the existence of prominent plasmon  satellites in the spectral function not obtainable within LDA+DMFT, and provide further  support for our recent reinterpretation of the satellite features in the related cubic  perovskite SrVO3. We then turn to stretched sodium as a model system to explore the  performance of the multitier self-consistent GW+EDMFT method in situations with  different degrees of correlation. While the results for the physical lattice spacing a0  show that the scheme is not very accurate for electron-gas-like systems, because  nonlocal corrections beyond GW are important, it does provide physically correct  results in the intermediate correlation regime, and a Mott transition around a lattice  spacing of 1.5a0. Remarkably, even though the Wannier functions in the stretched  compound are less localized, and hence the bare interaction parameters are reduced,  the self-consistently computed impurity interactions show the physically expected  trend of an increasing interaction strength with increasing lattice spacing.</dc:description>
  <dc:format>application/pdf</dc:format>
  <dc:identifier>https://folia.unifr.ch/global/documents/306290</dc:identifier>
  <dc:identifier>https://folia.unifr.ch/documents/306290/files/wer_msc.pdf</dc:identifier>
  <dc:language>eng</dc:language>
  <dc:relation>info:eu-repo/semantics/altIdentifier/doi/10.1103/PhysRevMaterials.1.043803</dc:relation>
  <dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
  <dc:rights>License undefined</dc:rights>
  <dc:source>Physical Review Materials. - 2017, vol. 1, no. 4, p. 043803</dc:source>
  <dc:subject>info:eu-repo/classification/udc/53</dc:subject>
  <dc:title xmlns:ns1="xml" ns1:lang="en">Multitier self-consistent $GW+\text{EDMFT}$</dc:title>
  <dc:type>http://purl.org/coar/resource_type/c_6501</dc:type>
</oai_dc:dc>
