Advanced Calculations for Defects in Materials 2011
DOI: 10.1002/9783527638529.ch3
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Electronic Properties of Interfaces and Defects from Many‐Body Perturbation Theory: Recent Developments and Applications

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Cited by 10 publications
(18 citation statements)
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“…At present, the BSE represents the most accurate approach for the ab initio study of neutral excitations in crystalline systems as it includes the attractive interaction between electrons and holes thus going beyond the random-phase approximation (RPA) employed in the GW approximation. In what follows, we mainly focus on the BSE implementation as the features of the GW part have been already discussed in the last ABINIT paper [8] and in the review article [79].…”
Section: Developments In Excited State Calculationsmentioning
confidence: 99%
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“…At present, the BSE represents the most accurate approach for the ab initio study of neutral excitations in crystalline systems as it includes the attractive interaction between electrons and holes thus going beyond the random-phase approximation (RPA) employed in the GW approximation. In what follows, we mainly focus on the BSE implementation as the features of the GW part have been already discussed in the last ABINIT paper [8] and in the review article [79].…”
Section: Developments In Excited State Calculationsmentioning
confidence: 99%
“…New G 0 W 0 implementation A high performance G 0 W 0 implementation [164] has been developed within ABINIT. It is more efficient than the traditional implementation [8,79] thanks to the treatment of the two major bottlenecks: the summations over conduction states and the inversion of the dielectric matrix. The first bottleneck is circumvented by converting the summations into Sternheimer equations.…”
Section: Van Der Waals Interactionsmentioning
confidence: 99%
“…On the real-frequency axis, Σ exhibits a complex structure with many poles, whereas it has a smooth form on the imaginary axis. 84,85 To avoid the complicated behavior for real frequencies, a common approach is to evaluate the self-energy in the imaginary frequency domain, where Σ is given by…”
Section: Analytic Continuation (Ac)mentioning
confidence: 99%
“…However, this leads to errors of several eV as discussed in Section 8.1. Circumventing the convergence problem by linearizing the QP equations 85 is not a good strategy either. For the HOMO levels, the linearized version yields very similar QP energies.…”
Section: Identification Of the Qp Energymentioning
confidence: 99%
“…However, two sources of error in the associated point defect calculations limit the application of charged defect DFT efforts in a high-throughput framework. First, semi-local exchange-correlation approximations (e.g., generalized gradient approximation (GGA)) can severely underestimate the band gap so that usage of post DFT methods becomes pivotal (e.g., GW [22,23,24] and GGA+U methods [25,26], and hybrid functionals [27]). Second, applying periodic boundary conditions with finite sized defect supercells to model point defects makes a defect interact with its own images [9,28], thus, causing departure from the key assumption made in the dilute limit formation energy formalism [9,28].…”
Section: Introductionmentioning
confidence: 99%