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Quasiparticle electronic structure of copper in the GW approximation
Andrea Marini1, Giovanni Onida, Rodolfo Del Sole
1Istituto Nazionale per la Fisica della Materia, Dipartimento di Fisica, Università di Roma Tor Vergata, Via della Ricerca Scientifica, I-00133 Rome, Italy.
Physical Review Letters
|January 22, 2002
Summary
Photoemission experiments on copper are explained by band-structure theory. Self-energy effects correct discrepancies, with core level exchange-correlation crucial for accurate results.
Area of Science:
- Condensed Matter Physics
- Quantum Chemistry
Background:
- Photoemission and inverse photoemission experiments probe electronic structure.
- Discrepancies exist between experimental data and density functional theory (DFT) Kohn-Sham eigenvalues for bulk copper.
- The single-quasiparticle approximation is often assumed in theoretical descriptions.
Purpose of the Study:
- To quantitatively describe photoemission and inverse photoemission experimental results for bulk copper using band-structure theory.
- To investigate the role of self-energy effects in correcting theoretical band structures.
- To identify the importance of specific exchange-correlation contributions.
Main Methods:
- Utilizing band-structure theory for theoretical calculations.
- Applying self-energy corrections to Kohn-Sham eigenvalues.
- Analyzing exchange-correlation contributions, particularly from 3s and 3p core levels.
Main Results:
- Experimental results for bulk copper are quantitatively reproduced by band-structure theory.
- Self-energy effects significantly correct the discrepancies between experimental band structures and DFT Kohn-Sham eigenvalues.
- Exchange-correlation contributions from 3s and 3p core levels are identified as critical for this correction.
Conclusions:
- Band-structure theory, including self-energy effects, provides an accurate description of photoemission experiments on copper.
- The single-quasiparticle approximation is valid for describing these experimental results.
- Core-level exchange-correlation effects are essential for reconciling theoretical predictions with experimental observations in copper.