TY - JOUR
T1 - Rich chemistry of copper in crystalline silicon
AU - Estreicher, S. K.
PY - 1999
Y1 - 1999
N2 - The interstitial copper ion (Cu+i) is a very fast-diffusing impurity in Si. While the isolated interstitial is a shallow donor, it reacts with impurities and defects and these reactions affect the electrical properties of the material. Copper passivates shallow acceptors, forms pairs with various impurities, including itself, and precipitates at defects. Some Cu precipitates are strong electron-hole recombination centers. In this paper, interstitial and substitutional copper, copper-acceptor pairs, and the precipitation of copper at a model nanodefect, the ring hexavacancy, are studied in clusters at the ab initio Hartree-Fock level. The chemistry of copper in Si is not as simple as commonly believed, even in the case of Cu+i. The interstitial ion is not in the 3d104sp0 configuration as often assumed, but transfers some electrons into the 4sp shell, which ultimately is responsible for the various covalent interactions between copper and its host crystal. In addition to energy-optimized configurations and binding energies, a number of details of the chemical interactions shed light on the behavior of copper in silicon.
AB - The interstitial copper ion (Cu+i) is a very fast-diffusing impurity in Si. While the isolated interstitial is a shallow donor, it reacts with impurities and defects and these reactions affect the electrical properties of the material. Copper passivates shallow acceptors, forms pairs with various impurities, including itself, and precipitates at defects. Some Cu precipitates are strong electron-hole recombination centers. In this paper, interstitial and substitutional copper, copper-acceptor pairs, and the precipitation of copper at a model nanodefect, the ring hexavacancy, are studied in clusters at the ab initio Hartree-Fock level. The chemistry of copper in Si is not as simple as commonly believed, even in the case of Cu+i. The interstitial ion is not in the 3d104sp0 configuration as often assumed, but transfers some electrons into the 4sp shell, which ultimately is responsible for the various covalent interactions between copper and its host crystal. In addition to energy-optimized configurations and binding energies, a number of details of the chemical interactions shed light on the behavior of copper in silicon.
UR - http://www.scopus.com/inward/record.url?scp=0000182949&partnerID=8YFLogxK
U2 - 10.1103/PhysRevB.60.5375
DO - 10.1103/PhysRevB.60.5375
M3 - Article
AN - SCOPUS:0000182949
SN - 1098-0121
VL - 60
SP - 5375
EP - 5382
JO - Physical Review B - Condensed Matter and Materials Physics
JF - Physical Review B - Condensed Matter and Materials Physics
IS - 8
ER -