Atomic structure, electronic structure, and band offsets at Ge:GeO:GeO2 interfaces

2010 ◽  
Vol 97 (24) ◽  
pp. 242902 ◽  
Author(s):  
L. Lin ◽  
K. Xiong ◽  
J. Robertson
2002 ◽  
Vol 747 ◽  
Author(s):  
J Robertson ◽  
P W Peacock

AbstractThe bonding, electronic structure and valence band offsets are calculated for various atomic models of interfaces between Si and high dielectric constant insulators ZrO2 and SrTiO3. A non-polar face of the oxide does not necessarily give a semiconducting interface, because of the need to fill Si dangling bond states on the Si side. This can be achieved by stoichiometry changes. Band offsets of semiconducting interfaces are generally the same as those found from bulk charge neutrality levels, indicating no dipole layers. Dipole layers are present at some configurations, where the offset is then changed by up to 1 eV. The states of hydrogen in the oxides are also considered.


2002 ◽  
Vol 745 ◽  
Author(s):  
J Robertson ◽  
P W Peacock

ABSTRACTThe bonding, electronic structure and valence band offsets are calculated for various atomic models of interfaces between Si and high dielectric constant insulators ZrO2 and SrTiO3. A non-polar face of the oxide does not necessarily give a semiconducting interface, because of the need to fill Si dangling bond states on the Si side. This can be achieved by stoichiometry changes. Band offsets of semiconducting interfaces are generally the same as those found from bulk charge neutrality levels, indicating no dipole layers. Dipole layers are present at some configurations, where the offset is then changed by up to 1 eV. The states of hydrogen in the oxides are also considered.


1996 ◽  
Vol 79 (6) ◽  
pp. 3108-3114 ◽  
Author(s):  
V. V. Afanas’ev ◽  
M. Bassler ◽  
G. Pensl ◽  
M. J. Schulz ◽  
E. Stein von Kamienski

1977 ◽  
Vol 55 (11) ◽  
pp. 1961-1967 ◽  
Author(s):  
J. E. Enderby

Two broad types of liquid semiconducting alloys will be discussed, namely those involving alkali metals (e.g., the Li–Pb and the Cs–Au system) and those in which a chalcogen is involved (e.g., Cu–Te or Ni–Te). It will be argued that relatively simple ionic bonding schemes in alkali metal systems must be replaced by more complicated ones in chalcogen based alloys. The close interaction between atomic structure on one hand, and the electronic structure on the other will be emphasized.


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