We investigated GaAs (1 1 3) surfaces prepared by molecular beam epitaxy (MBE) and metal-organic vapour phase epitaxy (MOVPE) with reflectance anisotropy spectroscopy (RAS) and low energy electron diffraction (LEED) and found two different static (non-growth) reconstructions: For many conditions the well known (8×1) reconstruction is observed, while under more arsenic rich conditions a reconstruction a p(1×1) symmetry shows up. The activation energy for the transition from the p(1×1) to the (8×1) reconstruction was determined to (1.50±0.02) eV. A structure model for the arsenic rich p(1×1) reconstruction is presented in accordance with the above findings
There currently exists a wide range of powerful techniques for probing surfaces, mainly involving th...
There currently exists a wide range of powerful techniques for probing surfaces, mainly involving th...
The optical anisotropy of differently reconstructed GaAs(001) surfaces has been analysed both theore...
GaAs(114)A surfaces were prepared using molecular beam epitaxy followed by annealing in As-2 pressur...
GaAs(114)A surfaces were prepared using molecular beam epitaxy followed by annealing in As-2 pressur...
GaAs(114)A surfaces were prepared using molecular beam epitaxy followed by annealing in As-2 pressur...
The method of reflectance anisotropy spectroscopy (RAS) has proved extremely useful in monitoring th...
The method of reflectance anisotropy spectroscopy (RAS) has proved extremely useful in monitoring th...
The method of reflectance anisotropy spectroscopy (RAS) has proved extremely useful in monitoring th...
The GaAs (113)A surface was prepared by molecular beam epitaxy and investigated in situ by means of ...
We have performed ab initio pseudopotential calculations of three alternative structures of the GaAs...
We have performed ab initio pseudopotential calculations of three alternative structures of the GaAs...
We have performed ab initio pseudopotential calculations of three alternative structures of the GaAs...
There currently exists a wide range of powerful techniques for probing surfaces, mainly involving th...
There currently exists a wide range of powerful techniques for probing surfaces, mainly involving th...
There currently exists a wide range of powerful techniques for probing surfaces, mainly involving th...
There currently exists a wide range of powerful techniques for probing surfaces, mainly involving th...
The optical anisotropy of differently reconstructed GaAs(001) surfaces has been analysed both theore...
GaAs(114)A surfaces were prepared using molecular beam epitaxy followed by annealing in As-2 pressur...
GaAs(114)A surfaces were prepared using molecular beam epitaxy followed by annealing in As-2 pressur...
GaAs(114)A surfaces were prepared using molecular beam epitaxy followed by annealing in As-2 pressur...
The method of reflectance anisotropy spectroscopy (RAS) has proved extremely useful in monitoring th...
The method of reflectance anisotropy spectroscopy (RAS) has proved extremely useful in monitoring th...
The method of reflectance anisotropy spectroscopy (RAS) has proved extremely useful in monitoring th...
The GaAs (113)A surface was prepared by molecular beam epitaxy and investigated in situ by means of ...
We have performed ab initio pseudopotential calculations of three alternative structures of the GaAs...
We have performed ab initio pseudopotential calculations of three alternative structures of the GaAs...
We have performed ab initio pseudopotential calculations of three alternative structures of the GaAs...
There currently exists a wide range of powerful techniques for probing surfaces, mainly involving th...
There currently exists a wide range of powerful techniques for probing surfaces, mainly involving th...
There currently exists a wide range of powerful techniques for probing surfaces, mainly involving th...
There currently exists a wide range of powerful techniques for probing surfaces, mainly involving th...
The optical anisotropy of differently reconstructed GaAs(001) surfaces has been analysed both theore...