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Surface charging at the (1 0 0) surface of Cu doped and undoped Li2B4O7
Authors:Jie XiaoN Lozova  YaB Losovyj  D WootenI Ketsman  MW SwinneyJ Petrosky  J McCloryYaV Burak  VT AdamivAT Brant  PA Dowben
Institution:a Department of Physics and Astronomy and the Nebraska Center for Materials and Nanoscience, University of Nebraska-Lincoln, Theodore Jorgensen Hall 855 North 16th Street, Lincoln, NE 68588-0299, USA
b J. Bennett Johnston Sr. Center for Advanced Microstructures and Devices, Louisiana State University, 6980 Jefferson Highway, Baton Rouge, LA 70806, USA
c Air Force Institute of Technology, 2950 Hobson Way, Wright Patterson Air Force Base, OH 45433-7765, USA
d Institute of Physical Optics, 23 Dragomanov Str., Lviv 79005, Ukraine
e Department of Engineering Physics, West Virginia University, Morgantown, WV 26506, USA
Abstract:We have compared the photovoltaic charging of the (1 0 0) surface termination for Cu doped and undoped Li2B4O7. While the surface charging at the (1 0 0) surface of Li2B4O7 is significantly greater than observed at (1 1 0) surface, the Cu doping plays a role in reducing the surface photovoltage effects. With Cu doping of Li2B4O7, the surface photovoltaic charging is much diminished at the (1 0 0) surface. The density of states observed with combined photoemission and inverse photoemission remains similar to that observed for the undoped material, except in the vicinity of the conduction band edge.
Keywords:79  60  Ai  68  55  Ln  29  40  Wk  81  05  J
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