Carrier behavior in the vicinity of pit defects in GaN characterized by ultraviolet light-assisted Kelvin probe force microscopy

Surface potentials in the vicinity of V-pits (cone bottom) and U-pits (blunt bottom) on epitaxial GaN surface have been systematically studied using ultraviolet (UV) light-assisted Kelvin probe force microscopy (KPFM). The band structure models are established to understand variation of the surface...

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Veröffentlicht in:Science China. Physics, mechanics & astronomy mechanics & astronomy, 2019-06, Vol.62 (6), p.67311, Article 67311
Hauptverfasser: Kai, CuiHong, Sun, XiaoJuan, Jia, YuPing, Shi, ZhiMing, Jiang, Ke, Ben, JianWei, Wu, You, Wang, Yong, Liu, HeNan, Li, XiaoHang, Li, DaBing
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container_issue 6
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container_title Science China. Physics, mechanics & astronomy
container_volume 62
creator Kai, CuiHong
Sun, XiaoJuan
Jia, YuPing
Shi, ZhiMing
Jiang, Ke
Ben, JianWei
Wu, You
Wang, Yong
Liu, HeNan
Li, XiaoHang
Li, DaBing
description Surface potentials in the vicinity of V-pits (cone bottom) and U-pits (blunt bottom) on epitaxial GaN surface have been systematically studied using ultraviolet (UV) light-assisted Kelvin probe force microscopy (KPFM). The band structure models are established to understand variation of the surface potentials at the pits and planar surface with and without UV light. The photo-generated carrier behavior at the pit defects is studied. According to the surface potential results, it can be deduced that the carrier distributions around the V- and U-pits are uneven. In dark, the electron concentration at the bottom of V-pit (30 n 0 ) and Upit (15 n 0 ) are higher than that at planar surface ( n 0 ). Under UV light, for V-pit, the electron concentration at the cone bottom (4.93×10 11 n 0 ) is lower than that at the surrounding planar surface (5.68×10 13 n 0 ). For U-pit, the electron concentration at the blunt bottom is 1.35×10 12 n 0 , which is lower than that at the surrounding planar surface (6.13×10 13 n 0 ). The non-equilibrium electron concentrations at different locations are calculated. Based on the non-equilibrium electron concentration, it can be concluded that the carrier recombination rate at pit defects is higher than that at planar surface.
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The band structure models are established to understand variation of the surface potentials at the pits and planar surface with and without UV light. The photo-generated carrier behavior at the pit defects is studied. According to the surface potential results, it can be deduced that the carrier distributions around the V- and U-pits are uneven. In dark, the electron concentration at the bottom of V-pit (30 n 0 ) and Upit (15 n 0 ) are higher than that at planar surface ( n 0 ). Under UV light, for V-pit, the electron concentration at the cone bottom (4.93×10 11 n 0 ) is lower than that at the surrounding planar surface (5.68×10 13 n 0 ). For U-pit, the electron concentration at the blunt bottom is 1.35×10 12 n 0 , which is lower than that at the surrounding planar surface (6.13×10 13 n 0 ). The non-equilibrium electron concentrations at different locations are calculated. 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Physics, mechanics &amp; astronomy</title><addtitle>Sci. China Phys. Mech. Astron</addtitle><description>Surface potentials in the vicinity of V-pits (cone bottom) and U-pits (blunt bottom) on epitaxial GaN surface have been systematically studied using ultraviolet (UV) light-assisted Kelvin probe force microscopy (KPFM). The band structure models are established to understand variation of the surface potentials at the pits and planar surface with and without UV light. The photo-generated carrier behavior at the pit defects is studied. According to the surface potential results, it can be deduced that the carrier distributions around the V- and U-pits are uneven. In dark, the electron concentration at the bottom of V-pit (30 n 0 ) and Upit (15 n 0 ) are higher than that at planar surface ( n 0 ). Under UV light, for V-pit, the electron concentration at the cone bottom (4.93×10 11 n 0 ) is lower than that at the surrounding planar surface (5.68×10 13 n 0 ). For U-pit, the electron concentration at the blunt bottom is 1.35×10 12 n 0 , which is lower than that at the surrounding planar surface (6.13×10 13 n 0 ). The non-equilibrium electron concentrations at different locations are calculated. 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Physics, mechanics &amp; astronomy</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Kai, CuiHong</au><au>Sun, XiaoJuan</au><au>Jia, YuPing</au><au>Shi, ZhiMing</au><au>Jiang, Ke</au><au>Ben, JianWei</au><au>Wu, You</au><au>Wang, Yong</au><au>Liu, HeNan</au><au>Li, XiaoHang</au><au>Li, DaBing</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Carrier behavior in the vicinity of pit defects in GaN characterized by ultraviolet light-assisted Kelvin probe force microscopy</atitle><jtitle>Science China. Physics, mechanics &amp; astronomy</jtitle><stitle>Sci. China Phys. Mech. Astron</stitle><date>2019-06-01</date><risdate>2019</risdate><volume>62</volume><issue>6</issue><spage>67311</spage><pages>67311-</pages><artnum>67311</artnum><issn>1674-7348</issn><eissn>1869-1927</eissn><abstract>Surface potentials in the vicinity of V-pits (cone bottom) and U-pits (blunt bottom) on epitaxial GaN surface have been systematically studied using ultraviolet (UV) light-assisted Kelvin probe force microscopy (KPFM). The band structure models are established to understand variation of the surface potentials at the pits and planar surface with and without UV light. The photo-generated carrier behavior at the pit defects is studied. According to the surface potential results, it can be deduced that the carrier distributions around the V- and U-pits are uneven. In dark, the electron concentration at the bottom of V-pit (30 n 0 ) and Upit (15 n 0 ) are higher than that at planar surface ( n 0 ). Under UV light, for V-pit, the electron concentration at the cone bottom (4.93×10 11 n 0 ) is lower than that at the surrounding planar surface (5.68×10 13 n 0 ). For U-pit, the electron concentration at the blunt bottom is 1.35×10 12 n 0 , which is lower than that at the surrounding planar surface (6.13×10 13 n 0 ). The non-equilibrium electron concentrations at different locations are calculated. Based on the non-equilibrium electron concentration, it can be concluded that the carrier recombination rate at pit defects is higher than that at planar surface.</abstract><cop>Beijing</cop><pub>Science China Press</pub><doi>10.1007/s11433-018-9320-x</doi></addata></record>
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subjects Astronomy
Carrier recombination
Classical and Continuum Physics
Defects
Microscopy
Observations and Techniques
Physics
Physics and Astronomy
Pits
Ultraviolet radiation
title Carrier behavior in the vicinity of pit defects in GaN characterized by ultraviolet light-assisted Kelvin probe force microscopy
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