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GaN photocathode is fully activated by employing a continuous Cs source and an alternate O source. The quantum efficiency curve of transmission-mode photocathode is tested in situ. The quantum efficiency reaches up to 13% in transmission-mode. According to the one-dimensional Schrdinger equation, the electron transmission coefficient formula of GaN vacuum electron source material is deduced. For a certain profile of photocathode surface potential barrier, the electron transmission coefficient relates to the incident electron energy, the height and the width of the surface potential. The energy band of transmission-mode negative electron affinity (NEA) GaN photocathode and the change of surface barrier in the deposit course of Cs,O are given. Using the double dipole layer surface model [CaN(Mg):Cs]:O-Cs, the NEA property formation of GaN vacuum electron source material is analyzed. The results show that the double dipole layer formed in the activation course of Cs,O is conducible to the escape of electrons, and it is the formation of double dipole layer that causes the drop of vacuum energy level of the material surface.
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Keywords:
- GaN /
- electron source /
- transmission coefficient /
- double dipole layer
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[1] Pierce D T, Meier F 1976 Phys. Rev. B 13 5484
[2] Maruyama T, Brachmann A, Clendenin J E, Desikan T, Garwin E L, Kirby R E, Luh D A, Turner J, Prepost R 2002 Nucl. Instrum. Meth. Phys. Res. A 492 199
[3] [4] [5] Machuca F, Liu Z, Sun Y, Pianetta P, Spicer W E, Pease R F W 2002 J. Vac. Sci. Technol. B 20 2721
[6] Herrera-Gmez A, Vergara G, Spicer W E 1996 J. Appl. Phys. 79 7318
[7] [8] [9] Machuca F 2003 Ph. D. Dissertation (Stanford: Stanford University)
[10] Li Q, Hao L, Pang W N 2008 Acta Phys. Sin. 57 172 (in Chinese)[李 倩、郝 亮、庞文宁 2008 物理学报 57 172 ]
[11] [12] Ruan C J 2003 Ph. D. Dissertation (Beijing: Tsinghua University) (in Chinese)[阮存军 2003 博士学位论文(北京:清华大学)]
[13] [14] Spicer W E, Herrera-Gmez A 1993 Proc. SPIE 2022 18
[15] [16] Siegmund O, Vallerga J, McPhate J, Malloy J, Tremsin A, Martin A, Ulmer M, Wessels B 2006 Nucl. Instrum. Meth. Phys. Res. A 567 89
[17] [18] [19] Qiao J L, Tian S, Chang B K, Du X Q, Gao P 2009 Acta Phys. Sin. 58 5847 (in Chinese)[乔建良、田 思、常本康、杜晓晴、高 频 2009 物理学报 58 5847]
[20] [21] Wang X H, Chang B K, Qian Y S, Gao P, Zhang Y J, Qiao J L, Du X Q 2011 Acta Phys. Sin. 60 057902 (in Chinese)[王 晓晖、常本康、钱芸生、高 频、张益军、乔建良、杜晓晴 2011 物理学报 60 057902]
[22] [23] Qiao J L, Chang B K, Yang Z, Gao Y T, Tian S 2008 Opt. Techn. 34 395 (in Chinese)[乔建良、常本康、杨 智、高有堂、田 思 2008 光学技术 34 395]
[24] Wang H M, Zhang Y F 2005 Acta Phys. Sin. 54 2226 (in Chinese) [王洪梅、张亚非 2005 物理学报 54 2226]
[25] [26] Lui W W, Fukuma M 1986 J. Appl. Phys. 60 1555
[27] [28] [29] Hsu D S, Hsu M Z, Tan C H, Wang Y Y 1992 J. Appl. Phys. 72 4972
[30] Allen S S, Richardson S L 1996 J. Appl. Phys. 79 886
[31] [32] [33] Zou J J 2007 Ph. D. Dissertation (Nanjing: Nanjing University of Science and Technology) (in Chinese)[邹继军2007 博士学位论文 (南京:南京理工大学)]
[34] [35] Qiao J L, Chang B K, Du X Q, Niu J, Zou J J 2010 Acta Phys. Sin. 59 2855 (in Chinese)[乔建良、常本康、杜晓晴、牛 军、邹继军 2010 物理学报 59 2855]
[36] [37] Qiao J L, Niu J, Yang Z, Zou J J, Chang B K 2009 Opt. Techn. 35 145 (in Chinese)[乔建良、牛 军、杨 智、邹继军、常本康 2009 光学技术 35 145]
[38] [39] Qiao J L, Chang B K, Qian Y S, Du X Q, Wang X H, Guo X Y 2011 Acta Phys. Sin. 60 017903 (in Chinese)[乔建良、常本康、钱芸生、杜晓晴、王晓晖、郭向阳 2011 物理学报 60 017903]
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