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Thermal activation of current in an inhomogeneous Schottky diode with a Gaussian distribution of barrier height |
Ru Guo-Ping(茹国平)†, Yu Rong(俞融), Jiang Yu-Long(蒋玉龙), and Ruan Gang(阮刚) |
State Key Laboratory of ASIC and System, Department of Microelectronics, Fudan University, Shanghai 200433, China |
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Abstract This paper investigates the thermal activation behaviour of current in an inhomogeneous Schottky diode with a Gaussian distribution of barrier height by numerical simulation. The analytical Gaussian distribution model predicted that the I–V–T curves may intersect with the possibility of the negative thermal activation of current, but may be contradictory to the thermionic emission mechanism in a Schottky diode. It shows that the cause of the unphysical phenomenon is related to the incorrect calculation of current across very low barriers. It proposes that junction voltage Vj, excluding the voltage drop across series resistance from the external bias, is a crucial parameter for correct calculation of the current across very low barriers. For correctly employing the thermionic emission model, Vj needs to be smaller than the barrier height $\phi$. With proper scheme of series resistance connection where the condition of Vj > $\phi$ is guaranteed, I–V–T curves of an inhomogeneous Schottky diode with a Gaussian distribution of barrier height have been simulated, which demonstrate normal thermal activation. Although the calculated results exclude the intersecting possibility of I–V–T curves with an assumption of temperature-independent series resistance, it shows that the intersecting is possible when the series resistance has a positive temperature coefficient. Finally, the comparison of our numerical and analytical results indicates that the analytical Gaussian distribution model is valid and accurate in analysing I–V–T curves only for small barrier height inhomogeneity.
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Received: 26 November 2009
Revised: 20 March 2010
Accepted manuscript online:
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Fund: Project supported by Shanghai-Applied Materials Research and Development Fund (Grant Nos. 07SA06 and 09700714200), and Fok Ying Tong Education Foundation (Grant No. 114006). |
Cite this article:
Ru Guo-Ping(茹国平), Yu Rong(俞融), Jiang Yu-Long(蒋玉龙), and Ruan Gang(阮刚) Thermal activation of current in an inhomogeneous Schottky diode with a Gaussian distribution of barrier height 2010 Chin. Phys. B 19 097304
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[1] |
Rhoderick E H and Williams R H 1988 Metal-Semiconductor Contacts 2nd ed. (Oxford: Clarendon)
|
[2] |
Ohdomari I and Tu K N 1980 J. Appl. Phys. 51 3735
|
[3] |
Song Y P, Van Meirhaeghe R L, Laflere W H and Cardon F 1986 Solid State Electron. 29 633
|
[4] |
Werner J H and Guttler H H 1991 J. Appl. Phys. 69 1522
|
[5] |
Horvath Zs J 1995 Vacuum 46 963
|
[6] |
Osvald J 1992 Solid State Electron. 35 1629
|
[7] |
Tung R T 1992 Phys. Rev. B 45 13509
|
[8] |
Chin V W L, Green M A and Sotrey J W V 1990 Solid State Electron. 33 299
|
[9] |
Dimitriadis C A, Logothetidis S and Alexandrou I 1995 Appl. Phys. Lett. 66 502
|
[10] |
Lauwers A, Larsen K K, Van Hove M, Verbeeck R, Maex K, Vercaemst A, Van Meirhaeghe R and Cardon F 1995 J. Appl. Phys. 77 2525
|
[11] |
McCafferty P G, Sellai A, Dawson P and Elabd H 1996 Solid State Electron. 39 583
|
[12] |
Chand S and Kumar J 1996 J. Appl. Phys. 80 288
|
[13] |
Paglino C, Fach A, John J, Muller P, Zogg H and Pescia D 1996 J. Appl. Phys. 80 7138
|
[14] |
Zhu S Y, Van Meirhaeghe R L, Detavernier C, Cardon F, Ru G P, Qu X P and Li B Z 2000 Solid State Electron. 44 663
|
[15] |
Hudait M K and Krupanidhi S B 2001 Physica B 307 125
|
[16] |
Palm H, Arbes M and Schulz M 1993 Phys. Rev. Lett. 71 2224
|
[17] |
Chand S 2002 Semicond. Sci. Technol. 17 L36
|
[18] |
Osvald J 2003 Semicond. Sci. Technol. 18 L24
|
[19] |
Chand S 2004 Semicond. Sci. Technol. 19 82
|
[20] |
Osvald J 2006 Solid State Commun. 138 39
|
[21] |
Rouag N, Boussouar L, Toumi S, Ouennoughi Z and Djouadi M A 2007 Semicond. Sci. Technol. 22 369
|
[22] |
Osvald J 2006 J. Appl. Phys. 99 033708
|
[23] |
Dobrocka E and Osvald J 1994 Appl. Phys. Lett. 65 575
|
[24] |
Chand S and Kumar J 1997 Semicond. Sci. Technol. 12 899
|
[25] |
Tugluoglu N, Karadeniz S and Altindal S 2005 Appl. Surf. Sci. 239 481
|
[26] |
Dokme I and Altindal S 2006 Semicond. Sci. Technol. 21 1053
|
[27] |
Yildiz D E, Altindal S and Kanbur H 2008 J. Appl. Phys. 103 124502
|
[28] |
Pakma O, Serin N, Serin T and Altindal S 2008 Semicond. Sci. Technol. 23 105014
|
[29] |
Tekeli Z, Altindal S, Cakmak M, Ozcelik S, Caliskan D and Ozbay E 2007 J. Appl. Phys. 102 054510
|
[30] |
Cheng C J, Zhang X F, Lu Z X, Ding J X, Zhang L, Zhao L, Si J J, Sun W G, Sang L W, Qin Z X and Zhang G Y 2008 Appl. Phys. Lett. 92 103505
|
[31] |
Ravinandan M, Rao P K and Reddy V R 2009 Semicond. Sci. Technol. 24 035004
|
[32] |
Arora N D, Hauser J R and Roulston D J 1982 IEEE Trans. Electron. Dev. 29 292 endfootnotesize
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