The Poole-Frenkel conduction mechanism in Mo-Cu2O-Au thin film structures

被引:18
作者
Rakhshani, AE
Makdisi, Y
Mathew, X
机构
[1] Physics Department, Kuwait University, Safat 13060
关键词
D O I
10.1023/A:1018506516020
中图分类号
TM [电工技术]; TN [电子技术、通信技术];
学科分类号
0808 ; 0809 ;
摘要
Thin films of cuprous oxide (4.6 mu m) were electrodeposited on molybdenum. Gold contacts were vacuum evaporated on the films to form devices. These films showed relatively low electrical resistivities at around 10(6) Ohm cm and a charge transport mechanism which is different from the space charge limited current conduction previously reported for the 10(11) Ohm cm films. The charge transport mechanism in these films was determined by isothermal measurements of the devices current-voltage (I-V) characteristics at some selected temperatures in the range of 78-321 K. In this temperature range the dominant transport mechanism can be explained by the Poole-Frenkel effect through the relation I = VG(0)exp(-phi(0L)/kT) exp (BLV1/2) + I(0)exp(-phi(0H)/kT)exp(BHV1/2) where the numerical values of the parameters are measured. phi(0L) = 0.12 eV is the zero-field ionization energy of a shallow acceptor-type level (measured from the edge of the valence band) which has the dominant effect in the range of 78-230 K. Similarly phi(0H) = 0.70 eV corresponds to a deep level dominant in the high-temperature range 230-321 K. In the high-temperature region a 2.7 mu m thick hole accumulation layer forms beneath the oxide-gold interface, assuming the ionized deep level is doubly charged.
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页码:207 / 211
页数:5
相关论文
共 26 条
[1]   REVISED ROLE FOR THE POOLE-FRENKEL EFFECT IN DEEP-LEVEL CHARACTERIZATION [J].
BUCHWALD, WR ;
JOHNSON, NM .
JOURNAL OF APPLIED PHYSICS, 1988, 64 (02) :958-961
[2]  
CAMPBELL DS, 1978, ACTIVE PASSIVE THIN, P113
[3]   ELECTRODEPOSITION AND CHARACTERIZATION OF CUPROUS-OXIDE FILMS [J].
CHATTERJEE, AP ;
MUKHOPADHYAY, AK ;
CHAKRABORTY, AK ;
SASMAL, RN ;
LAHIRI, SK .
MATERIALS LETTERS, 1991, 11 (10-12) :358-362
[4]  
Frenkel J, 1938, PHYS REV, V54, P647, DOI 10.1103/PhysRev.54.647
[5]  
Frenkel J., 1938, TECHN PHYS USSR, V5, P685
[6]   ELECTROLESS CHEMICAL-DEPOSITION TECHNIQUE FOR CU2O THIN-FILMS [J].
GROZDANOV, I .
MATERIALS LETTERS, 1994, 19 (5-6) :281-285
[7]  
Hill R. M., 1967, Thin Solid Films, V1, P39
[8]  
Jonscher A.K., 1967, Thin Solid Films, V1, P213, DOI DOI 10.1016/0040-6090(67)90004-1
[9]   ON SPACE-CHARGE-LIMITED CONDUCTION IN SEMI-INSULATING GAAS [J].
MARES, JJ ;
KRISTOFIK, J ;
SMID, V ;
DEML, F .
SOLID-STATE ELECTRONICS, 1988, 31 (08) :1309-1313
[10]   ELECTRON TRANSPORT MECHANISMS IN THIN INSULATING FILMS [J].
MEAD, CA .
PHYSICAL REVIEW, 1962, 128 (05) :2088-&