Thermoelectric properties of p-type lead telluride doped with silver or potassium

被引:22
作者
Noda, Y
Orihashi, M
Nishida, IA
机构
[1] Tohoku Univ, Grad Sch Engn, Dept Mat Sci, Sendai, Miyagi 9808579, Japan
[2] Natl Res Inst Met, Tsukuba, Ibaraki 3050047, Japan
来源
MATERIALS TRANSACTIONS JIM | 1998年 / 39卷 / 05期
关键词
lead telluride; p-type dopant; scattering mechanism; thermoelectricity; figure of merit; diffusion;
D O I
10.2320/matertrans1989.39.602
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
Single crystals of p-type PbTe were prepared by the Bridgman method, where either Ag2Te or K was doped as the source material of silver or potassium, respectively. Carrier concentration and Hall mobility were measured from 77 to 300 K. The hole concentration was successfully controlled in the range from 2.0 x 10(24) to 9.0 x 10(24) m(-3) by doping 100 to 700 mol ppm Ag2Te, while the conduction type changed from p- to n-type in the region more than 1000 mol ppm Ag2Te. In the case of K-doping, the carrier concentration was controlled in the region of 8.0 x 10(24) to 4.0 x 10(25) m(-3) with 1000 to 25000 mol ppm it. Figure of merits (Z) of p-PbTe at 300 K were 8.0 x 10(-4) K-1 at a hole concentration of 1.34 x 10(25) m(-3) (2400 mol ppm K) and 1.38 x 10(-3) K-1 at 2.34 x 10(24) m(-3) (200 mol ppm Ag2Te). Diffusion lengths of dopant elements of Ag, K and Sn for p-type and I for n-type PbTe were estimated using the literature data. The result indicates that long distance diffusion occurs in a short period in the case of Ag and K. Therefore, the stable functionally graded materials (FGM) of PbTe might be prepared by gradient I doping or Sn alloying, while those by Ag or K doping will be soon changed into non-FGM due to the rapid diffusion resulting in the decreased efficiency of thermoelectric energy conversion.
引用
收藏
页码:602 / 605
页数:4
相关论文
共 13 条
[1]   MOBILITY OF ELECTRONS AND HOLES IN PBS, PBSE, AND PBTE BETWEEN ROOM TEMPERATURE AND 4.2-DEGREES-K [J].
ALLGAIER, RS ;
SCANLON, WW .
PHYSICAL REVIEW, 1958, 111 (04) :1029-1037
[2]  
ANDREEV AA, 1967, SOV PHYS SEMICOND+, V1, P145
[3]  
BATTAGLIOLI M, 1982, P 4 INT C THERM EN C, P114
[4]   A REVIEW OF SEMICONDUCTOR PROPERTIES OF PBTE, PBSE, PBS AND PBO [J].
DALVEN, R .
INFRARED PHYSICS, 1969, 9 (04) :141-+
[5]  
IMAI Y, 1996, P 4 INT S FUNCT GRAD, P617
[6]  
NIINO M, 1993, P 12 INT C THERM, P527
[7]  
Noda Y., 1996, Transactions of the Institute of Electrical Engineers of Japan, Part A, V116-A, P242
[8]  
NODA Y, 1996, P S THERM CONV 96 TE, P20
[9]  
NODA Y, 1995, P S THERM CONV 95 TE, P40
[10]  
ORIHASHI M, 1996, P 4 INT S FUNCT GRAD, P569