Ryusuke KondoTatsuo HashimotoKeiichi EdagawaShin TakeuchiTsunehiro TakeuchiUichiro Mizutani
The electrical resistivity and the magnetoresistance have been measured for icosahedral phases of Zn–Mg–RE (RE=Y, Gd). Electrical resistivities of bulk samples of Zn 56 Mg 36 Y 8 , annealed ribbon samples of Zn 62 Mg 30 Y 8 and annealed ribbon samples of Zn 55 Mg 35.5 Gd 9.5 are 1 mΩcm, 0.3 mΩcm and 0.3 mΩcm, respectively. The resistivities of all the samples decrease by 5∼7% from 4.2 K to 273 K. At low temperatures, the conductivity of Zn–Mg–Y obeys T 1/2 dependence, while the resistivity of Zn–Mg–Gd obeys ln T dependence, where Gd atoms bear magnetic moments. In Zn–Mg–Y, the magnetoresistance is negative and insensitive to temperature, while in Zn–Mg–Gd it is positive in a low field range and becomes negative at high field with its magnitude larger at lower temperature. These results are interpreted by the theories of electron-electron interaction, weak localization and s-d exchange interaction.
Yoshinori HattoriK. FukamichiKenji SuzukiAkio NiikuraA.‐P. TsaiA. InoueT. Masumoto
T. SatoHiroyuki TakakuraA. P. TsaiKenji OhoyamaKaoru ShibataK.H. Andersen
Robert GallerR. SterzelW. AßmusH. Mehrer
A.‐P. TsaiAkio NiikuraAkihisa InoueT. MasumotoYasushi NishidaKenji TsudaMichiyoshi Tanaka
Arun Kumar SR. RajeshJithu JayarajK. G. RaghuA. Srinivasan