Kondo effect and impurity interactions in the resistivity of diluteZnMn alloys
Kondo effect and impurity interactions in the resistivity of diluteZnMn alloys
复制标题
稀锌锰合金电阻率中的近藤效应和杂质相互作用
DOI:
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发表时间:
1977
期刊:
影响因子:
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通讯作者:
E. Wassermann
中科院分区:
文献类型:
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作者:
J. Kästner;E. Wassermann
The electrical resistivity of diluteZnMn alloys (c=1.7–2400 ppm Mn) has been investigated in the temperature range from 0.05 to 14 K. For the most dilute sample, single-impurity Kondo behavior is found, well described by the Hamann formula withTK=0.9 K,S=3/2. ForT<50 mK, aT2 law with θR=0.3 K is expected. In the dilute limit the Kondo slope is −(1/c)d(Δρ)/d(logT)=3.7±0.2 µΩ-cm/at % dec. In the more highly concentrated alloys, the slope decreases with increasing c and the lnT-like variation of the Kondo resistivity roughly terminates near a temperatureTW(c),TW being related to the average Ruderman-Kittel-Kasuya-Yosida (RKKY) interaction strength between the Mn impurities. For 20 ppm ≤c ≤ 1000 ppm, the resistivity slightly decreases at low temperatures and a broad resistivity maximum is observed atTm(c), withTm ∝c0.7. ForT 2<Tm, the resistivity dependence is linear inT, and for the most concentrated alloy aT3/2 orT2 dependence is measured at the lowest temperatures attainable. The investigation of the transition temperatureTc(c) to superconductivity ofZnMn results in a critical concentrationccr=18 ppm Mn. The concentration dependence ofTc below 0.3 K suggests the presence of the Kondo effect, although impurity interactions may also influenceTc in this temperature range.