2007
DOI: 10.1016/j.intermet.2007.05.009
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Nuclear spin-lattice relaxation in narrow gap semiconductors TiPtSn and ZrPtSn

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Cited by 9 publications
(11 citation statements)
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“…We stress that the observed low-temperature 1/ T 1 T clearly rules out the possibility that for this loading range the system can be discussed as a narrow-gap semiconductor. In this case, 1/ T 1 T would be dominated by the exp(−Δ/ k B T ) term for , which decays exponentially with decreasing temperature 24 , in disagreement with the experimental data.…”
Section: Resultsmentioning
confidence: 52%
“…We stress that the observed low-temperature 1/ T 1 T clearly rules out the possibility that for this loading range the system can be discussed as a narrow-gap semiconductor. In this case, 1/ T 1 T would be dominated by the exp(−Δ/ k B T ) term for , which decays exponentially with decreasing temperature 24 , in disagreement with the experimental data.…”
Section: Resultsmentioning
confidence: 52%
“…24 On the other hand, in a standard topologically trivial half-Heusler semiconductor such as TiPtSn, the 195 Pt Knight shifts were found to weakly shift to lower frequencies with increasing temperature (∂K/∂T < 0). 38 From ∂K/∂T > 0 one may conclude that the thermally excited charge carriers in LuPtBi predominantly have s character, with a positive s-hyperfine constant. Evidently, a classical temperature dependence of the NMR shift, K(T) ∝ n H /k B T, does not apply for LuPtBi.…”
Section: Resultsmentioning
confidence: 99%
“…In Figure 1 inset we plot ( ) versus . A straight line is indicative of a metallic sample, where the quantity ( ) is proportional to the carrier density [17][18][19][20][21][22]. The inset graph shows that the nanocrystals have higher carrier density than the m&p samples across all temperatures investigated.…”
Section: Introductionmentioning
confidence: 99%
“…The Korringa values, T 1• T, were 24 s•K for the m&p sample (below 200 K) and 11 s•K for the nanocrystals (across all temperatures, 140-420 K). These values are not unusual for semiconductors and tend to reflect the fact that T 1 •T is inversely proportional to the square of the electronic density of states (DOS) at the Fermi level, ( ) [16][17][18][19][20][21]. A lower Korringa value means higher carrier density and a more metallic state.…”
Section: Introductionmentioning
confidence: 99%