2012
DOI: 10.1016/j.scriptamat.2012.03.002
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High figure of merit in (Ti,Zr,Hf)NiSn half-Heusler alloys

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Cited by 140 publications
(101 citation statements)
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“…23 In general, j values are in a range typical for HH compounds with isoelectronic substitution on the X site. 6,8 Tasubstituted compounds show j values comparable to nanostructured Sb-substituted (Zr,Hf)NiSn. 10 Even lower thermal conductivity should be expected when the grain size and shape are refined.…”
Section: à3mentioning
confidence: 99%
See 1 more Smart Citation
“…23 In general, j values are in a range typical for HH compounds with isoelectronic substitution on the X site. 6,8 Tasubstituted compounds show j values comparable to nanostructured Sb-substituted (Zr,Hf)NiSn. 10 Even lower thermal conductivity should be expected when the grain size and shape are refined.…”
Section: à3mentioning
confidence: 99%
“…Each atom site can be substituted for tuning the electron and phonon transport properties. 5 In the scope of the PGEC concept, the most successful strategies for improving the thermoelectric properties of XNiSn HH compounds have been: (1) isoelectric substitution on the X site with Ti and/or Zr and/or Hf to induce point defect scattering in order to suppress j latt ; [6][7][8] (2) Sb doping on the Sn site to adjust the carrier concentration for a high PF; 6,9,10 and (3) nanostructuring to limit the phonon mean free path and further suppress j latt . 11,12 Physical properties of the samples of the same nominal composition show considerable differences, as listed in Table I, raising questions about the influence of different synthesis methods on sample morphology and phase purity.…”
mentioning
confidence: 99%
“…14, 23 The lattice parameter a of the Zr-Hf-rich phase (HH1) and the Ti-rich phase (HH2) was estimated by a rene-ment of the peak position using LaB 6 as an internal standard and found to be 6.068Å, and 6.001Å, respectively. With increasing Nb content, a decrease in the lattice parameter could be observed.…”
Section: Crystal Structurementioning
confidence: 99%
“…Splitting of the Bragg reflection peaks is caused by the coexistence of two 4 HH phases. During the solidification process, the multi-component HH system dissipates into a Ti-poor (HH 1) and a Ti-rich (HH 2) phases [15] . The backscattering electron mode (BSE) SEM images of the n-and p-type samples before and after 500 cycles, shown in Figure 2, revealed the intrinsic phase separation into the main Ti-poor HH 1 phase and the Ti-rich HH 2 phases, which is dendritically interlaced through the microstructure.…”
Section: Resultsmentioning
confidence: 99%