Negative differential resistance and quantum oscillations in FeSb<sub>2</sub> with embedded antimony<xref rid="cpb_28_3_037104fn1" ref-type="fn">*</xref><fn id="cpb_28_3_037104fn1"><label>*</label><p>Project supported by Guangdong Innovative and Entrepreneurial Research Team Program, China (Grant No. 2016ZT06D348), the National Natural Science Foundation of China (Grant No. 11874193), and the Shenzhen Fundamental Subject Research Program, China (Grant Nos. JCYJ20170817110751776 and JCYJ20170307105434022). The work at Brookhaven is supported by the US Department of Energy, Office of Basic Energy Sciences as part of the Computational Material Science Program (material synthesis).</p></fn>

Negative differential resistance and quantum oscillations in FeSb₂ with embedded antimony**

Project supported by Guangdong Innovative and Entrepreneurial Research Team Program, China (Grant No. 2016ZT06D348), the National Natural Science Foundation of China (Grant No. 11874193), and the Shenzhen Fundamental Subject Research Program, China (Grant Nos. JCYJ20170817110751776 and JCYJ20170307105434022). The work at Brookhaven is supported by the US Department of Energy, Office of Basic Energy Sciences as part of the Computational Material Science Program (material synthesis).

Tang Fangdong^{1, 2}, Du Qianheng^{3, 4}, Petrovic Cedomir^{3, 4}, Zhang Wei¹, He Mingquan⁵, Zhang Liyuan^{2, †}

(a) Temperature dependence of the resistance R(T) for sample 5 using the temperature readings recorded by a thermometer attached onto sample surface. Inset: a photograph of the experimental setup. (b) The temperatures recorded on the thermometer as a function of bias current T(I) at various base temperatures. (c) Comparison between the recreated I–V curves (lines) using R(T), T(I) shown in panels (a) and (b) and the I–V results obtained from direct measurements (points). See the main text for details.