TY - JOUR
T1 - High-temperature solvothermal synthesis and magnetic properties of nearly monodisperse CdCr2S4 nanocrystals
AU - Pang, Chao
AU - Gao, Ling
AU - Chaturvedi, Anurag
AU - Bao, Ningzhong
AU - Yanagisawa, Kazumichi
AU - Shen, Liming
AU - Gupta, Arunava
N1 - Publisher Copyright:
© The Royal Society of Chemistry 2015.
PY - 2015
Y1 - 2015
N2 - Magnetic spinel CdCr2S4 nanocrystals have been synthesized using a high-temperature solvothermal method. The synthesis process involves the reaction of excess 1-dodecanethiol (1-DDT) with CdCl2 and CrCl3·6H2O in 1-octadecene (ODE) solution carried out in a sealed titanium alloy autoclave. Nearly monodisperse spherical CdCr2S4 nanocrystals with an average size of 8.0 ± 1.5 nm are obtained. X-ray diffraction patterns confirm formation of the pure spinel phase without any impurities. Magnetic measurements indicate a Curie temperature (Tc) of ∼76 K for the synthesized CdCr2S4 nanocrystals, which are ferromagnetic at lower temperatures with a saturation magnetization value of 19 emu g-1 at 5 K. The magnetic entropy change ΔSm, evaluated from isothermal magnetic measurements, exhibits a maximum around 82 K, with a value of -ΔSm = 0.86 J kg-1 K-1 at Hmax = 5 T. ΔSm spans a broad temperature range, with a full width at half maximum of ∼88 K in the magnetic field range of 0-5 T, which is attractive for magnetic refrigeration applications in the liquid nitrogen temperature range.
AB - Magnetic spinel CdCr2S4 nanocrystals have been synthesized using a high-temperature solvothermal method. The synthesis process involves the reaction of excess 1-dodecanethiol (1-DDT) with CdCl2 and CrCl3·6H2O in 1-octadecene (ODE) solution carried out in a sealed titanium alloy autoclave. Nearly monodisperse spherical CdCr2S4 nanocrystals with an average size of 8.0 ± 1.5 nm are obtained. X-ray diffraction patterns confirm formation of the pure spinel phase without any impurities. Magnetic measurements indicate a Curie temperature (Tc) of ∼76 K for the synthesized CdCr2S4 nanocrystals, which are ferromagnetic at lower temperatures with a saturation magnetization value of 19 emu g-1 at 5 K. The magnetic entropy change ΔSm, evaluated from isothermal magnetic measurements, exhibits a maximum around 82 K, with a value of -ΔSm = 0.86 J kg-1 K-1 at Hmax = 5 T. ΔSm spans a broad temperature range, with a full width at half maximum of ∼88 K in the magnetic field range of 0-5 T, which is attractive for magnetic refrigeration applications in the liquid nitrogen temperature range.
UR - http://www.scopus.com/inward/record.url?scp=84947795863&partnerID=8YFLogxK
U2 - 10.1039/c5tc02727f
DO - 10.1039/c5tc02727f
M3 - 文章
AN - SCOPUS:84947795863
SN - 2050-7526
VL - 3
SP - 12077
EP - 12082
JO - Journal of Materials Chemistry C
JF - Journal of Materials Chemistry C
IS - 46
ER -