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磁场对空穴掺杂铁磁锰氧化物LaNaMnO中电输运和热输运的影响

Influence of magnetic field on electrical and thermal transport in the hole doped ferromagnetic manganite: LaNaMnO.

作者信息

Das Rajasree, Chanda Amit, Mahendiran Ramanathan

机构信息

Department of Physics, Faculty of Science, National University of Singapore 2 Science Drive 3 Singapore - 117542 Republic of Singapore

出版信息

RSC Adv. 2019 Jan 14;9(3):1726-1733. doi: 10.1039/c8ra08694j. eCollection 2019 Jan 9.

DOI:10.1039/c8ra08694j
PMID:35518048
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC9059764/
Abstract

We report the magnetization (), magnetostriction, electrical resistivity (), thermal conductivity () and thermopower () of polycrystalline LaNaMnO over a wide temperature range of 5 to 360 K. This sample undergoes a paramagnetic to ferromagnetic transition around = 274 K and electrical resistivity shows an insulator-metal transition around = 292 K. The sign of thermopower is positive in the entire temperature range which indicates that majority charge carriers are holes. Thermopower exhibits a peak and thermal conductivity shows a dip at in the absence of magnetic field. Large difference between the experimentally determined activation energies of and in the insulating state indicates small polaron hopping dominant conduction above . Polaron formation above , was further confirmed from the anomaly observed in thermal expansion (Δ/ ) which shows a change in slope at . In the vicinity of at 3 T applied field, magneto-thermopower (∼61.5%) is larger than magnetothermal conductivity (∼12.7%) and magnetoresistance (∼49%).

摘要

我们报告了多晶LaNaMnO在5至360 K的宽温度范围内的磁化强度()、磁致伸缩、电阻率()、热导率()和热电势()。该样品在 = 274 K左右经历顺磁到铁磁转变,电阻率 在 = 292 K左右显示绝缘体 - 金属转变。热电势 的符号在整个温度范围内为正,这表明多数载流子是空穴。在无磁场时,热电势在 处出现峰值,热导率在 处出现下降。在绝缘状态下,实验测定的 和 的激活能之间的巨大差异表明,高于 时小极化子跳跃主导传导。高于 时极化子的形成,从热膨胀(Δ/ )中观察到的异常进一步得到证实,该异常在 处显示斜率变化。在3 T外加磁场下接近 时,磁热电势(约61.5%)大于磁热导率(约12.7%)和磁电阻(约49%)。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3ab5/9059764/083770db00ee/c8ra08694j-f5.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3ab5/9059764/46c56cdbfa89/c8ra08694j-f1.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3ab5/9059764/acb04d6b5580/c8ra08694j-f2.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3ab5/9059764/2ca61e0a2f2b/c8ra08694j-f3.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3ab5/9059764/b79366f1746f/c8ra08694j-f4.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3ab5/9059764/083770db00ee/c8ra08694j-f5.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3ab5/9059764/46c56cdbfa89/c8ra08694j-f1.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3ab5/9059764/acb04d6b5580/c8ra08694j-f2.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3ab5/9059764/2ca61e0a2f2b/c8ra08694j-f3.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3ab5/9059764/b79366f1746f/c8ra08694j-f4.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/3ab5/9059764/083770db00ee/c8ra08694j-f5.jpg

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