Interplay between structure and magnetism and effect of size of HoMn2O5 nanorods

碩士 === 中原大學 === 物理研究所 === 101 === Abstract Various size of HoMn2O5 nanorods were fabricated by combining hydrothermal and annealing method with 240、300、500、700、900、1100 °C annealing temperatures. X-ray diffraction experiments reveal that all the samples are crystallized in orthorhombic with space gr...

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Main Authors: SHENG-SIANG YOU, 游聲翔
Other Authors: Chun-Chuen Yang
Format: Others
Language:zh-TW
Published: 2013
Online Access:http://ndltd.ncl.edu.tw/handle/26089448905035924255
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spelling ndltd-TW-101CYCU51980112015-10-13T22:40:29Z http://ndltd.ncl.edu.tw/handle/26089448905035924255 Interplay between structure and magnetism and effect of size of HoMn2O5 nanorods HoMn2O5奈米尺寸效應與結構、磁性交互作用研究 SHENG-SIANG YOU 游聲翔 碩士 中原大學 物理研究所 101 Abstract Various size of HoMn2O5 nanorods were fabricated by combining hydrothermal and annealing method with 240、300、500、700、900、1100 °C annealing temperatures. X-ray diffraction experiments reveal that all the samples are crystallized in orthorhombic with space group Pbam phase. The extreme value of lattice parameters is observed at the sample with annealing temperature of 700 °C. Six samples with annealing temperatures of 240、300、500、700、900、1100 °C are idendified by TEM and SAED scheme, which can be labeled in the form of long axis × short axis as 23(6) nm×44(14) nm、24(7) nm×49(19) nm、33(14) nm×66(25) nm、31(9) nm×69(24) nm、54(13) nm×95(27) nm、114(52) nm×409(109) nm, respectively。All the long axis of nanorods are parallel to c axis of the crystal. The <LC> symbol is employed to label the long axis of nanorods and in place of sample name. An antiferromagnetic (AFM) peak was observed in <LC>=409 nm sample in the ac magnetic susceptibility experiment. No similar peak was found in another sample. These observations implied the occurrence of size effect between <LC>=69 and 409 nm. The AFM peak of <LC>=409 nm is decreased with increasing applied magnetic field, and shifted to lower temperature. The 1 T magnetic field is not able to eliminate the AFM peak. Hystersis loop were not found in all samples at 2 K. The maxima fitted saturated magnetic moment were found in <LC>=69 nm sample, which is consisted with the observation of the maxima value of lattice parameters. Raman spectroscopy revealed a Raman peak at 697 cm-1 is correlated with Mn1-O2/O3 plane of <LC>=409 nm as temperature varied. The Mn1-O2 bond length is also associated with Raman peak at 686 cm-1. No similar behavior of these two Raman peak were found in <LC>=69 nm sample. This indicates that the more III distortion inside the smaller size of nanorods, the less adjust and response of crystal vibration. And this phenomena, also weakness the magnetic ordering at lower temperature. Chun-Chuen Yang 楊仲準 2013 學位論文 ; thesis 81 zh-TW
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language zh-TW
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description 碩士 === 中原大學 === 物理研究所 === 101 === Abstract Various size of HoMn2O5 nanorods were fabricated by combining hydrothermal and annealing method with 240、300、500、700、900、1100 °C annealing temperatures. X-ray diffraction experiments reveal that all the samples are crystallized in orthorhombic with space group Pbam phase. The extreme value of lattice parameters is observed at the sample with annealing temperature of 700 °C. Six samples with annealing temperatures of 240、300、500、700、900、1100 °C are idendified by TEM and SAED scheme, which can be labeled in the form of long axis × short axis as 23(6) nm×44(14) nm、24(7) nm×49(19) nm、33(14) nm×66(25) nm、31(9) nm×69(24) nm、54(13) nm×95(27) nm、114(52) nm×409(109) nm, respectively。All the long axis of nanorods are parallel to c axis of the crystal. The <LC> symbol is employed to label the long axis of nanorods and in place of sample name. An antiferromagnetic (AFM) peak was observed in <LC>=409 nm sample in the ac magnetic susceptibility experiment. No similar peak was found in another sample. These observations implied the occurrence of size effect between <LC>=69 and 409 nm. The AFM peak of <LC>=409 nm is decreased with increasing applied magnetic field, and shifted to lower temperature. The 1 T magnetic field is not able to eliminate the AFM peak. Hystersis loop were not found in all samples at 2 K. The maxima fitted saturated magnetic moment were found in <LC>=69 nm sample, which is consisted with the observation of the maxima value of lattice parameters. Raman spectroscopy revealed a Raman peak at 697 cm-1 is correlated with Mn1-O2/O3 plane of <LC>=409 nm as temperature varied. The Mn1-O2 bond length is also associated with Raman peak at 686 cm-1. No similar behavior of these two Raman peak were found in <LC>=69 nm sample. This indicates that the more III distortion inside the smaller size of nanorods, the less adjust and response of crystal vibration. And this phenomena, also weakness the magnetic ordering at lower temperature.
author2 Chun-Chuen Yang
author_facet Chun-Chuen Yang
SHENG-SIANG YOU
游聲翔
author SHENG-SIANG YOU
游聲翔
spellingShingle SHENG-SIANG YOU
游聲翔
Interplay between structure and magnetism and effect of size of HoMn2O5 nanorods
author_sort SHENG-SIANG YOU
title Interplay between structure and magnetism and effect of size of HoMn2O5 nanorods
title_short Interplay between structure and magnetism and effect of size of HoMn2O5 nanorods
title_full Interplay between structure and magnetism and effect of size of HoMn2O5 nanorods
title_fullStr Interplay between structure and magnetism and effect of size of HoMn2O5 nanorods
title_full_unstemmed Interplay between structure and magnetism and effect of size of HoMn2O5 nanorods
title_sort interplay between structure and magnetism and effect of size of homn2o5 nanorods
publishDate 2013
url http://ndltd.ncl.edu.tw/handle/26089448905035924255
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AT yóushēngxiáng homn2o5nàimǐchǐcùnxiàoyīngyǔjiégòucíxìngjiāohùzuòyòngyánjiū
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