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^<141>Pr nuclear spin relaxation time in Pr and related compounds.

^<141>Pr nuclear spin relaxation time in Pr and related compounds.
^<141>Pr及相关化合物中的Pr核自旋弛豫时间。
批准号:
07640465
负责人:
SHIMIZU Kenji
金额:
$1.41万
依托单位:
依托单位国家:
日本
项目类别:
Grant-in-Aid for Scientific Research (C)
财政年份:
1995
资助国家:
日本
项目状态:
已结题
起止时间:
1995 至 1996

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中文摘要
翻译
稀土自旋回波核磁共振测量了Pr化合物及其相关化合物:RCo_<5+x> (R=Pr, Tb), Pr_2Fe_<14>B,Pr_xGd_<1-x>Ni, Sm_xGd_<1-x>Ni和RFe_<11>Ti (R=稀土)。Pr_xGd_<1-x>Ni的^<141>Pr核磁共振信号出现在较宽的频率范围内。在Pr_<0.2>Gd_<0.8>Ni的情况下,频谱宽度约为1000MHz,在2800 ~ 3800MHz的频率范围内,与Pr_2Fe_<14>B和Sm_xGd_<1-x>Ni不同。超精细场分析结果表明,PrCo_5和Pr_<0.2>Gd_<0.8>Ni的稀土离子磁矩分别为2.4和2.6mu_B。在1.4K ~ 4.2K的温度范围内,在PrCo_5、Pr_2Fe_<14>B和Pr_xGd_<1-x>Ni上测量了原子核自旋弛豫时间T_2。发现自旋-自旋弛豫服从简单的指数函数,呈现快速衰减。在PrCo_5中,1.4K时T_2为4.2musec, 4.2K时T_2为2.1musec。在Pr_xGd_<1-x>中,当x=0.2和0.35时,T_2在1.4K时分别为-5musec和-3musec。在Sm_<0.2>Gd_<0.8>Ni中,它们大约是^<147>Sm的1/20到1/30。假设观测到的信号主要来自于-1/2 <互变异构体> 1/2跃迁对应的线,则利用关系T_1/T_2= (I+1/2)^2估计自旋晶格弛豫时间T_1。得到PrCo_5和Pr_xGd_<1-x>Ni的T_1T分别为- 110kmusc和- 50kmusc。对于Pr_2Fe_<14>B, f和g位点的T_1T分别为900kmusc和300kmusc。
英文摘要
Rare-earth spin-echo NMR measurements have been carried out on Pr compounds and the related compounds : RCo_<5+x> (R=Pr, Tb), Pr_2Fe_<14>B,Pr_xGd_<1-x>Ni, Sm_xGd_<1-x>Ni and RFe_<11>Ti (R=rare-earth). The ^<141>Pr NMR signal of Pr_xGd_<1-x>Ni appeared in the wide frequency range. In the case of Pr_<0.2>Gd_<0.8>Ni, the width of spectrum was about 1000MHz, in the frequency range from 2800 to 3800MHz, which was different from those of Pr_2Fe_<14>B and Sm_xGd_<1-x>Ni. The magnetic moments of rare-earth ions in the compounds which were estimated from the hyperfine field analysis were 2.4 and 2.6mu_B for PrCo_5 and Pr_<0.2>Gd_<0.8>Ni, respectively. ^<141>Pr nuclear spin-spin relaxation times, T_2, have been measured on PrCo_5, Pr_2Fe_<14>B and Pr_xGd_<1-x>Ni in the temperature range from 1.4K to 4.2K.It was found that the spin-spin relaxation followed a simple exponential function and showed fast decay. In PrCo_5, T_2 were 4.2musec at 1.4K and 2.1musec at 4.2K.In Pr_xGd_<1-x>Ni, T_2 at 1.4K were -5musec and -3musec for x=0.2 and 0.35, respectively. These were roughly 1/20 to 1/30 of ^<147>Sm in Sm_<0.2>Gd_<0.8>Ni. Assuming that the observed signals arised mostly from the line corresponding to the -1/2 <tautomer> 1/2 transition, the spin-lattice relaxation time, T_1, was estimated by using the relation T_1/T_2= (I+1/2)^2. T_1T was obtained to be - 110Kmusec and -50Kmusec for PrCo_5 and Pr_xGd_<1-x>Ni, respectively. For Pr_2Fe_<14>B, T_1T were obtained to be 900Kmusec and 300Kmusec for the f and g sites, respectively.
期刊论文(8)
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会议论文
清水建次: "^<143>Nd NMR Study of 3d and 4f Magnetism in Nd_2 (Fe_<1-x>Co_x)_<14>B and Nd_2 (Fe_<1-y>Ni_y)_<14>B" Solid State Communications. 96. 671-674 (1995)
Kenji Shimizu:“^<143>Nd NMR 研究 Nd_2 (Fe_<1-x>Co_x)_<14>B 和 Nd_2 (Fe_<1-y>Ni_y)_<14>B 中的 3d 和 4f 磁性”固体国家通讯。96。671-674(1995)
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清水建次: "^<141>Pr and ^<147>Sm Spin-Echo NMR in R_xGd_<1-x>Ni (R=Pr and Sm)" Journal of Phys. Soc. Jpn.65. 2736-2737 (1996)
Kenji Shimizu:“R_xGd_<1-x>Ni(R=Pr 和 Sm)中的 ^<141>Pr 和 ^<147>Sm 自旋回波 NMR”Soc.65。 )
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通讯作者:
K.Shimizu, K.Ichinose et al.: "^<143>Nd NMR Study of 3d and 4f Magnetism in Nd_2 (Fe_<1-x>Co_x)_<14>B and Nd_2 (Fe_<1-y>Ni_y)_<14>B" Solid State Commun.vol.96. 671-674 (1995)
K.Shimizu、K.Ichinose 等人:“^<143>Nd NMR 研究 Nd_2 (Fe_<1-x>Co_x)_<14>B 和 Nd_2 (Fe_<1-y>Ni_y) 中的 3d 和 4f 磁性
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清水建次: "143Nd NMR Study of 3d and 4f Magnetism in Nd2 (Fel-xCox) 14B and Nd2 (Fe1-yNiy) 14B" Solid State Communication. 96. 671-674 (1995)
Kenji Shimizu:“Nd2 (Fel-xCox) 14B 和 Nd2 (Fe1-yNiy) 14B 中 3d 和 4f 磁性的 143Nd NMR 研究”固态通信。 96. 671-674 (1995)
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