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  1. NTU Theses and Dissertations Repository
  2. 理學院
  3. 物理學系
請用此 Handle URI 來引用此文件: http://tdr.lib.ntu.edu.tw/jspui/handle/123456789/64702
完整後設資料紀錄
DC 欄位值語言
dc.contributor.advisor陳政維(Jeng-Wei Chen)
dc.contributor.authorDing-En Linen
dc.contributor.author林鼎恩zh_TW
dc.date.accessioned2021-06-16T22:57:40Z-
dc.date.available2012-08-10
dc.date.copyright2012-08-10
dc.date.issued2012
dc.date.submitted2012-08-09
dc.identifier.citation1. E.V. Sampathkumaran, S. Majumdar. , W. Schneider, S. L. Molodtsov, C. Laubschat, Physica B 312-313, 152 (2002).
2. S. Baran, J. Leciejewicz, M. Slaski, A. Szytula, B. Penc, Y. Ding, N. Stusser, J. Alloys Compounds 256, L18 (1997).
3. T. Nishioka, Y. Tabata, T. Taniguchi, Y. Miyako, J. Phys. Soc. Jpn. 69, 1012 (2000).
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5. D. Huo, J. Sakurai, T. Kuwai, Y. Isikawa, Phys. Rev. B 64, 224405 (2001).
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9. A.C. Hewson, The Kondo Problem to Heavy Fermions (Cambridge University Press, 1993).
10. I. Das and E. V. Sampathkumaran, Phys. Rev. B 49, 6 (1994).
11. J de la Venta, Ali C Basaran, T Grant, A J S Machado, M R Suchomel, R T Weber, Z Fisk and Ivan K Schuller, Supercond. Sci. Technol. 24 075017 (2011).
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14. A.V. Morozkin, Jinlei Yao and Y. Mozharivskyj, Journal of Solid State Chemistry (2012).
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dc.identifier.urihttp://tdr.lib.ntu.edu.tw/jspui/handle/123456789/64702-
dc.description.abstractThe crystal structure, electrical resistivity (ρ) and magnetic susceptibility (χdc of the R2CoAl3 (R = Y and rare earth element) compounds are investigated. Powder X-ray diffraction patterns reveal that all the samples crystallize in the cubic MgCu2 type structure except Ho and Er and lattice parameters are found to decrease monotonically from 8.1A to 7.7 A with increasing the atomic number of R. Structure transforms from cubic to hexagonal in Ho and Er sample The ρ(T) curve of La2CoAl3 drops to zero at 6 K and the diamagnetic behavior observed in χdc(T) curve confirms the presence of bulk superconductivity with Tc=6K and ΔTc=1K. Above the superconducting transition temperature the ρ(T) curve exhibit a metallic behavior. The ρ(T) curves of R2CoAl3 (R =Sm, Tb, Ho, and Er ) compounds shows the etallic behavior with local minima at low temperature. The χdc(T) vurves for all samples studied follow the Curie-Weiss behavior for T > 150 K except Sm, with the obtained value of effective moments μeff slightly larger than the moment of the corresponding R3+ ions. The occurrence of anomaly in the χdc(T) curves and a drop off in the ρ(T) curve at the corresponding temperatures indicate that antiferromagnetic transition occurs in R2CoAl3 (R = Ce, Pr and Nd) and ferromagnetic transition in Sm2CoAl3 and Tb2CoAl3 compounds.en
dc.description.provenanceMade available in DSpace on 2021-06-16T22:57:40Z (GMT). No. of bitstreams: 1
ntu-101-R99222068-1.pdf: 4240845 bytes, checksum: 6a6e61a40cf8c8b6c2d05ae355f805bf (MD5)
Previous issue date: 2012
en
dc.description.tableofcontents致謝.......................................................i
Abstract .................................................ii
Table of content.........................................iii
List of Figures .......................................... v
List of Tables...........................................vii
Chapter 1 Introduction ................................... 1
a. Overview .............................................. 1
b. Spin-glass behavior ................................... 5
c. Kondo effect .......................................... 7
d. Superconductivity ..................................... 9
Chapter 2 Experimental Detail............................ 11
a. Sample preparation ................................... 11
b. X-ray diffraction..................................... 13
c. Electrical resistivity measurement ................... 14
d. Susceptibility and magnetization measurement.......... 15
e. 3He cryostat.......................................... 16
Chapter 3 Theoretical Model ............................. 19
a. The electrical resistivity of metals ................. 19
b. Magnetic susceptibility .............................. 23
Chapter 4 Results and discussions ....................... 25
a. Y2CoAl3 .............................................. 25
b. La2CoAl3 ............................................. 30
c. Ce2CoAl3...............................................34
d. Pr2CoAl3...............................................38
e. Nd2CoAl3 ..............................................42
f. Sm2CoAl3 ..............................................43
g. Gd2CoAl3 ..............................................51
h. Tb2CoAl3...............................................55
i. Ho2CoAl3 ..............................................59
j. Er2CoAl3 ..............................................63
Chapter 5 Summary . ......................................67
a. Crystallographic structures ...........................67
b. Electrical resistivity ................................69
c. Magnetic susceptibility................................70
References. ..............................................71
dc.language.isoen
dc.subject超導現象zh_TW
dc.subject近藤效應zh_TW
dc.subject自旋玻璃zh_TW
dc.subjectsuperconductivityen
dc.subjectKondo effecten
dc.subjectspin galssen
dc.titleR2CoAl3(R=Y and 鑭系元素)三元稀土化合物之物性研究zh_TW
dc.titleStructure, Electrical and Magnetic Properties of R2CoAl3
(R = Y and rare-earth ions) compounds
en
dc.typeThesis
dc.date.schoolyear100-2
dc.description.degree碩士
dc.contributor.oralexamcommittee林昭吟,陳洋元
dc.subject.keyword超導現象,近藤效應,自旋玻璃,zh_TW
dc.subject.keywordsuperconductivity,Kondo effect,spin galss,en
dc.relation.page73
dc.rights.note有償授權
dc.date.accepted2012-08-09
dc.contributor.author-college理學院zh_TW
dc.contributor.author-dept物理研究所zh_TW
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