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  1. NTU Theses and Dissertations Repository
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請用此 Handle URI 來引用此文件: http://tdr.lib.ntu.edu.tw/jspui/handle/123456789/62175
完整後設資料紀錄
DC 欄位值語言
dc.contributor.advisor陳政維(Jenq-Wei Chen)
dc.contributor.authorYi-Hsuan Suen
dc.contributor.author蘇怡瑄zh_TW
dc.date.accessioned2021-06-16T13:31:57Z-
dc.date.available2013-07-26
dc.date.copyright2013-07-26
dc.date.issued2013
dc.date.submitted2013-07-19
dc.identifier.citation[1] Jun Nagamatsu, Norimasa Nakagawa, Takahiro Muranaka, Yuji Zenitani and Jun Akimitsu, Superconductivity at 39 K in magnesium diboride, Nature 410, 63 (2001).
[2] M. Xu, H. Kitazawa, Y. Takano, J. Ye, K. Nishida, H. Abe, A. Matsushita and G.Kido, Single crystal MgB2 with anisotropic superconducting properties, cond-mat/0105271 (2001)
[3] Cristina Buzea and Tsutomu Yamashita, Review of superconducting properties of MgB2, cond-mat/0108265 (2001)
[4] S. L. Bud’ko, G. Lapertot, C. Petrovic, C. E. Cunningham, N. Anderson and P. C. Canfield, Boron Isotope Effect in Superconducting MgB2, Phys. Rev. Lett. 86, 1877 (2001)
[5] D. G. Hinks, H. Claus and J. D. Jorgensen, The complex nature of superconductivity in MgB2 as revealed by the reduced total isotope effect, Nature 411, 457 (2001)
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dc.identifier.urihttp://tdr.lib.ntu.edu.tw/jspui/handle/123456789/62175-
dc.description.abstract三元稀土合金R8CoGa3(R = 釔及稀土元素),結構為六角晶系,空間群為P63mc 與Space No. 186。晶格常數由La8CoGa3的a = 11.05 A and c = 7.064 A隨著稀土元素的原子量增加減少。
這個系列R8CoGa3的電阻率量測範圍由室溫的300 K量測到低溫約4~5 K。La8CoGa3這個樣品在6 K顯示典型的超導相轉換。而對於R = Ce, Pr, Nd, Gd, Dy, Ho的樣品們,電阻率隨著溫度下降而上升,分別在不同的溫度顯現出電阻極大值。而Y8CoGa3這個樣品則在溫度為155 K時顯示出電阻極小值。部分的樣品的雌性電阻在某些溫度區間有「-lnT」¬的傾向,這可能與「近藤效應(Kondo effect)」有關。¬
在磁化率的量測部分,量測了R = La, Ce, Pr, Nd的樣品。在La8CoGa3的部分,量測出來發現磁化率在4 K的部分有超導的現象,和電阻量測的6 K超導溫度並不相同。Ce8CoGa3和Pr8CoGa3顯示出反鐵磁性,Nd8CoGa3而則是顯示出鐵磁性。
zh_TW
dc.description.abstractThese R8CoGa3 (R = Y and rare earth atoms) compounds crystallize in the hexagonal structure with space group P63mc (Space No. 186). The obtained values of the lattice parameters are a = 11.05 A and c = 7.064 A for La8CoGa3. Both the values of a and c are found decreasing monotonically with increasing atomic number of the rare earth ions.
The temperature dependence of electrical resistivity ρ(T) below room temperature of the R8CoGa3 have been investigated. The ρ(T) curve of La8CoGa3 shows a typical superconducting phase transition at 6 K. The electrical resistivity of R8CoGa3 (for R = Ce, Pr, Nd, Gd, Dy, Ho) are found increasing with decreasing temperature T from room temperature and reveal local maximum. The ρ(T) of Y8CoGa3 shows a local minimum at 155 K. The magnetic resistivity of some compounds show “-lnT” dependence which may due to the Kondo effect.
The susceptibility measurements are done for R = La, Ce, Pr, Nd. For La8CoGa3, superconducting transition is observed but at 4 K which differs from 6 K. It shows the antiferromagnetic correlation in the paramagnetic state for Ce8CoGa3 and Pr8CoGa3 While for Nd8CoGa3, it shows the ferromagnetic correlation in the paramagnetic state.
en
dc.description.provenanceMade available in DSpace on 2021-06-16T13:31:57Z (GMT). No. of bitstreams: 1
ntu-102-R00222017-1.pdf: 2051485 bytes, checksum: 24fe5355e689ca292e82af623952498d (MD5)
Previous issue date: 2013
en
dc.description.tableofcontentsTable of Contents
誌謝…………………………………………………………………………………...i
摘要………………………………………………………...........................................ii
Abstract..........................................................................................................................iii
Table of Contents...........................................................................................................iv
List of figures ................................................................................................................vi
List of tables ..................................................................................................................x
Chapter1 Introduction ……………………………………………………………….1
1.a Superconductivity ………………………………………………………….1
1.b The superconductivity of MgB2 ………………….....................................3
1.c AlB2 structure and R8CoGa3 series ……………….........................................5
Chapter2 Theoretical Model ……………………………………..…………………..13
2.a The electrical resistivity of metals ……………………………….………...13
2.b Kondo Effect …………………………………………………….......…….18
2.c Magnetic susceptibility ..........................................................……………..21
2.d Spin glass ….............................................................………………………...23
Chapter 3 Experimental Detail ...............................................................………….25
3.a Sample Preparation .......................................................................………….25
3.b X-ray diffraction ........................................................................................27
3.c Electrical Resistivity Measurement …............................................…………28
3.d Susceptibility and magnetization measurement ......................…………..29
3.e 3He cryostat ………...............................................................…………….30
Chapter 4 Results and Discussion ................................................................…………33
4.a. La8CoGa3 ......................................................………………………………..34
4.b. Ce8CoGa3 ...................................................………………………………….37
4.c. Pr8CoGa3 ..................................................…………………………………..43
4.d. Nd8CoGa3 ....................................................…………………………………48
4.e. Sm8CoGa3...................................................................……………………….53
4.f. Gd8CoGa3…………........................................................................………….55
4.g. Dy8CoGa3……………………………............................................................58
4.h. Ho8CoGa3………………................................................................................61
4.i. Y8CoGa3………………...................................................................................64
Chapter 5 Summary …...........……………….........................................................67
5.a. Crystal structure …………………………………………………………67
5.b. Electrical resistivity …………………………………………………………69
5.c. Susceptibility ………………………………………………………………73
Reference ………………........................................................................................74
dc.language.isozh-TW
dc.title三元稀土合金R8CoGa3(R = 釔及稀土元素)之結構、電性與磁性研究zh_TW
dc.titleStructure, Electrical and Magnetic Properties of the R8CoGa3 (R = Y and rare earth atoms) compoundsen
dc.typeThesis
dc.date.schoolyear101-2
dc.description.degree碩士
dc.contributor.oralexamcommittee張慶瑞(Ching-Ray Chang),周方正(F.C. Chou),林金福(King-Fu Lin)
dc.subject.keyword稀土元素,三元合金,AlB2結構,近藤效應,超導,zh_TW
dc.subject.keywordrare earth,ternary alloy,AlB2 structure,Kondo effect,superconductivity,en
dc.relation.page78
dc.rights.note有償授權
dc.date.accepted2013-07-19
dc.contributor.author-college理學院zh_TW
dc.contributor.author-dept物理研究所zh_TW
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