Kondo Effect on the Transport Properties of Cuprates
碩士 === 國立交通大學 === 物理研究所 === 90 === A procedure is By conventional point of view, the prominent carriers in cuprates are holes. However, Nagaosa and Lee claimed that the residual resistivity was in the form of r0µnimp/p in the underdoped regime and r0µnimp/(1-p)in the overdoped regime for...
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ndltd-TW-090NCTU01980022016-06-27T16:08:59Z http://ndltd.ncl.edu.tw/handle/42282801822535313906 Kondo Effect on the Transport Properties of Cuprates 近藤效應在銅氧化物導體傳輸特性之研究 Pei-Chun Chung 鍾佩君 碩士 國立交通大學 物理研究所 90 A procedure is By conventional point of view, the prominent carriers in cuprates are holes. However, Nagaosa and Lee claimed that the residual resistivity was in the form of r0µnimp/p in the underdoped regime and r0µnimp/(1-p)in the overdoped regime for Zn-doped cuprates with the Kondo screening effect in the spin-charge separation context. Here nimp is the Zn impurity concentration and p the hole concentration. If this case is true, a novel change of the electronic structure would happen from underdoped to overdoped regime. To verify this important puzzle, we focus our study on the electric transport properties of Y0.7Ca0.3Ba2(Cu1-xZnx) 3O7-y. The key point is to fix a Zn impruity concentration while the carrier concentration in the sample is changed. In contrast with Nagaosa and Lee’s conclusions, we discovered that r0µnimp/p when carrier concentration is changed from overdoped to underdoped. Our experimental suggest the invalidity of the scenario proposed by Nagaosa and Lee. Jiunn-Yuan Lin 林俊源 2002 學位論文 ; thesis 56 zh-TW |
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碩士 === 國立交通大學 === 物理研究所 === 90 === A procedure is By conventional point of view, the prominent carriers in cuprates are holes. However, Nagaosa and Lee claimed that the residual resistivity was in the form of r0µnimp/p in the underdoped regime and r0µnimp/(1-p)in the overdoped regime for Zn-doped cuprates with the Kondo screening effect in the spin-charge separation context. Here nimp is the Zn impurity concentration and p the hole concentration. If this case is true, a novel change of the electronic structure would happen from underdoped to overdoped regime. To verify this important puzzle, we focus our study on the electric transport properties of Y0.7Ca0.3Ba2(Cu1-xZnx) 3O7-y. The key point is to fix a Zn impruity concentration while the carrier concentration in the sample is changed. In contrast with Nagaosa and Lee’s conclusions, we discovered that r0µnimp/p when carrier concentration is changed from overdoped to underdoped. Our experimental suggest the invalidity of the scenario proposed by Nagaosa and Lee.
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author2 |
Jiunn-Yuan Lin |
author_facet |
Jiunn-Yuan Lin Pei-Chun Chung 鍾佩君 |
author |
Pei-Chun Chung 鍾佩君 |
spellingShingle |
Pei-Chun Chung 鍾佩君 Kondo Effect on the Transport Properties of Cuprates |
author_sort |
Pei-Chun Chung |
title |
Kondo Effect on the Transport Properties of Cuprates |
title_short |
Kondo Effect on the Transport Properties of Cuprates |
title_full |
Kondo Effect on the Transport Properties of Cuprates |
title_fullStr |
Kondo Effect on the Transport Properties of Cuprates |
title_full_unstemmed |
Kondo Effect on the Transport Properties of Cuprates |
title_sort |
kondo effect on the transport properties of cuprates |
publishDate |
2002 |
url |
http://ndltd.ncl.edu.tw/handle/42282801822535313906 |
work_keys_str_mv |
AT peichunchung kondoeffectonthetransportpropertiesofcuprates AT zhōngpèijūn kondoeffectonthetransportpropertiesofcuprates AT peichunchung jìnténgxiàoyīngzàitóngyǎnghuàwùdǎotǐchuánshūtèxìngzhīyánjiū AT zhōngpèijūn jìnténgxiàoyīngzàitóngyǎnghuàwùdǎotǐchuánshūtèxìngzhīyánjiū |
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