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| DC 欄位 | 值 | 語言 |
|---|---|---|
| dc.contributor.advisor | 王立民 | |
| dc.contributor.author | Jing-Yuan Zhang | en |
| dc.contributor.author | 張景淵 | zh_TW |
| dc.date.accessioned | 2021-06-08T00:55:47Z | - |
| dc.date.copyright | 2015-03-16 | |
| dc.date.issued | 2015 | |
| dc.date.submitted | 2015-02-13 | |
| dc.identifier.citation | [1] Y. Kamihara, T. Watanabe, M. Hirano, and H. Hosono: J. Am. Chem. Soc. 130(2008) 3296.
[2] Ren Zhi-An et al 2008 Chinese Phys. Lett. 25 2215 [3] Hsu F. C., Luo J. Y., Yeh K. W., Chen T. K., Huang T. W., Wu Phillip M., Lee Y.C., Huang Y. L., Chu Y. Y., Yan D. C. and Wu M. K., Proc. Natl. Acad. Sci. U.S.A., 105 (2008) 14262 [4] Kuo-Wei Yeh et al EPL, 84 (2008) 37002 arXiv:0808.0474 [5] Kumary T G, Baisnab D K, Janaki J, Mani A, SargunaR M, Ajikumar P K, Tyagi A K and Bharathi A 2009 arXiv:0904.1502v1 [6] E Bellingeri et al 2009 Supercond. Sci. Technol. 22 105007 [7] E Bellingeri et al Appl. Phys. Lett. 96, 102512 (2010) [8] Y. Imai et al., Physica C (2010) [9] J. Luo, T. P. Orlando, J. M. Graybeal, X. D. Wu, and R. Muenchausen, Phys. Rev. Lett.68, 690 (1992). [10] V. M. Vinokur, V. B. Geshkenbein, M. V. Feigel’man, and G. BlatterPhys. Rev. Lett. 71, 1242 (1993) [11] Wu Liu, T. W. Clinton, and C. J. Lobb Phys. Rev. B 52, 7482 (1995) – Published 1 September 1995 [12] W. Gob, W. Liebich, W. Lang, I. Puica, Roman Sobolewski, R. Rossler, J. D. Pedarnig, and D. Bauerle Phys. Rev. B 62, 9780 (2000) – Published 1 October 2000 [13] N. B. Kopnin and V. M. Vinokur Phys. Rev. Lett. 83, 4864 (1999) [14] S C Speller et al 2011 Supercond. Sci. Technol. 24 075023 [15] Poole, Farach, Creswick, Superconductivity [16] 張裕恆 李春芝,超導物理,page 242 [17] KITTEL, Introduction to Solid State Physics 8th Edition [18] B. C. sales et al 2009 Phys. Rev. B 79, 094521 [19] L. J. van der Pauw, Philips. Res. Pepts. 13, 1-9(1958) [20] Y. Han, W. Y. Li, L. X. Cao, X. Y. Wang, B. Xu, B. R. Zhao, Y. Q. Guo, and J. L. Yang PRL 104, 017003 (2010) [21] S C Speller et al 2011 Supercond. Sci. Technol. 24 075023 [22] N. R. Werthamer, E. Helfand, and P. C. Hohenberg Phys. Rev. 147, 295 [23] Wang Z D, Dong J and Ting C S 1994 Phys. Rev. Lett. 72 3875 [24] Ao P 1998 J. Phys.: Condens. Matter 10 L677 [25] Zhu B Y, Xing D Y, Wang Z D, Zhao B R and Zhao Z X 1999 Phys. Rev. B 60 3080 [26] L M Wang et al 2013 J. Phys.: Condens. Matter 25 395702 [27] L M Wang et al 2011 Phys. Rev. B 83, 134506 [28] W. N. Kang, D. H. Kim, S. Y. Shim, J. H. Park, T. S. Hahn, S. S. Choi, W. C. Lee, J. D. Hettinger, K. E. Gray, and B. Glagola Phys. Rev. Lett. 76, 2993 [29] Samoilov A V 1993 Phys. Rev. Lett. 71 617 [30] W. N. Kang, Hyeong-Jin Kim, Eun-Mi Choi, Heon Jung Kim, Kijoon H. P. Kim, and Sung-Ik Lee Phys. Rev. B 65, 184520 [31] Dorsey A T and Fisher M P A 1992 Phys. Rev. Lett. 68 694 [32] Vinokur V M, Geshkenbein V B, Feigel’man M V and Blatter G 1993 Phys. Rev. Lett. 71 1242 [33] Lei H, Hu R, Choi E S and Petrovic C 2010 Phys. Rev. B 82 134525 [34] H.H. Chang et al., Physica C (2009) [35] Anderson P W 1991 Phys. Rev. Lett. 67 2092 [36] Naira S, Wirtha S, Friedemanna S, Steglicha F, Sic Q and Schofield A J 2012 Adv. Phys. 61 583 [37] Harris M, Yan Y F, Matl P, Ong N P, Anderson P W, Kimura T and Kitazawa K 1995 Phys. Rev. Lett. 75 1391 [38] H. C. Yang, L. M. Wang, and H. E. Horng, Phys. Rev. B59, 8956 (1999). [39] Zeldov E, Amer N M, Koren G, Gupta A, Gambino R J and McElfresh M W 1989 Phys. Rev. Lett. 62 3093 [40] Palstra T T M, Batlogg, van Dover R B, Schneemeyer L F and Waszczak J V 1990 Phys. Rev. B41 6621 [41] Y. Abulafa, A Shaulov, Y. Wolfus, R. Prozorov, L. Burlachkov, and Y. Yeshurun, Phys. Rev. Lett. Volume 77, number 8 (1996) [42] P. W. Anderson, Phys. Rev. Lett.9, 309 (1962). [43] Y. B. Kim, C. F. Hempstead, and A. R. Strnad, Phys. Rev. 131, 2486 (1963). [44] Y. Yeshurun and A. P. Malozemoff, Phys. Rev. Lett.60, 2202 (1988). [45] Farallel D E, Williams C M, Wolf S A, Bansal N P and Kogan V G 1988 Phys. Rev. Lett. 61 2805 [46] Farallel D E, Rice J P, Ginsberg D M and Liu J Z 1990 Phys. Rev. Lett. 64 1573 [47] Farallel D E, Bonham S, Foster J, Chang Y C, Jiang P Z, Vandervoort K G, Lam D J and Kogan V G 1989 Phys. Rev. Lett. 63 782 [48] Martinez J C, Brongersma S H, Koshelev A, Ivlev B, Kes P H, Griessen R P, de Groot D G, Tarnavski Z and Menovsky A A 1992 Phys. Rev. Lett. 69 2276 [49] Gray K E, Kampwirth R T and Farrel D E 1990 Phys. Rev. B 41 819 [50] Farallel D E, Beck R G, Booth M F, Bukowski C J and Ginsberg D M 1990 Phys. Rev. B 42 6758 | |
| dc.identifier.uri | http://tdr.lib.ntu.edu.tw/jspui/handle/123456789/18230 | - |
| dc.description.abstract | 本研究利用FeSe0.5Te0.5單晶樣品,量測其混合態及正常態之縱向電阻率及橫向電阻率(霍爾電阻率)。依據Anderson和Kim之理論,計算FeSe0.5Te0.5之活化能約400-1500 K,相對於其他超導體而言是比較低的,表示其釘扎力也較低。並計算其活化能與磁場之冪次關係,符合塑性渦旋蠕動模型。其橫向及縱向電阻率冪次關係之beta值約為1,並不符合W-T理論。由磁場平行c軸及磁場垂直c軸之電阻率計算出上臨界場不同向性γ值約等於1.61。依據Kohler’s rule討論FeSe0.5Te0.5正常態磁阻特性,FeSe0.5Te0.5系統不屬於費米液體。
本論文也研究利用RF磁控濺鍍系統製作FeSe0.5Te0.5薄膜。實驗配製不同成分比例之靶材及主要使用MgO基板,搭配不同的鍍膜參數,雖未成功沉積出超導薄膜,但由EDS分析來看,得知薄膜Te含量易受靶材成分之元素比例影響。要有效地控制薄膜組成比例使之達到Fe : Se : Te = 1 : 0.5 : 0.5,還需更一步研究。 | zh_TW |
| dc.description.abstract | In this thesis, the in-plane longitudinal and Hall resistivities of superconducting FeSe0.5Te0.5 (FST) single crystals in the mixed state and the normal state were measured. According to Anderson-Kim theory, we calculated activation energy to be in 102 K order. The values of activation energy of FeSe0.5Te0.5 are relatively small than other superconductors, indicating a relatively weak vortex pinning.We also obtained a power law magnetic field dependence of activation energy which are within the plastic vortex creep model.The scaling behavior obtained with beta=1 is not in agreement with W-T theory.Anisotropic upper critical fields and coherence lengths with an anisotropy ratio of 1.61 have been deduced. The normal-state magnetoresistance were scaled by the Kohler’s rule.
In addition, we deposited FeSexTey films mainly on MgO substrates by radio frequency sputtering. Using different target of stoichiometry and by adjusting parameters, none of films reached zero resistance. EDS analysis revealed that the ratio of Te in films are subject to the composition of the target. To deposit FeSexTey films with Fe : Se : Te = 1 : 0.5 : 0.5 requires further works. | en |
| dc.description.provenance | Made available in DSpace on 2021-06-08T00:55:47Z (GMT). No. of bitstreams: 1 ntu-104-R99222085-1.pdf: 2149900 bytes, checksum: defb1e9c4a78f9867b779b72b051c1e7 (MD5) Previous issue date: 2015 | en |
| dc.description.tableofcontents | 中文摘要............................................................I
英文摘要...........................................................II 目錄...............................................................III 圖目錄.............................................................VI 表目錄.............................................................IX 第一章 緒論...............................................1 1.1 鐵基超導體.......................................................1 1.2 FeSe0.5Te0.5薄膜...................................................3 1.3 混合態霍爾效應及scaling behavior .........................4 1.4 研究內容.........................................................5 第二章 超導體概述.........................................6 2.1 超導體之研究發展歷史.............................................6 2.2 超導體零電阻特性.................................................7 2.3 完美反磁及麥斯納效應(Meissner Effect) ..............................8 2.4 超導體內部磁場及London方程式....................................8 2.5 Ginzburg-Landau方程式............................................11 2.6 第一類超導體及第二類超導體......................................15 2.7 磁通渦旋線......................................................16 2.8 Anderson-Kim磁通蠕動模型........................................18 第三章 實驗步驟、技術與量測..............................20 3.1 鐵硒碲FeSe0.5Te0.5單晶製作.......................................20 3.1.1 製作FeSe0.5Te0.5塊材........................................20 3.1.2 製作FeSe0.5Te0.5單晶........................................22 3.2 鐵硒碲FeSe0.5Te0.5薄膜製作........................................23 3.2.1 製作FeSexTey鍍膜用靶材....................................23 3.2.2 鍍膜參數..................................................23 3.2.3 基板清洗..................................................24 3.3 真空及薄膜技術................................................ ..25 3.3.1 分子在真空中的平均自由徑..................................25 3.3.2 真空系統..................................................25 3.3.3 射頻磁控濺鍍..............................................27 3.4 量測系統........................................................28 3.4.1 XRD......................................................28 3.4.2 EDS.......................................................30 第四章 實驗結果與討論....................................32 4.1 FeSe0.5Te0.5單晶傳輸特性..........................................32 4.1.1 FeSe0.5Te0.5單晶XRD.........................................32 4.1.2 FeSe0.5Te0.5單晶電阻率........................................33 4.1.3 FeSe0.5Te0.5單晶上臨界場Hc2...................................34 4.1.4 FeSe0.5Te0.5單晶釘扎能探討....................................36 4.1.5 混合態霍爾效應及scaling behavior ....................38 4.1.6 正常態霍爾效應.............................................41 4.2 Fe-Se-Te薄膜....................................................43 第五章 結論..............................................47 Reference..........................................................48 | |
| dc.language.iso | zh-TW | |
| dc.title | 鐵基超導 鐵-硒-碲 之縱向與橫向霍爾電阻率之研究:釘扎效應與異常電傳輸性質 | zh_TW |
| dc.title | Longitudinal and Transverse Hall Resistivities in FeSe0.5Te0.5 Single Crystals : Pinning Effect and Anomalous Electrical Transport Properties | en |
| dc.type | Thesis | |
| dc.date.schoolyear | 103-1 | |
| dc.description.degree | 碩士 | |
| dc.contributor.oralexamcommittee | 陳昭翰,吳秋賢 | |
| dc.subject.keyword | 鐵基超導,霍爾效應,超導混合態,釘扎效應,鐵-硒-碲薄膜, | zh_TW |
| dc.subject.keyword | iron-based superconductor,hall effect,mixed state of superconductor,pinning effect,Fe-Se-Te flims, | en |
| dc.relation.page | 50 | |
| dc.rights.note | 未授權 | |
| dc.date.accepted | 2015-02-13 | |
| dc.contributor.author-college | 理學院 | zh_TW |
| dc.contributor.author-dept | 物理研究所 | zh_TW |
| 顯示於系所單位: | 物理學系 | |
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