| 研究生: |
洪綮嶸 Hung, Chi-jung |
|---|---|
| 論文名稱: |
利用固相燒結法製備FeSe及其超導性質之研究 Preparation of FeSe by solid state sintering and characterization of superconducting properties |
| 指導教授: |
齊孝定
Qi, Xiaoding |
| 學位類別: |
碩士 Master |
| 系所名稱: |
工學院 - 材料科學及工程學系 Department of Materials Science and Engineering |
| 論文出版年: | 2009 |
| 畢業學年度: | 97 |
| 語文別: | 中文 |
| 論文頁數: | 89 |
| 中文關鍵詞: | 超導 、鐵硒化合物 |
| 外文關鍵詞: | superconductivity, superconductor, FeSe |
| 相關次數: | 點閱:54 下載:1 |
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本研究以粉末固相燒結法,進行FeSe樣品之製備以及性質之研究並進行FeSe單晶以及磊晶生長實驗。超導材料PbO type-FeSe於2008年8月被發現具有超導性質,且可能為Fe扮演超導電子傳遞關鍵角色而受到重視。其超導特性以及理論機制仍然需要深入的實驗研究來佐證。
為了製備純度較高之PbO type-FeSe樣品,本研究製程條件做系列變化,如溫度、時間,以及樣品成分 (Fe/Se)。研究發現FeSe於750o進行製備可得純FeSe相。文獻得知PbO type-FeSe必須在Se比例較低的的成分組成下生成,本研究實驗Fe:Se為名義成分為1:0.84時具有最佳的PbO type-FeSe。
本研究摻雜不同元素來探討摻雜與超導性質的變化。發現摻雜10%的S可以在不產生相變下提升Tc至12K而原本為7K。進行晶格參數計算,摻雜S產生晶格畸變造成FeSe層狀面(ab平面)縮收。
本研究進行FeSe熔融凝固成核,並於LAO基板上進行磊晶生長。本研究發現使用Sn為助熔劑可以使得FeSe於830oC完全融熔並分佈於基板上。目前研究結果顯示,FeSe於基板上有似磊晶的規則生長。
The focus of this research is to prepare a new superconductive material like FeSe by solid state method and analyzing its superconductivity. The key role of Superconductivity was reported recently for PbO type-FeSe.
In this study was varied with the anneal temperature and time and element ratio(Fe/Se) to make pure phase PbO type-FeSe. The result indicateed that we could get the pure FeSe phases synthesized at 750OC. Other superconducting group reported that when the ratio of Se become less they could get PbO type-FeSe phase. Here we get PbO type-FeSe phase mainly at the ratio Fe:Se 1:0.84 nominally .
Doping is a complex but important subject in superconductor. This research discusses about the effect doping on superconductivity. This research get the result that when doped 10% S can raise the Tc from 7K to 12K without changed the phase. Doping S compress the layer of FeSe(ab plane) by calculating the X-Ray data.
This research try to growth epitaxially on LAO substrate by melting and nucleation method. Using Sn as flux can let the FeSe melt at 830oC and cover over the substrate. We could see some FeSe practices on LAO identically epitaxy.
[1]J.G.Bednorz,and K.A muller,Z” Flux trapping and superconductive glass state in La2CuO4-y:Ba “Phys. Rev. Lett. 58, 1143 (1987)
[2]J.Bardeen,L.N.Cooper,J.R.Schrieffer,”Mircroscopic Theory of superconductivity” Phys.Rev.106,162 (1957).
[3] Fong-Chi Hsu,Jiu-Yong,Luo,Kuo-WeiYeh.”superconductivity in the Pb-O type FeSe “www.pnas.org/cgl/dol/10.1073/ pnas. 0807325105(2008)
[4]H.Q.Yuan,J.Singleton2,”nearly isotropic superconductivity in (Ba,K)Fe2As2” nature 457,29 (2009)
[5]Yoshikazu Mizuguchi “superconductivity at 27K in tetradonal FeSe under hugh pressure” APL 93.152505(2008)
[6] M.K. Wu, J.R. Ashburn, “superconductivity at 93K in a new mixed phase Y-Ba-Cu-O superconducting compound system” Phys. Rev. Lett. 58,908. (1987)
[7]Michel Cyrot and Davor Pavuna, Introduction to Superconductivity andHigh-Tc Materials,World Scientific, (1992).
[8] M. Tinkham, “Introduction to Superconductivity”, McGraw-Hill, Inc.
(1996)
[9]B.D.Josephson .”supercurrents through barriers”Adv.phys., 14,419,(1965)
[10]B.DJosephson ”couplesuperconductors” ,Rev.Mod.Phys.,36,216.(1964)
[11] Kamihara, Y.; Hiramatsu, H.; Hirano, M.; Kawamura, R.; Yanagi, H.; Kamiya, T.; Hosono, H.”Iron-base layered superconductor:LaOFeP” J. Am. Chem. Soc., 128, 10012.( 2006)
[12] Watanabe, T.; Yanagi, H.; Kamiya, T.; Kamihara, Y.; Hiramatsu, H.; Hirano, M.; Hosono, H. “Nikcel-based oxyphosphide superconductor with a layered crystal structure LaOFeP “Inorg. Chem., 46, 7719(2007).
[13] X.J.Wu,Z.Z.Zhang,J”Two-carrier transport and ferromagnetism in FeSe thin films”.Appl.Ph.103,113501(2008)
[14] Lebegue, S.”Electronic structure and properties of the Fermi surface of rhe superconductor LaOFeP” Phys. ReV. B, 75, 035110(2007).
[15] Yoichi Kamihara”Iron-based layered superconductor La[OF]FeAs with Tc~26k”,J.Am.Chem.Soc, 130,3296(2008)
[17]. Shrieffer, J. R. & Brooks, J. S. “Handbook of High-Temperature Superconductivity”(Springer, 2006).
[18] Vedeneev, S. I. et al.” Reaching the Pauli limit in the cuprate Bi2Sr2CuO6+ in high parallel magnetic fields“. Phys. Rev. B 73, 014528 (2006).
[19] Nam, M. S. et al.”Angle dependence of the upper critical field in the layered organic superconductor tetrathiafulvalene” J. Phys. Condens. Matter 11, L477–L484 (1999).
[20]Handbook of ternary alloy phase diagram,10847 ASM international (1995)
[21]W.Schuster,H.Miklerand .L.Komarek,Monatsh”transition metal-chalcogen system VII:the iron selenium phase diagram”.Chem.110,1153(1979)
[22]汪建民 材料分析 中國材料科學會 民國94年三月
[23]M.H Fang. “Superconductivity close to magnetic instability in Fe(Se1−xTex)0.82 “Phy.rev B 78.224503(2008)