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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/123456789/88716
完整後設資料紀錄
DC 欄位值語言
dc.contributor.advisor王立民zh_TW
dc.contributor.advisorLi-Min Wangen
dc.contributor.author吳洺宏zh_TW
dc.contributor.authorMing-Hong Wuen
dc.date.accessioned2023-08-15T17:29:24Z-
dc.date.available2023-11-09-
dc.date.copyright2023-08-15-
dc.date.issued2023-
dc.date.submitted2023-08-07-
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[16] https://en.wikipedia.org/wiki/Meissner_effect

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[18] Huebener, Rudolf P. "The Abrikosov Vortex Lattice: Its Discovery and Impact." Journal of Superconductivity and Novel Magnetism 32 (2019): 475-481.

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[24] Jiao, Wen-He, et al. "Possible Evidence for Berezinskii–Kosterlitz–Thouless Transition in Ba (Fe0. 914Co0. 086) 2As2 Crystals." Materials 14.21 (2021): 6294.

[25] Zou, Yi-Chao, et al. "Superconductivity and magnetotransport of single-crystalline NbSe 2 nanoplates grown by chemical vapour deposition." Nanoscale 9.43 (2017): 16591-16595.

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[28] https://zh.wikipedia.org/zh-tw/%E7%A3%81%E9%98%BB%E6%95%88%E5%BA%94

[29] Pavlosiuk, Orest, and Dariusz Kaczorowski. "Galvanomagnetic properties of the putative type-II Dirac semimetal PtTe2." Scientific Reports 8.1 (2018): 11297.

[30] 徐寬,台大物理所碩士論文,2021

[31] Pervin, Rukshana, et al. "Enhancement of superconducting critical current density by Fe impurity substitution in NbSe 2 single crystals and the vortex pinning mechanism." Physical Chemistry Chemical Physics 19.18 (2017): 11230-11238.

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[34] Pervin, Rukshana, et al. "Study of transport properties in Se-deficient and Fe-intercalated NbSe2 single crystals: experiment and theory." Journal of Materials Science 55.1 (2020): 250-262.

[35] Naik, Subham, et al. "The effect of Sn intercalation on the superconducting properties of 2HNbSe2." Physica C: Superconductivity and its applications 561 (2019): 18-23.

[36] Krishnan, Manikandan, et al. "Pressure assisted enhancement in superconducting properties of Fe substituted NbSe2 single crystal." Scientific REPORtS 8.1 (2018): 1251.

[37] Pervin, Rukshana. "Single crystals growth and physical properties characterization of NbSe2 superconductor." (2020).

[38] Leijnse, Martin, and Karsten Flensberg. "Introduction to topological superconductivity and Majorana fermions." Semiconductor Science and Technology 27.12 (2012): 124003.

[39] Sato, Masatoshi, and Yoichi Ando. "Topological superconductors: a review." Reports on Progress in Physics 80.7 (2017): 076501.

[40] Naik, I., and A. K. Rastogi. "Charge density wave and superconductivity in 2H-and 4H-NbSe2: A revisit." Pramana 76.6 (2011): 957-963.

[41] Arumugam, S., et al. "Enhancement of superconducting properties and flux pinning mechanism on Cr0. 0005NbSe2 single crystal under Hydrostatic pressure." Scientific Reports 9.1 (2019): 347.

[42] Strnad, A. R., C. F. Hempstead, and Y. B. Kim. "Dissipative mechanism in type-II superconductors." Physical Review Letters 13.26 (1964): 794.

[43] Matsushita, T., and B. Ni. "Fluxoid motion and resistive transition in high Tc superconductors." Cryogenics 30.7 (1990): 614-617.

[44] Kim, Y. B., C. F. Hempstead, and A. R. Strnad. "Flux-flow resistance in type-II superconductors." Physical Review 139.4A (1965): A1163.

[45] Sanchez, David, et al. "Specific heat of 2H-NbSe2 in high magnetic fields." Physica B: Condensed Matter 204.1-4 (1995): 167-175.

[46] Toyota, Naoki, et al. "Temperature and angular dependences of upper critical fields for the layer structure superconductor 2H-NbSe 2." Journal of Low Temperature Physics 25 (1976): 485-499.

[47] Pervin, Rukshana, et al. "Study of transport properties in Se-deficient and Fe-intercalated NbSe2 single crystals: experiment and theory." Journal of Materials Science 55.1 (2020): 250-262.

[48] Shen, Dong, et al. "Two-dimensional superconductivity and magnetotransport from topological surface states in AuSn4 semimetal." Communications Materials 1.1 (2020): 56.

[49] Zhao, Jia-Ming, and Zhi-He Wang. "Anisotropic superconducting properties of FeSe0. 5Te0. 5 single crystals." Chinese Physics B 31.9 (2022): 097402.

[50] Khan, Masood Rauf, et al. "Effective Magnetic Field Dependence of the Flux Pinning Energy in FeSe0. 5Te0. 5 Superconductor." Materials 14.18 (2021): 5289.

[51] Li, Lin-jun, et al. "The effect of a charge-density wave transition on the transport properties of 2H-NbSe2." Journal of Physics: Condensed Matter 17.3 (2005): 493.

[52] Li, Linjun, et al. "MAGNETORESISTANCE AND HALL EFFECT OF TWO-DIMENSIONAL 2 H-NbSe 2." International Journal of Modern Physics B 19.01n03 (2005): 275-279.

[53] Reyren, Nicolas, et al. "Superconducting interfaces between insulating oxides." Science 317.5842 (2007): 1196-1199.

[54] Straub, Th, et al. "On the Peierls transition in 2H–NbSe2." Physica B: Condensed Matter 259 (1999): 981-982.

[55] https://ebrary.net/158504/mathematics/classical_hall_effect
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dc.identifier.urihttp://tdr.lib.ntu.edu.tw/jspui/handle/123456789/88716-
dc.description.abstract本研究首先對於化學氣相傳導法(Chemical Vapor Transport, CVT)成長的單晶樣品,經過Se元素補充後尋求改善超導特性之最佳熱處理條件,發現在固定壓力6000 atm下使用了不同的退火溫度400 °C、500 °C、600 °C以及800 °C的最佳化退火溫度為600 °C。我們便進行對加壓前和加壓後的樣品進行電性的量測以及分析,以找出加壓退火後對超導特性的影響。透過R-T得到加壓熱處理前後的Tc,分別為Tc=6.45 K以及Tc=7.14 K,之後便經由R-T的量測得出Hc2,ab(0)在加壓熱處理前後為12.45 T和14.34 T,Hc2,c(0)在加壓熱處理前後分別為4.16 T和6.36 T,發現Hc2,ab>>Hc2,c跟Ising超導的性質符合,相干長度\xi_c分別為2.97 nm和3.33 nm、\xi_{ab}分別為8.9 nm和6.62 nm,∆Tc(Tconset-Tc(ρ=0))分別為0.44 K和0.17 K、RRR(R_{300\ K}/R_{T_c})分別為8和16.5,從U-H 分析兩樣品在磁通蠕動模型下的釘扎能,得出加壓熱處理後的樣品在兩方向上都比較大,I-V量測下的BKT相變在加磁場前後比較,判斷出具有二維特性,MR量測以及霍爾和載子濃度的量測下分析得下得出RRR(R_{300\ K}/R_{T_c})值對於磁阻為正相關,以及傳輸載子的轉變發生的更明顯,從在ab方向Hc3和Hc2的比較下發現大小差異不大,加壓後的僅在5 K時有Hc3=1.173 Hc2小於傳統理論Hc3=1.69 Hc2顯示出Ising超導的抑制。zh_TW
dc.description.abstractIn this study, we aimed to improve the superconducting properties of single-crystal samples grown using the Chemical Vapor Transport (CVT) method by supplementing Se elements and optimizing the annealing conditions. After conducting experiments at a fixed pressure of 6000 atm and different annealing temperatures 400 °C, 500 °C, 600 °C, and 800 °C, we found that the optimal annealing temperature for enhancing superconducting properties was 600 °C.
We performed electrical measurements and analysis on the samples before and after pressurization to investigate the effects of pressurized annealing on superconducting characteristics. Through resistance-temperature (R-T) measurements, we determined the critical temperatures to be Tc=6.45 K before pressurization and Tc=7.14 K after pressurized annealing. Furthermore, the upper critical fields, Hc2,ab(0), were 12.45 T and 14.34 T, and Hc2,c(0) were 4.16 T and 6.36 T before and after pressurized annealing, respectively. We observed that Hc2,ab was significantly greater than Hc2,c, consistent with the properties of Ising superconductors.
The coherence lengths, \xi_c and \xi_{ab}, were determined to be 2.97 nm and 3.33 nm, and 8.9 nm and 6.62 nm before and after pressurization, respectively. The difference in transition width, ∆Tc(Tconset-Tc(ρ=0)), was 0.44 K and 0.17 K, and the residual resistance ratios RRR(R_{300\ K}/R_{T_c}) were 8 and 16.5 before and after pressurized annealing.
Using the U-H analysis, we found that the pressurized annealing resulted in higher pinning energies in both directions. Through I-V measurements, we compared the BKT transition before and after applying a magnetic field and determined that the samples exhibited 2D characteristics. Analyzing magnetoresistance and Hall measurements revealed a positive correlation between RRR values and magnetoresistance, indicating a more evident transition of transport carriers.
By comparing Hc3 and Hc2 values in the ab direction, we observed that there was not a significant difference in magnitude. However, after pressurization, at 5 K, Hc3=1.173 Hc2, which was lower than the traditional theoretical value of Hc3=1.69 Hc2, suggesting the suppression from Ising superconductivity.
en
dc.description.provenanceSubmitted by admin ntu (admin@lib.ntu.edu.tw) on 2023-08-15T17:29:24Z
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dc.description.provenanceMade available in DSpace on 2023-08-15T17:29:24Z (GMT). No. of bitstreams: 0en
dc.description.tableofcontents致謝 i
摘要 ii
Abstract iii
圖目錄 viii
表目錄 xii
第一章緒論 1
1-1超導簡介 1
1-2 Ising超導 3
1-3 NbSe2文獻回顧 3
1-4 研究動機 11
第二章 理論背景與原理簡介 12
2-1 超導體特性 12
2-1-1零電阻 12
2-1-2 邁斯納效應(Meissner Effect, Perfect Diamagnetism) 13
2-1-3 倫敦穿透深度(London penetration depth) 14
2-1-4 二流體模型(two-fluid model) 16
2-1-5 吉因茨堡-朗道理論(Ginzburg-Landau,簡稱G-L 理論) 17
2-1-6 I類和II類超導體 20
2-1-7 磁通渦流 22
2-1-8 相干長度 (coherence length) 24
2-1-9 Anderson-Kim 磁通蠕動模型 24
2-1-10 Hc3 (表面超導態的臨界磁場) 26
2-2 BKT相變(Berezinskii-Kosterlitz-Thouless相變) 28
2-3 磁阻 Magnetoresistance (MR) 28
2-4 Kohler’s rule 30
2-5 霍爾效應 31
第三章 實驗方法 33
3-1 實驗流程 33
3-1-1 NbSe2樣品合成 34
3-1-2初步判斷NbSe2性質 35
3-1-3 NbSe2樣品的加壓退火再製備 35
3-2量測系統 40
3-2-1 X光繞射儀(X-ray Diffractometer, XRD) 40
3-2-2 SQUID量測系統 41
第四章實驗結果與討論 44
4-1初步判斷NbSe2性質XRD、M-T結果 44
4-2 NbSe2補Se退火XRD、M-T結果 45
4-3 NbSe2補Se退火及加壓後的XRD、M-T結果 47
4-4 退火溫度Tann對超導特性的影響 50
4-5 電阻率、上臨界磁場與釘扎能分析 52
4-5-1 電阻率與溫度變化圖 52
4-5-2 上臨界磁場、相干長度與溫度關係圖 58
4-5-3 釘扎能分析 64
4-6 MR及霍爾分析 69
4-6-1 磁阻( MR )分析 69
4-6-2 霍爾及載子濃度分析 72
4-7 BKT 相變、Hc3分析 74
4-7-1 BKT 相變 74
4-7-2 Hc3分析 78
第五章 結論 81
Reference 83
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dc.language.isozh_TW-
dc.subject二維材料zh_TW
dc.subjectHc3zh_TW
dc.subjectBKT 相變zh_TW
dc.subject釘扎效應zh_TW
dc.subjectIsing超導zh_TW
dc.subjectNbSe2zh_TW
dc.subject第二類超導zh_TW
dc.subjectType-II superconductorsen
dc.subjectHc3en
dc.subjectPinning effecten
dc.subjectBKT transitionen
dc.subjectNbSe2en
dc.subjectIsing Superconductivityen
dc.subjectTwo-dimensional materialsen
dc.title加壓熱處理下二硒化鈮單晶的超導特性之研究zh_TW
dc.titleSuperconducting Properties of NbSe2 with heat treatment under pressureen
dc.typeThesis-
dc.date.schoolyear111-2-
dc.description.degree碩士-
dc.contributor.oralexamcommittee尤孝雯;陳昭翰;廖書賢zh_TW
dc.contributor.oralexamcommitteeHsiao-Wen Yu;Jau-Han Chen;Shu-Hsien Liaoen
dc.subject.keyword二維材料,第二類超導,NbSe2,Ising超導,釘扎效應,BKT 相變,Hc3,zh_TW
dc.subject.keywordTwo-dimensional materials,Type-II superconductors,NbSe2,Ising Superconductivity,Pinning effect,BKT transition,Hc3,en
dc.relation.page88-
dc.identifier.doi10.6342/NTU202302431-
dc.rights.note同意授權(限校園內公開)-
dc.date.accepted2023-08-08-
dc.contributor.author-college理學院-
dc.contributor.author-dept物理學系-
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