Skip navigation

DSpace

機構典藏 DSpace 系統致力於保存各式數位資料(如:文字、圖片、PDF)並使其易於取用。

點此認識 DSpace
DSpace logo
English
中文
  • 瀏覽論文
    • 校院系所
    • 出版年
    • 作者
    • 標題
    • 關鍵字
    • 指導教授
  • 搜尋 TDR
  • 授權 Q&A
    • 我的頁面
    • 接受 E-mail 通知
    • 編輯個人資料
  1. NTU Theses and Dissertations Repository
  2. 理學院
  3. 應用物理研究所
請用此 Handle URI 來引用此文件: http://tdr.lib.ntu.edu.tw/jspui/handle/123456789/103708
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-Ming Wangen
dc.contributor.author徐辰硯zh_TW
dc.contributor.authorChen-Yen Hsuen
dc.date.accessioned2026-08-19T16:10:18Z-
dc.date.available2026-08-20-
dc.date.copyright2026-08-19-
dc.date.issued2026-
dc.date.submitted2026-08-10 17:05:40-
dc.identifier.citation[1] D. Van Delft and P. Kes, “The discovery of superconductivity,” Phys. Today, vol. 63, no. 9, pp. 38–43, Sep. 2010, doi: 10.1063/1.3490499.
[2] D. Goodstein and J. Goodstein, “Richard Feynman and the History of Superconductivity,” Phys. Perspect., vol. 2, no. 1, pp. 30–47, Mar. 2000, doi: 10.1007/s000160050035.
[3] J. E. Hirsch, “The Meissner effect in superconductors: emergence versus reductionism,” J. Phys. Condens. Matter, vol. 38, no. 7, p. 073001, Feb. 2026, doi: 10.1088/1361-648X/ae3cf2.
[4] J. Bardeen, L. N. Cooper, and J. R. Schrieffer, “Theory of Superconductivity,” Phys. Rev., vol. 108, no. 5, pp. 1175–1204, Dec. 1957, doi: 10.1103/PhysRev.108.1175.
[5] “ON THE THEORY OF SUPERCONDUCTIVITY,” in Collected Papers of L.D. Landau, Elsevier, 1965, pp. 546–568. doi: 10.1016/B978-0-08-010586-4.50078-X.
[6] G. I. González-Pedreros, J. A. Camargo-Martínez, and F. Mesa, “Cooper Pairs Distribution function for bcc Niobium under pressure from first-principles,” Sci. Rep., vol. 11, no. 1, p. 7646, Apr. 2021, doi: 10.1038/s41598-021-87028-x.
[7] D. Möckli and M. K. D. Azambuja, “Magnetic superconductivity,” Rev. Bras. Ensino Física, vol. 46, no. suppl 1, p. e20240094, 2024, doi: 10.1590/1806-9126-rbef-2024-0094.
[8] G. I. González-Pedreros, J. A. Camargo-Martínez, and F. Mesa, “Cooper Pairs Distribution function for bcc Niobium under pressure from first-principles,” Sci. Rep., vol. 11, no. 1, p. 7646, Apr. 2021, doi: 10.1038/s41598-021-87028-x.
[9] N. Schwartz, M. Gresh, and S. Karlik, “Niobium Solid Electrolytic Capacitors,” J. Electrochem. Soc., vol. 108, no. 8, p. 750, 1961, doi: 10.1149/1.2428210.
[10] M. Z. Hasan and C. L. Kane, “Colloquium : Topological insulators,” Rev. Mod. Phys., vol. 82, no. 4, pp. 3045–3067, Nov. 2010, doi: 10.1103/RevModPhys.82.3045.
[11] M. König et al., “Quantum Spin Hall Insulator State in HgTe Quantum Wells,” Science, vol. 318, no. 5851, pp. 766–770, Nov. 2007, doi: 10.1126/science.1148047.
[12] D. Hsieh et al., “A topological Dirac insulator in a quantum spin Hall phase,” Nature, vol. 452, no. 7190, pp. 970–974, Apr. 2008, doi: 10.1038/nature06843.
[13] H. Zhang, C.-X. Liu, X.-L. Qi, X. Dai, Z. Fang, and S.-C. Zhang, “Topological insulators in Bi2Se3, Bi2Te3 and Sb2Te3 with a single Dirac cone on the surface,” Nat. Phys., vol. 5, no. 6, pp. 438–442, Jun. 2009, doi: 10.1038/nphys1270.
[14] D. Mondal, A. Bandyopadhyay, and D. Jana, “Su-Schrieffer-Heeger Model - From Fundamentals to Responses,” Int. J. Theor. Phys., vol. 64, no. 5, p. 125, Apr. 2025, doi: 10.1007/s10773-025-05981-z.
[15] X. Zhang et al., “Investigation on the electrical transport properties of highly (00l)-textured Sb2Te3 films deposited by molecular beam epitaxy,” J. Appl. Phys., vol. 115, no. 2, p. 024307, Jan. 2014, doi: 10.1063/1.4861394.
[16] Shama, R. K. Gopal, G. Sheet, and Y. Singh, “2D weak anti-localization in thin films of the topological semimetal Pd$$_{3}$$Bi$$_{2}$$S$$_{2}$$,” Sci. Rep., vol. 11, no. 1, p. 12618, Jun. 2021, doi: 10.1038/s41598-021-91930-9.
[17] S. Hikami, A. I. Larkin, and Y. Nagaoka, “Spin-Orbit Interaction and Magnetoresistance in the Two Dimensional Random System,” Prog. Theor. Phys., vol. 63, no. 2, pp. 707–710, Feb. 1980, doi: 10.1143/PTP.63.707.
[18] L. Fu and C. L. Kane, “Superconducting Proximity Effect and Majorana Fermions at the Surface of a Topological Insulator,” Phys. Rev. Lett., vol. 100, no. 9, p. 096407, Mar. 2008, doi: 10.1103/PhysRevLett.100.096407.
[19] W. Meissner and R. Ochsenfeld, “Ein neuer Effekt bei Eintritt der Supraleitf�higkeit,” Naturwissenschaften, vol. 21, no. 44, pp. 787–788, Nov. 1933, doi: 10.1007/BF01504252.
[20] F. London and H. London, “The electromagnetic equations of the supraconductor,” Proc. R. Soc. Lond. Ser. - Math. Phys. Sci., vol. 149, no. 866, pp. 71–88, Mar. 1935, doi: 10.1098/rspa.1935.0048.
[21] Y. Zhang et al., “High-temperature superconductivity with zero resistance and strange-metal behaviour in La3Ni2O7−δ,” Nat. Phys., vol. 20, no. 8, pp. 1269–1273, Aug. 2024, doi: 10.1038/s41567-024-02515-y.
[22] L. D. Landau, “ON THE THEORY OF SUPERCONDUCTIVITY,” in Collected Papers of L.D. Landau, Elsevier, 1965, pp. 546–568. doi: 10.1016/B978-0-08-010586-4.50078-X.
[23] A. A. Abrikosov, “The magnetic properties of superconducting alloys,” J. Phys. Chem. Solids, vol. 2, no. 3, pp. 199–208, Jan. 1957, doi: 10.1016/0022-3697(57)90083-5.
[24] J. M. Lock, “Critical Currents in Superconductors,” Phys. Bull., vol. 24, no. 10, pp. 620–620, Oct. 1973, doi: 10.1088/0031-9112/24/10/041.
[25] C. P. Bean, “Magnetization of High-Field Superconductors,” Rev. Mod. Phys., vol. 36, no. 1, pp. 31–39, Jan. 1964, doi: 10.1103/RevModPhys.36.31.
[26] G. Blatter, M. V. Feigel’man, V. B. Geshkenbein, A. I. Larkin, and V. M. Vinokur, “Vortices in high-temperature superconductors,” Rev. Mod. Phys., vol. 66, no. 4, pp. 1125–1388, Oct. 1994, doi: 10.1103/RevModPhys.66.1125.
[27] D. Dew-Hughes, “Flux pinning mechanisms in type II superconductors,” Philos. Mag. J. Theor. Exp. Appl. Phys., vol. 30, no. 2, pp. 293–305, Aug. 1974, doi: 10.1080/14786439808206556.
[28] M. Tinkham, Introduction to superconductivity, 2 ed. in Dover books on physics. Mineola, NY: Dover Publ, 2015.
[29] R. Flükiger, “Overview of Superconductivity and Challenges in Applications,” Rev. Accel. Sci. Technol., vol. 05, pp. 1–23, Jan. 2012, doi: 10.1142/S1793626812300010.
[30] A. B. Pippard and W. L. Bragg, “An experimental and theoretical study of the relation between magnetic field and current in a superconductor,” Proc. R. Soc. Lond. Ser. Math. Phys. Sci., vol. 216, no. 1127, pp. 547–568, Feb. 1953, doi: 10.1098/rspa.1953.0040.
[31] A. B. Pippard, “The surface impedance of superconductors and normal metals at high frequencies II. The anomalous skin effect in normal metals,” Proc. R. Soc. Lond. Ser. Math. Phys. Sci., vol. 191, no. 1026, pp. 385–399, Nov. 1947, doi: 10.1098/rspa.1947.0122.
[32] J. Bardeen, L. N. Cooper, and J. R. Schrieffer, “Theory of Superconductivity,” Phys. Rev., vol. 108, no. 5, pp. 1175–1204, Dec. 1957, doi: 10.1103/PhysRev.108.1175.
[33] A. A. Abrikosov, “On the Magnetic Properties of Superconductors of the Second Group,” Sov Phys JETP, vol. 5, pp. 1174–1182, 1957.
[34] A. I. Larkin and Yu. N. Ovchinnikov, “Pinning in type II superconductors,” J. Low Temp. Phys., vol. 34, no. 3–4, pp. 409–428, Feb. 1979, doi: 10.1007/BF00117160.
[35] P. W. Anderson and Y. B. Kim, “Hard Superconductivity: Theory of the Motion of Abrikosov Flux Lines,” Rev. Mod. Phys., vol. 36, no. 1, pp. 39–43, Jan. 1964, doi: 10.1103/RevModPhys.36.39.
[36] C. P. Bean, “Magnetization of Hard Superconductors,” Phys. Rev. Lett., vol. 8, no. 6, pp. 250–253, Mar. 1962, doi: 10.1103/PhysRevLett.8.250.
[37] E. Zeldov et al., “Geometrical Barriers in High-Temperature Superconductors,” Phys. Rev. Lett., vol. 73, no. 10, pp. 1428–1431, Sep. 1994, doi: 10.1103/PhysRevLett.73.1428.
[38] E. H. Brandt, “Irreversible magnetization of pin-free type-II superconductors,” Phys. Rev. B, vol. 60, no. 17, pp. 11939–11942, Nov. 1999, doi: 10.1103/PhysRevB.60.11939.
[39] D. M. Gokhfeld, “Secondary Peak on Asymmetric Magnetization Loop of Type-II Superconductors,” J. Supercond. Nov. Magn., vol. 26, no. 2, pp. 281–283, Feb. 2013, doi: 10.1007/s10948-012-1741-8.
[40] T. H. Johansen, M. R. Koblischka, H. Bratsberg, and P. O. Hetland, “Critical-state model with a secondary high-field peak in J c ( B ),” Phys. Rev. B, vol. 56, no. 17, pp. 11273–11278, Nov. 1997, doi: 10.1103/PhysRevB.56.11273.
[41] W. Zhou, X. Xing, W. Wu, H. Zhao, and Z. Shi, “Second magnetization peak effect, vortex dynamics and flux pinning in 112-type superconductor Ca0.8La0.2Fe1−xCoxAs2,” Sci. Rep., vol. 6, no. 1, p. 22278, Mar. 2016, doi: 10.1038/srep22278.
[42] G. P. Mikitik and E. H. Brandt, “Peak effect, vortex-lattice melting line, and order-disorder transition in conventional and high- T c superconductors,” Phys. Rev. B, vol. 64, no. 18, p. 184514, Oct. 2001, doi: 10.1103/PhysRevB.64.184514.
[43] B. Rosenstein, B. Ya. Shapiro, I. Shapiro, Y. Bruckental, A. Shaulov, and Y. Yeshurun, “Peak effect and square-to-rhombic vortex lattice transition in La 2 − x Sr x Cu O 4,” Phys. Rev. B, vol. 72, no. 14, p. 144512, Oct. 2005, doi: 10.1103/PhysRevB.72.144512.
[44] D. Stamopoulos and M. Pissas, “Hysteretic behavior of the vortex lattice at the onset of the second peak for the HgBa 2 CuO 4 + δ superconductor,” Phys. Rev. B, vol. 65, no. 13, p. 134524, Mar. 2002, doi: 10.1103/PhysRevB.65.134524.
[45] I. M. Babich, E. H. Brandt, G. P. Mikitik, and E. Zeldov, “Critical current in type-II superconductors near the order-disorder transition,” Phys. Rev. B, vol. 81, no. 5, p. 054517, Feb. 2010, doi: 10.1103/PhysRevB.81.054517.
[46] H. M. Cole, M. B. Venuti, B. Gorman, E. D. Bauer, M. K. Chan, and S. Eley, “Plastic vortex creep and dimensional crossovers in the highly anisotropic superconductor HgBa 2 CuO 4 + x,” Phys. Rev. B, vol. 107, no. 10, p. 104509, Mar. 2023, doi: 10.1103/PhysRevB.107.104509.
[47] E. J. Patiño, M. Aprili, M. G. Blamire, and Y. Maeno, “Vortex flipping in superconductor/ferromagnet spin-valve structures,” Phys. Rev. B, vol. 87, no. 21, p. 214514, Jun. 2013, doi: 10.1103/PhysRevB.87.214514.
[48] 洪浩哲, “磊晶碲化銻薄膜之成長與超導碲化銻/鈮多層膜之電磁傳輸特性之研究,” Master’s Thesis, 國立臺灣大學, 2024. doi: 10.6342/NTU202404181.
[49] R. Sultana, G. Gurjar, S. Patnaik, and V. P. S. Awana, “Crystal growth and characterization of bulk Sb2 Te3 topological insulator,” Mater. Res. Express, vol. 5, no. 4, p. 046107, Apr. 2018, doi: 10.1088/2053-1591/aabc33.
[50] L. S. Brooks, “The Vapor Pressures of Tellurium and Selenium,” J. Am. Chem. Soc., vol. 74, no. 1, pp. 227–229, Jan. 1952, doi: 10.1021/ja01121a059.
[51] M. J. Smith, R. J. Knight, and C. W. Spencer, “Properties of Bi2Te3-Sb2Te3 Alloys,” J. Appl. Phys., vol. 33, no. 7, pp. 2186–2190, Jul. 1962, doi: 10.1063/1.1728925.
[52] M. Tan, Y. Deng, and Y. Hao, “Enhanced thermoelectric properties and layered structure of Sb2Te3 films induced by special (0 0l) crystal plane,” Chem. Phys. Lett., vol. 584, pp. 159–164, Oct. 2013, doi: 10.1016/j.cplett.2013.08.084.
[53] S. Swann, “Magnetron sputtering,” Phys. Technol., vol. 19, no. 2, pp. 67–75, Mar. 1988, doi: 10.1088/0305-4624/19/2/304.
[54] P. Gu, X. Zhu, H. Wu, and D. Yang, “Regulation of Substrate-Target Distance on the Microstructural, Optical and Electrical Properties of CdTe Films by Magnetron Sputtering,” Materials, vol. 11, no. 12, p. 2496, Dec. 2018, doi: 10.3390/ma11122496.
[55] G. Zhu, B. Xiao, G. Chen, and Z. Gan, “Study on the Deposition Uniformity of Triple-Target Magnetron Co-Sputtering System: Numerical Simulation and Experiment,” Materials, vol. 15, no. 21, p. 7770, Nov. 2022, doi: 10.3390/ma15217770.
[56] V. Strenzke et al., “Challenges and solutions in RF sputtering of superconducting Nb for nanostructuring processes,” J. Appl. Phys., vol. 136, no. 20, p. 205301, Nov. 2024, doi: 10.1063/5.0239203.
[57] T. L. Anderson and H. B. Krause, “Refinement of the Sb2 Te3 and Sb2 Te2 Se structures and their relationship to nonstoichiometric Sb2 Te 3− y Se y compounds,” Acta Crystallogr. B, vol. 30, no. 5, pp. 1307–1310, May 1974, doi: 10.1107/S0567740874004729.
[58] V. Sandu, A. M. Ionescu, G. Aldica, M. A. Grigoroscuta, M. Burdusel, and P. Badica, “On the pinning force in high density MgB2 samples,” Sci. Rep., vol. 11, no. 1, p. 5951, Mar. 2021, doi: 10.1038/s41598-021-85209-2.
[59] N. M. Hapipi et al., “Excess Mg in situ powder addition for enhancing critical current density of ex situ MgB2,” Appl. Phys. A, vol. 128, no. 10, p. 913, Oct. 2022, doi: 10.1007/s00339-022-06060-4.
[60] A. Xu et al., “Strongly enhanced vortex pinning from 4 to 77 K in magnetic fields up to 31 T in 15 mol.% Zr-added (Gd, Y)-Ba-Cu-O superconducting tapes,” APL Mater., vol. 2, no. 4, p. 046111, Apr. 2014, doi: 10.1063/1.4872060.
[61] Y. Yeshurun, A. P. Malozemoff, and A. Shaulov, “Magnetic relaxation in high-temperature superconductors,” Rev. Mod. Phys., vol. 68, no. 3, pp. 911–949, Jul. 1996, doi: 10.1103/RevModPhys.68.911.
[62] C. J. Van Der Beek et al., “Flux pinning in PrFeAsO 0.9 and NdFeAsO 0.9 F 0.1 superconducting crystals,” Phys. Rev. B, vol. 81, no. 17, p. 174517, May 2010, doi: 10.1103/PhysRevB.81.174517.
[63] M. V. Feigel’man, V. B. Geshkenbein, A. I. Larkin, and V. M. Vinokur, “Theory of collective flux creep,” Phys. Rev. Lett., vol. 63, no. 20, pp. 2303–2306, Nov. 1989, doi: 10.1103/PhysRevLett.63.2303.
[64] W. Braunisch et al., “Paramagnetic Meissner effect in Bi high-temperature superconductors,” Phys. Rev. Lett., vol. 68, no. 12, pp. 1908–1911, Mar. 1992, doi: 10.1103/PhysRevLett.68.1908.
[65] M. R. Koblischka, L. Půst, C.-S. Chang, T. Hauet, and A. Koblischka-Veneva, “The Paramagnetic Meissner Effect (PME) in Metallic Superconductors,” Metals, vol. 13, no. 6, p. 1140, Jun. 2023, doi: 10.3390/met13061140.
[66] A. E. Koshelev and A. I. Larkin, “Paramagnetic moment in field-cooled superconducting plates: Paramagnetic Meissner effect,” Phys. Rev. B, vol. 52, no. 18, pp. 13559–13562, Nov. 1995, doi: 10.1103/PhysRevB.52.13559.
[67] G. Lasher, “Series Solution of the Ginzburg-Landau Equations for the Abrikosov Mixed State,” Phys. Rev., vol. 140, no. 2A, pp. A523–A528, Oct. 1965, doi: 10.1103/PhysRev.140.A523.
[68] D. R. Strachan, M. C. Sullivan, and C. J. Lobb, “Probing the limits of superconductivity,” presented at the International Symposium on Optical Science and Technology, I. Bozovic and D. Pavuna, Eds., Seattle, WA, Nov. 2002, p. 65. doi: 10.1117/12.452479.
[69] R. Griessen et al., “Evidence for mean free path fluctuation induced pinning in YBa 2 Cu 3 O 7 and YBa 2 Cu 4 O 8 films,” Phys. Rev. Lett., vol. 72, no. 12, pp. 1910–1913, Mar. 1994, doi: 10.1103/PhysRevLett.72.1910.
[70] Q. Li, M. Suenaga, Z. Ye, S. R. Foltyn, and H. Wang, “Crossover of thickness dependence of critical current density Jc(T,H) in YBa2Cu3O7−δ thick films,” Appl. Phys. Lett., vol. 84, no. 18, pp. 3528–3530, May 2004, doi: 10.1063/1.1737067.
[71] C. Cai, B. Holzapfel, J. Hänisch, L. Fernández, and L. Schultz, “High critical current density and its field dependence in mixed rare earth (Nd,Eu,Gd)Ba2Cu3O7−δ thin films,” Appl. Phys. Lett., vol. 84, no. 3, pp. 377–379, Jan. 2004, doi: 10.1063/1.1640802.
-
dc.identifier.urihttp://tdr.lib.ntu.edu.tw/jspui/handle/123456789/103708-
dc.description.abstract本論文研究不同堆疊配置之Nb/Sb2Te3多層薄膜的磁通釘札行為與渦旋動力學,並建立一套規範化且具再現性的分析架構,由溫度與磁場相依的磁化量測中取得超導轉變溫度、特徵磁場、臨界電流密度 J_{c} 與釘札力密度 F_{p}。磁性響應呈現多重超導轉變特徵,顯示此多層薄膜無法以單一均勻的超導態描述。透過分析 J_{c}\left(H\right)、F_{p}\left(H\right)、歸一化釘札力與對數 J_{c}\left(H\right),可辨識出不同的釘札區域與類第二峰值行為,顯示渦旋響應會隨磁場及溫度演變。

最值得注意的是,當磁場平行於 ab 平面時,系統於約3 K呈現異常的低場釘札增強。排除受額外磁性訊號影響的區域後,面外方向並未重現相同的增強現象。此方向差異顯示該異常增強具有異向性,且對多層膜介面敏感,而非僅源自傳統的塊材Nb釘札。儘管僅憑磁性量測尚無法唯一判定其微觀來源,本研究結果仍為進一步探討Nb/Sb2Te3多層薄膜中受介面調控的渦旋動力學提供了實驗基礎。
zh_TW
dc.description.abstractThis thesis investigates flux pinning behavior and vortex dynamics in Nb/Sb2Te3 multilayer thin films with different multilayer configurations. A standardized and reproducible framework was established to extract superconducting transition temperatures, characteristic magnetic fields, critical current density J_{c}, and pinning-force density F_{p} from temperature- and field-dependent magnetization measurements. The magnetic responses exhibit multiple superconducting-transition features, indicating that the multilayer films cannot be described by a single homogeneous superconducting state. Analyses of J_{c}\left(H\right), F_{p}\left(H\right), normalized pinning force, and logarithmic J_{c}\left(H\right) reveal distinct pinning regimes and second-peak-like behavior, demonstrating the evolution of the vortex response with magnetic field and temperature.

Most notably, an anomalous low-field pinning enhancement appears near 3 K when the magnetic field is applied parallel to the ab plane. No comparable enhancement is reproduced in the out-of-plane configuration after excluding regions affected by additional magnetic signals. This directional contrast indicates that the anomalous enhancement is anisotropic and sensitive to the multilayer interfaces, rather than arising solely from conventional bulk Nb pinning. Although its microscopic origin cannot be uniquely determined from magnetic measurements alone, these results provide an experimental basis for investigating interface-modified vortex dynamics in Nb/Sb2Te3 multilayer thin films.
en
dc.description.provenanceSubmitted by admin ntu (admin@lib.ntu.edu.tw) on 2026-08-19T16:10:18Z
No. of bitstreams: 0
en
dc.description.provenanceMade available in DSpace on 2026-08-19T16:10:18Z (GMT). No. of bitstreams: 0en
dc.description.tableofcontentsPREFACE I
摘要 II
ABSTRACT III
CONTENTS IV
LIST OF FIGURES IX
LIST OF TABLES XIII
CHAPTER 1 INTRODUCTION 1
1.1 Superconductivity 1
1.1.1 Superconductivity 1
1.1.2 Niobium 3
1.2 Topological Insulator 4
1.2.1 Discovery of Topological Insulators 4
1.2.2 Sb2Te3 5
1.2.3 Topological Superconductor 6
1.3 Research Motivation and Objectives 6
CHAPTER 2 BACKGROUND KNOWLEDGE FOR MAGNETIC ANALYSIS 8
2.1 Magnetic Response of Superconductors 8
2.1.1 Superconducting Transition and Zero Resistance 8
2.1.2 Meissner Effect 9
2.1.3 Critical Magnetic Field 11
2.1.4 Critical Current 12
2.2 Critical Fields in Type-II Superconductors 14
2.2.1 London penetration depth 14
2.2.2 Pippard coherence length 17
2.2.3 Ginzburg–Landau Theory and Type-I/Type-II Classification 21
2.3 Vortex Matter and Irreversible Magnetization 27
2.4 Interpretation of anomalous magnetization-loop morphologies 34
2.4.1 Second Peak Effect 34
2.4.2 Abrupt low-field vortex processes 41
CHAPTER 3 EXPERIMENTAL METHODS AND DATA PROCESSING PROCEDURES 46
3.1 Chapter Overview 46
3.2 Sb2Te3 Bulk Target Preparation 47
3.2.1 Stoichiometric Calculation and Sintering Process 47
3.2.2 EDS and XRD Characterization of Sb2Te3 Bulk Crystal 50
3.2.3 Grinding and Target Compression 53
3.3 Thin Film Deposition 55
3.3.1 Sputtering System Configuration 55
3.3.2 Substrate Cleaning and Chamber Pre-conditioning 58
3.3.3 Thin Film Deposition Parameters 62
3.3.4 Deposition Rate Calibration 65
3.3.5 Multilayer Structure Design 69
3.4 Structural Characterization 71
3.4.1 X-ray Diffraction Measurement 71
3.4.2 Crystallographic Analysis 72
3.5 Definitions and Extraction Criteria of Magnetic Quantities 73
3.5.1 SQUID Output and Magnetization Conversion 73
3.5.2 Superconducting Transition Temperature Determination 74
3.5.3 Background Subtraction Procedure 76
3.5.4 Lower Critical Field Determination 77
3.5.5 Upper Critical Field Determination 79
3.5.6 Irreversibility Field Determination 80
3.6 Automated Data Analysis Workflow 81
3.6.1 Overview of the Analysis Programs 81
3.6.2 Derivative and Local-Slope Processing Module 83
3.6.3 Hc2 Extraction Module 85
3.6.4 Jc, Fp, and Hirr Processing Module 87
3.6.5 Dew-Hughes Fitting Module 93
3.6.6 Output Consistency and Workflow Limitations 96
3.7 Summary of Experimental Workflow 97
CHAPTER 4 MAGNETIC RESPONSE AND VORTEX PINNING BEHAVIOR IN NB/SB2TE3 MULTILAYERS 100
4.1 Analysis strategy and evidence chain 100
4.2 Temperature-dependent magnetization: superconducting transition and anomalous magnetic response 102
4.2.1 Superconducting quality verification of single-layer Nb film 102
4.2.2 M(T) curves of Nb/Sb2Te3 multilayer samples 105
4.3 Field-dependent magnetization from m(H)-curves: characteristic superconducting fields 108
4.3.1 Initial m(H)-curves and field-induced suppression of diamagnetism 108
4.3.2 Determination of Hc1 and Hc2 110
4.3.3 Effective coherence length, penetration depth, and GL parameter 113
4.3.4 Definition of Hg as an empirical diamagnetic maximum field 123
4.3.5 Temperature dependence of Hc1, Hg, and Hc2 126
4.4 Magnetic hysteresis and irreversible vortex response 129
4.4.1 Temperature evolution of m(H)-loops 129
4.4.2 Temperature evolution of Jc(H) 132
4.4.3 Temperature dependence of the zero-field critical current density and Griessen-type pinning analysis 134
4.4.4 Irreversibility field Hirr(T) and extended phase diagram 140
4.5 Pinning force Fp(H) and Field-dependent Pinning Regimes 142
4.5.1 Field dependence of Fp(H) and Normalized pinning force fp(h) 142
4.5.2 Dew-Hughes-type analysis of low-field and high-field regimes 145
4.6 Evidence for competing vortex-pinning regimes 150
4.6.1 Logarithmic analysis of Jc(H) 150
4.6.2 Temperature evolution of HSPE, Hcollapse, hmax,L and hmax,H 153
4.7 Field-orientation dependence of vortex pinning in the 3ML sample 162
CHAPTER 5 CONCLUSION AND FUTURE WORK 171
5.1 Conclusion 171
5.2 Future works 174
REFERENCES 176
-
dc.language.isoen-
dc.subject多層薄膜-
dc.subject拓樸超導體-
dc.subject磁通釘札-
dc.subject渦旋動力學-
dc.subject介面效應-
dc.subjectMultilayer thin films-
dc.subjecttopological superconductor-
dc.subjectflux pinning-
dc.subjectvortex dynamics-
dc.subjectinterface effects-
dc.titleNb/Sb2Te3多層薄膜中磁通釘札行為與渦旋動力學之研究zh_TW
dc.titleInvestigation of Flux Pinning Behavior and Vortex Dynamics in Nb/Sb2Te3 Multilayer Thin Filmsen
dc.typeThesis-
dc.date.schoolyear114-2-
dc.description.degree碩士-
dc.contributor.oralexamcommittee尤孝雯;陳昭翰;林晉緯zh_TW
dc.contributor.oralexamcommitteeHsiao-Wen Yu;Jau-Han Chen;Chin-Wei Linen
dc.subject.keyword多層薄膜; 拓樸超導體; 磁通釘札; 渦旋動力學; 介面效應zh_TW
dc.subject.keywordMultilayer thin films; topological superconductor; flux pinning; vortex dynamics; interface effectsen
dc.relation.page183-
dc.identifier.doi10.6342/NTU202603691-
dc.rights.note同意授權(全球公開)-
dc.date.accepted2026-08-13-
dc.contributor.author-college理學院-
dc.contributor.author-dept應用物理研究所-
dc.date.embargo-lift2026-08-20-
顯示於系所單位:應用物理研究所

文件中的檔案:
檔案 大小格式 
ntu-114-2.pdf6.12 MBAdobe PDF檢視/開啟
顯示文件簡單紀錄


系統中的文件,除了特別指名其著作權條款之外,均受到著作權保護,並且保留所有的權利。

社群連結
聯絡資訊
10617臺北市大安區羅斯福路四段1號
No.1 Sec.4, Roosevelt Rd., Taipei, Taiwan, R.O.C. 106
Tel: (02)33662353
Email: ntuetds@ntu.edu.tw
意見箱
相關連結
館藏目錄
國內圖書館整合查詢 MetaCat
臺大學術典藏 NTU Scholars
臺大圖書館數位典藏館
本站聲明
© NTU Library All Rights Reserved