中文版 | English
题名

FeTe-SrTiO3 异质结的光电性能研究

其他题名
STUDY ON PHOTOELECTRONIC PROPERTIES OF FeTe-SrTiO3 HETEROJUNCTION
姓名
姓名拼音
WANG Haochen
学号
12132942
学位类型
硕士
学位专业
0856 材料与化工
学科门类/专业学位类别
0856 材料与化工
导师
王干
导师单位
物理系
论文答辩日期
2023-09-19
论文提交日期
2023-12-26
学位授予单位
南方科技大学
学位授予地点
深圳
摘要

  半导体产业是我国当下的产业升级规划中至关重要的一环,其中光电二极管是半导体领域中关系到国防、医疗、工业自动控制以及光电计量等行业的重要组成部件。相比于传统p-n结二极管,基于二维范德华异质结的肖特基光电二极管具有快速响应、高探测率等优点,具备广阔的研究前景。过去的研究中肖特基探测器往往受制于表面态、悬挂键等因素而具备较大的反向漏电流,而无法实现高信噪比探测,因此开发具有良好二维特性的肖特基二极管很有必要。

  本文主要基于分子束外延技术,制备高质量外延FeTe薄膜,探究FeTe薄膜的厚度与外延衬底(SrTiO3)掺杂浓度两大因素对异质结光电效应的影响,寻求优化该异质结光电效应的方向。实验结果表明,在一定范围内FeTe薄膜的厚度对于入射光的吸收影响不大,当FeTe厚度小于15 nm时,入射光都可以照射到异质结区域,器件可以在一到几个原子层内具备良好的二维特性。在探究半导体衬底的掺杂浓度对光电效应的影响时发现,掺杂浓度变大时,器件的光谱吸收边会红移,低掺杂浓度(0.05%)的衬底外延的器件具备短波和长波两个区域的吸收边。测试FeTe薄膜的紫外光电子能谱时发现其功函数相比前人的研究结果偏大,达到4.9 eV,但可以与外延衬底形成良好的肖特基接触。在一定波长入射光照射下,低掺杂浓度的衬底外延的FeTe薄膜形成的异质结相比高掺杂浓度的衬底(0.5%0.7%)外延的异质结具备更稳定的光电流,且响应度更显著,达到了1.8×10-2 A/W,表明衬底的掺杂浓度对于器件的光电效应有影响。

     本文通过对FeTe薄膜与衬底SrTiO3形成的异质结的光电效应的研究探索了优化该异质结光电性能的方向,并且实现了对单层FeTe薄膜异质结的光电流探测,确认了其具备肖特基探测器应用潜力,为该器件在光电探测领域的研究奠定了基础。

关键词
语种
中文
培养类别
独立培养
入学年份
2021
学位授予年份
2023-12
参考文献列表

[1]尚慧明, 戴明金, 高峰, 等. 无机紫外光电探测器材料研究进展[J]. 中国材料进展, 2019, 38(09): 875-886.
[2]ROCCAFORTE F, FIORENZA P, GRECO G, et al. Emerging trends in wide band gap semiconductors technology for power devices[J]. Microelectronic Engineering, 2018, 187-188(FEB.):66-77.
[3]SUN M, ZHANG Y, GAO X, et al. High-Performance GaN Vertical Fin Power Transistors on Bulk GaN Substrates[J]. IEEE Electron Device Letters, 2017, 38(4): 509-512.
[4]IKEDA N, NIIYAMA Y, KAMBAYASHI H, et al. GaN Power Transistors on Si Substrates for Switching Applications[J]. Proceedings of the IEEE, 2010, 98(7): 1151-1161.
[5]CASADY J B, JOHNSON R W. Status of Silicon Carbide as a Wide-Bandgap Semiconductor for High-Temperature Applications: A review[J]. Solid State Electronics, 1996, 39(10): 1409-1422.
[6]赵庆添, 杨连生, 耿秀珍. 半导体光电探测器件光谱响应和响应度的测试[J]. 半导体光电, 1980(4): 35-39.
[7]李雨轩. 新型锗硅光电探测器的研制[D]. 吉林:吉林大学,2022.
[8]吕磊. 高性能有机光电探测器的制备与研究[D]. 中国科学院大学,2020.
[9]王颖华. p型透明导电薄膜及其二极管的研究[D]. 上海:复旦大学,2008.
[10]WANG Y, LI J, D. VIEHLAND. Magneto electrics for magnetic sensor applications: status, challenges and perspectives[J]. Mater. Today, 17 (2014) 269–275.
[11]Q XU. A wind vector detecting system based on triboelectric and photoelectric sensors for simultaneously monitoring wind speed and direction[J]. Nano Energy 89 (2021), 106382.
[12]A Mondal, P Yadav, Y. A. Reddy. A review on device architecture engineering on various 2-D materials toward high-performance photodetectors[J]. Mater. Today Communications, Volume 34,2023,105094,ISSN 2352-4928.
[13]LI L. Ultrahigh-Performance Solar-Blind Photodetectors Based on individual single-crystalline In₂Ge₂O₇ nanobelts[J]. Adv Mater. 2010 Dec 1;22(45):5145-9.
[14]P V K. YADAV, B AJITHA, Y A K. REDDY, et al. Enhanced performance of WO3 photodetectors through hybrid graphene-layer integration[J]. ACS Appl. Electron. Mater. 3 (2021) 2056–2066.
[15]P V K. YADAV, B AJITHA, Y A K. REDDY, et al. Recent advances in development of nanostructured photodetectors from ultraviolet to infrared region: a review[J]. Chemosphere 279 (2021), 130473.
[16]K. S. NOVOSELOVET et al. 2D materials and van der Waals heterostructures[J]. Science. 353, aac9439(2016).
[17]SHI L. Status and outlook of metal–inorganic semiconductor–metal photodetectors[J]. Laser Photonics Rev. 15 (2021), 2000401.
[18]RICHARD O. OCAYA, YUSUF ORMAN, ABDULLAH, et al. Bias and illumination-dependent room temperature negative differential conductance in Ni-doped ZnO/p-Si Schottky photodiodes for quantum optics applications[J]. Heliyon, Volume 9, Issue 5, 2023, e16269, ISSN 2405-8440.
[19]C PARK,Y SEO,J JUNG,et al. Electrode-dependent electrical properties of metal/Nb-doped SrTiO3 junctions[J]. Applied Physics, 103 054106. (2008)
[20]U Y WON, B.H. LEE, Y.R. KIM, et al. Efficient photovoltaic effect in graphene/h-BN/silicon heterostructure self-powered photodetector[J]. Nano Res. 14 (2021) 1967–1972.
[21]HU W J,WANG Z,YU W,et al. Optically controlled electroresistance and electrically controlled photovoltage in ferroelectric tunnel junctions[J]. Nature Communications,7. (2016)
[22]ZHANG X, LIU B, GAO L et al. Near-ideal van der Waals rectifiers based on all-two-dimensional Schottky junctions. Nat Commun 12, 1522 (2021).
[23]CHEN Y, WANG Y, WANG Z. et al. Unipolar barrier photodetectors based on van der Waals heterostructures[J]. Nat Electron 4, 357–363 (2021).
[24]LONG M, LIU E, WANG P, et al. Broadband Photovoltaic Detectors Based on an Atomically Thin Heterostructure. Nano Lett. 2016 Apr 13;16(4):2254-9.
[25]YU C Y, HUANG Z W, LIN G Y, et al. High-specific-detectivity, low-dark-current Ge nanowire metal–semiconductor–metal photodetectors fabricated by Ge condensation method[J]. Phys. D 53 125103
[26]K HAYATO, T HIDEKAZU, TOMOJI. Anomalous Photoconductivity in SrTiO3[J]. Japanese Journal of Applied Physics, 39, 2657. (2000)
[27]A ALLAIN, J KANG, K BANERJEE. Electrical contacts to two-dimensional semiconductors[J]. Nat. Mater. 14 (2015) 1195–1205.
[28]J KANG, D SARKAR, Y KHATAMI et al. Proposal for all-graphene monolithic logic circuits[J]. Appl. Phys. Lett. 103 (2013) 083113.
[29]R J NELMES, G M MEYER, J HUTTON. Thermal motion in SrTiO3 at room temperature: Anharmonic or disordered[J]. Ferroelectrics 21 (1978) 461–462.
[30]PISKUNOV S, HEIFETS E, EGLITIS R I, et al. Bulk properties and electronic structure of SrTiO3, BaTiO3, PbTiO3 perovskites: an ab initio HF/DFT study[J]. Computational Materials Science, 2004, 29(2): 165-178
[31]Y J CHANG, S H PHARK. Initial stages of nickel oxide growth on Ag (001) by pulsed laser deposition[J]. Appl. Phys. 17 (2017) 640–656.
[32]R J NELMES, G M MEYER, J HUTTON. Thermal motion in SrTiO3 at room temperature: Anharmonic or disordered[J]. Ferroelectrics 21 (1978) 461–462.
[33]T OKUDA, K NAKANISHI, S MIYASAKA, et al. Large thermoelectric response of metallic perovskites: Sr1−xLaxTiO3(0[34]M GUENNOU, P BOUVIER, J KREISEL, et al. Pressure-temperature phase diagram of SrTiO3 up to 53 GPa[J]. Phys. Rev. B 81 (2010), 054115.
[35]D A MULLER, N NAKAGAWA, A OHTOMO, et al. Atomic-scale imaging of nanoengineered oxygen vacancy profiles in SrTiO3[J]. Nature 430 (2004) 657–661.
[36]H OHTA. Thermoelectrics based on strontium titanate[J]. Mater. Today 10 (2007) 44–49.
[37]K LAAJALEHTO. XPS study of clean metal sulfide surfaces[J]. Appl. Surf. Sci. 81 (1994) 11–15.
[38]KOMA A. Van der Waals epitaxy—a new epitaxial growth method for a highly lattice-mismatched system[J]. Thin Solid Films, 1992, 216(1): 72-76.
[39]TANG C, LIU C, ZHOU G, et al. Interface enhanced electron–phonon coupling and high temperature superconductivity in potassium-coated ultra-thin FeSe films on SrTiO3[J]. Phys Rev B 93:020507 (2016)
[40]ZHANG Y, LEE JJ, MOORE RG, et al. Superconducting gapanisotropy in monolayer FeSe thin film[J]. ArXiv:1512.06322 (2015)
[41]郭斌. Bi2Te3/FeTe异质结的超导性质研究[D]. 黑龙江:哈尔滨工业大学,2019.
[42]J LANGEVOORT. On the oxide formation on stainless steels AISI 304 and incoloy 800H investigated with XPS[J]. Appl. Surf. Sci. 28 (1987) 167–179.
[43]L SORIANO. An XPS study of Cs2Te photocathode materials[J]. Surf. Interface Anal. 16 (1990) 193–198.
[44]WANG XINGGUO, BIAN CE, HE YIXIANG, at al. Ultrathin FeTe nanosheets with tetragonal and hexagonal phases synthesized by chemical vapor deposition,Materials Today[J]. Volume 45,2021, Pages 35-43, ISSN 1369-7021.
[45]LI JIAN, HUANG GUIQIN, ZHU XINGFENG. Whether FeTe is superconductor: Insights from first-principles calculations[J]. Physica C: Superconductivity,Volume 492,2013,Pages 152-157, ISSN 0921-4534.
[46]HAN ZHI QING et al. High-Quality FeTe1−xSex Monolayer Films on SrTiO3(001) Substrates Grown by Molecular Beam Epitaxy[J]. 2017 Chinese Phys. Lett. 34 107401
[47]SHYU K W. Method for forming compound epitaxial layer by chemical bonding and epitaxy product made by the same method[M]. 2014.
[48]CHAMBERS A. Modern vacuum physics[M]. CRC Press, 2004.
[49]KAREN JOHNSTON, MARTIN R CASTELL, First-principles calculations of surface energy and atomic structure compared with scanning tunneling microscopy images[J]. Phys. Rev. B 70, 085415 – Published 26 August 2004
[50]CHO A Y. Morphology of epitaxial growth of GaAs by a molecular beam method: The observation of surface structures[J]. Journal of Applied Physics, 1970, 41(7): 2780-2786.
[51]ZHANG Z, LAGALLY M G. Atomic-scale mechanisms for surfactant-mediated layerby-layer growth in homoepitaxy[J]. Physical review letters, 1994, 72(5): 693.
[52]BRAUN W, SHAYDUK R, FLISSIKOWSKI T, et al. Epitaxy of Ge–Sb–Te phase-change memory alloys[J]. Applied Physics Letters, 2009, 94(4): 041902.
[53]BRAUN W. Applied RHEED: reflection high-energy electron diffraction during crystal growth[M]. Springer Science & Business Media, 1999
[54]H NOHIRA, et al. Characterization of ALCVD-Al2O3 and ZrO2 layer using X-ray photoelectron spectroscopy[J]. Non-Crystalline Solids 303 (2002) 83–87.
[55]MC BIESINGER, et al. Resolving surface chemical states in XPS analysis of first row transition metals, oxides and hydroxides: Cr, Mn, Fe, Co and Ni[J]. Applied Surface Science 257 (2011) 2717-2730.ZHANG H, ZHANG D, LU X, et al. Origin of charge transfer and enhanced electron–phonon coupling in single unit-cell FeSe films on SrTiO3[J]. Nat Commun 8, 214 (2017).

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材料与化工
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王昊琛. FeTe-SrTiO3 异质结的光电性能研究[D]. 深圳. 南方科技大学,2023.
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