研究生: |
陳柏翰 Bo-Han Chen |
---|---|
論文名稱: |
不同金屬摻雜之二硫化鉬層狀半導體之光學特性研究 The optical characterization of MoS2 layered crystals with different dopants |
指導教授: |
黃鶯聲
Ying-Sheng Huang |
口試委員: |
何清華
Ching-Hwa Ho 蔡大翔 Dah-Shyang Tsai 李奎毅 Kuei-Yi Lee 程光蛟 Kwong-Kau Tiong |
學位類別: |
碩士 Master |
系所名稱: |
電資學院 - 電子工程系 Department of Electronic and Computer Engineering |
論文出版年: | 2013 |
畢業學年度: | 101 |
語文別: | 中文 |
論文頁數: | 56 |
中文關鍵詞: | 二硫化鉬 、調製光譜 、X光繞射 、激子躍遷 、間接能隙 、光電壓量測 |
外文關鍵詞: | Modulation spectroscopy, Excitonic transition, Indirect bandgap, Photovoltage |
相關次數: | 點閱:237 下載:14 |
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本論文主要探討利用化學氣相傳導法成長層狀半導體MoS2摻雜不同過渡性金屬MoS2:X (X=Re,Nb,Fe,Co,Ni) 之相關特性。
在日本National Institute of Advanced Industrial Science, AIST Suenaga 博士研究群協助下,利用掃描式穿透式電子顯微鏡觀察錸及鐵原子在樣品中所在的位置,發現摻雜錸金屬的樣品中,錸原子會取代鉬原子;摻雜鐵的樣品中,鐵原子會聚集成團不均勻地分散在層狀單晶表面上。X光繞射分析,決定樣品主要結構,MoS2:X (X=Re,Nb) 為3R結構;而MoS2:X (X= Fe,Co,Ni) 為2H結構。
光學方面利用電解液電場調制反射光譜來決定直接能隙附近激子A與激子B之躍遷能量。在摻雜錸與鈮之樣品中,激子A與B躍遷能量之分裂量約為150 meV;在摻雜鐵、鈷及鎳之樣品中,激子A與B躍遷能量之分裂量約為200 meV,此差異主要來自於3R與2H之不同結構所致。此外利用光電壓量測技術,決定不同摻雜樣品之間接能隙、激子躍遷能量及雜質相關之吸收訊號。
Electrolyte electroreflectance (EER) and photoresponse spectroscopy in the electrolyte were used to study of doping effects of two-dimensional layered semiconductor MoS2 at room temperature. Single crystals MoS2:X with different dopants X (X=Re, Nb, Fe, Co, Ni) were grown by the chemical vapor transport method using Br2 as transport agent. The electrolytes were 0.5 M H2SO4 or 0.05 M NaI/0.002 M I2/0.05 M H2SO4.
EER measurements were carried out under low field regime. For Nb and Re doped samples only exciton A and B related features were observed. The excitonic transition energies of feature A and B were determined precisely and the splitting of excitonic transition energies for A and B were estimated to be around 150 meV. For Fe/Co/Ni doped samples, the two dominant features located at higher energy side as compared with those observed in the Nb/Re doped samples, an additional feature located below A excitonic transition feature were detected and the splitting of A and B features were estimated to be ~200 meV. The differences between these two groups of samples can be attributed to the formation of two different polytypes 3R and 2H. These results were ascertained by the X-ray diffraction patterns of the samples.
Detailed analyzing photoresponse spectra, the indirect band gap were determined, the excitonic transition energies of A and B features were estimated and the additional features due to different dopants were detected.
[1] J. A. Wilson and A. D. Yoffe, "The Transition Metal Dichalcogenides Discussion and Interpretation of the Observed Optical, Electrical and Structural Properties," Adv. Phys., vol. 18, pp. 193-212, 1969.
[2] H. Tributsch, "Layer-type Transition Metal Dichalcogenides a New Class of Electrodes for Electrochemical Solar Cells," Hauptversammiung der Deutschen Bunsen-Gesellschaft, vol. 4, pp. 361-368, 1978.
[3] R. B. Somoano and A. Rembaum, "Superconductivity in Intercalated Molybdenum Disufide," Phys. Rev. Lett., vol. 27, pp. 402-404, 1971.
[4] J. M. Martin and C. Donnet, "Superlubricity of Molybdenum Disulfide," Phys. Rev. B., vol. 48, pp. 10583-10586, 1993.
[5] C. Pina, P. Bosch, D. Acosta, J. Barreto, A. Vazquez, and E. C. Amrillo, "Growth of MoS2 and MoS2: Co Crystals using I2 as Transport Material," J. Cryst. Growth., vol. 96, pp. 685-690, 1989.
[6] E. Fortin and F. Raga, "Excitons in Molybedenum Disulfide," Phys. Rev. B., vol. 11, pp. 905-912, 1975.
[7] S. Cincotti and J. R. Rabe, "Seft-assembled Alkane Mono-layer on MoSe2 and MoS2," Appl. Phys. Lett, vol. 62, pp. 531-533, 1993.
[8] C. Hamaguchi, "Basic Semiconductor Physics," Springer-Verlag, vol. 2th, 2010.
[9] P. Bhattacharya, "Semiconductor Optoelectronic Devices," Pearson Education Taiwan, vol. 2th, 2003.
[10] A. Beiser, "Modern Physics," McGraw-Hill, vol. 6th, 2003.
[11] M. C. Ball, "chemical Transport Reaction," J. Chem. Educ., vol. 45, pp. 651-654, 1968.
[12] H. Schaufer, "Chemical transport reactions," Academic Press, Inc., 1964.
[13] D. Yang and R. F. Frindt, "Powder x-ray diffraction of two -dimensional materials," J. appl. Phys., vol. 79, pp. 2376-2385, 1996.
[14] C. H. Ho, C. S. Wu, Y. S. Huang, P. C. Liao, and K. K. Tiong, "Temperature dependence of energies and broadening parameters of the band-edge excitons of Mo1-xWxS2 single crystals," J. Phys. Condens.Matter, vol. 10, pp. 9317-9328, 1998.
[15] Y. P. Varshni, "Temperature Dependence of the Energy Gap in Semiconductors," Physica, vol. 34, pp. 149-154, 1967.
[16] K. K. Tiong, T. S. Shou, and C. H. Ho, "Temperature Dependence Piezoreflectance Study of the Effect of Doping MoS2 with Rhenium," J. Phys. Condens. Matter, vol. 12, pp. 3441-3449, 2000.
[17] K. K. Tiong and T. S. Shou, "Anisotropic Electrolyte Electroreflectance Study of Rhenium-doped MoS2," J. Phys.Condens. Matter, vol. 12, pp. 5043-5052, 2000.
[18] K. K. Tiong and T. S. Shou, "Anisotropic Electrolyte Electroreflectance Study of Rhenium-doped MoS2," J. Phys. Condens. Matter, vol. 12, pp. 5043-5052, 2000.
[19] M. Yanagisawa, "Adsorption and configuration of lubrication molecules on overcoat materials," Wear, vol. 168, pp. 167-173, 1993.
[20] G. L. Frey, S. Elani, M. Homyonfer, Y. Feldman, and R. Tenne, "Optical-absorption spectraofinorganicfullerenelike MS2(M=Mo, W)," Phys. Rev. B., vol. 57, pp. 6666-6671, 1998.
[21] K. F. Mak, C. Lee, J. Hone, J. Shan, and F. T. Heinz, "Atomically Thin MoS2: A New Direct-Gap Semiconductor," Phys. Rev. Lett., vol. 105, pp. 136805-1~136805-4, 2010.
[22] A. M. Goldberg, A. R. Beal, F. A. Levy, and E. A. Davis, "The low-energy absorption edge in 2H-MoS2and 2H-MoSe2," Philos. Mag., vol. 32, pp. 367-378, 1975.