| 研究生: |
張祐銘 Chang, Yu-Ming |
|---|---|
| 論文名稱: |
釩摻雜之二硒化鎢薄膜的光學特性與電性研究 Optical and Electrical Properties of V-Doped WSe2 Thin Films |
| 指導教授: |
王書瑋
Wang, Shu-Wei |
| 學位類別: |
碩士 Master |
| 系所名稱: |
智慧半導體及永續製造學院 - 半導體製程學位學程 Program on Semiconductor Manufacturing Technology |
| 論文出版年: | 2026 |
| 畢業學年度: | 114 |
| 語文別: | 中文 |
| 論文頁數: | 108 |
| 中文關鍵詞: | 二硒化鎢 、層數相依性 、釩摻雜濃度相依性 、拉曼光譜 、光致發光光譜 |
| 外文關鍵詞: | WSe2, layer dependence, V-doping dependence, Raman spectroscopy, photoluminescence |
| 相關次數: | 點閱:47 下載:1 |
| 分享至: |
| 查詢本校圖書館目錄 查詢臺灣博碩士論文知識加值系統 勘誤回報 |
本研究系統性探討釩(vanadium, V)取代式摻雜對二硒化鎢(WSe2)之振動、光學與電性的影響。以化學計量式VxW1−xSe2表示樣品,建立四種摻雜濃度(x = 0、0.002、0.003、0.005)與四種層數(單層至四層)共十六個樣品之系統性矩陣,進行拉曼光譜與光致發光光譜分析;並針對V0.003W0.997Se2之雙層與四層樣品,透過電子束微影(electron beam lithography, EBL)與反應性離子蝕刻(reactive ion etching, RIE)製作霍爾元件(Hall bar),進行電性量測。
拉曼光譜分析顯示,釩摻雜誘發 E_2g^1 、 A_1g 與 B_2g^1 三個振動模態之系統性紅移:顯示 V 原子取代 W 位點後可能造成局部鍵結環境改變,並降低有效鍵結力常數,使相關聲子模態呈現軟化現象。E_2g^1 紅移量隨層數增加而遞減(單層:1.47 cm⁻¹、四層:0.47 cm⁻¹),反映層間凡德瓦耦合對摻雜效應之穩定化作用。光致發光分析則顯示釩摻雜引發顯著之光譜紅移(單層約 60 meV、多層約 20–30 meV)、線形展寬與發光強度衰減,源於能帶重整化、能隙內缺陷態與非輻射復合通道之共同作用。電性量測結果顯示,雙層與四層元件均呈現雙極性傳輸行為,確認釩摻雜引入有效之受體能階。V0.003W0.997Se2之雙層元件具備較佳之閘極控制能力,四層元件則展現較高之場效遷移率與較大之開關電流比。
綜合上述結果,釩取代式摻雜於 WSe2 中所引發之鍵結軟化、晶格無序、能帶重整化等現象呈現相互呼應之物理機制,並隨層數展現顯著之相依行為。
This study systematically investigates the optical and electrical properties of vanadium-doped WSe2. V-doped WSe2 samples are denoted by VxW1−xSe2, where x is the fraction of W lattice sites substituted by V. A 4 × 4 sample matrix of four doping levels (x = 0, 0.002, 0.003, 0.005) and four layer thicknesses (monolayer to four-layer) was prepared for Raman and photoluminescence (PL) characterization, and Hall bar devices were fabricated from V0.003W0.997Se2 bilayer and four-layer flakes for electrical transport measurements at room temperature.
Raman analysis shows that V doping induces systematic redshifts in theE_2g^1,A_1g, and B_2g^1vibrational modes, suggesting that V substitution at W sites modifies the local bonding environment and reduces the effective force constant, leading to phonon softening. The E_2g^1 redshift magnitude decreases from 1.47 cm⁻¹ in monolayer to 0.47 cm⁻¹ in four-layer samples, evidencing the stabilizing influence of interlayer van der Waals coupling. PL spectroscopy further reveals a pronounced doping-induced redshift (~60 meV for monolayer, ~20–30 meV for multilayer), accompanied by linewidth broadening and emission quenching, arising from bandgap renormalization, in-gap defect states, and defect-mediated non-radiative recombination. Both bilayer and four-layer devices exhibit ambipolar transport behavior, confirming that V doping introduces effective acceptor states.
Overall, V substitution in WSe2 gives rise to bond softening, lattice disorder, band-structure modification, and acceptor-state formation, with pronounced layer-dependent behavior throughout.
[1] Novoselov, K. S., Jiang, D., Schedin, F., Booth, T. J., Khotkevich, V. V., Morozov, S. V., & Geim, A. K. (2005). Two-dimensional atomic crystals. Proceedings of the National Academy of Sciences, 102(30), 10451-10453.
[2] Wang, G., Chernikov, A., Glazov, M. M., Heinz, T. F., Marie, X., Amand, T., & Urbaszek, B. (2018). Colloquium: Excitons in atomically thin transition metal dichalcogenides. Reviews of Modern Physics, 90(2), 021001.
[3] Manzeli, S., Ovchinnikov, D., Pasquier, D., Yazyev, O. V., & Kis, A. (2017). 2D transition metal dichalcogenides. Nature Reviews Materials, 2(8), 17033.
[4] Tonndorf, P., Schmidt, R., Böttger, P., Zhang, X., Börner, J., Liebig, A., ... & Bratschitsch, R. (2013). Photoluminescence emission and Raman response of monolayer MoS2, MoSe2, and WSe2. Optics express, 21(4), 4908-4916.
[5] Zhao, W., Ghorannevis, Z., Amara, K. K., Pang, J. R., Toh, M., Zhang, X., ... & Eda, G. (2013). Lattice dynamics in mono-and few-layer sheets of WS 2 and WSe 2. Nanoscale, 5(20), 9677-9683.
[6] Kozhakhmetov, A., Stolz, S., Tan, A. M. Z., Pendurthi, R., Bachu, S., Turker, F., ... & Robinson, J. A. (2021). Controllable p‐type doping of 2D WSe2 via vanadium substitution. Advanced Functional Materials, 31(42), 2105252.
[7] Das, S., & Appenzeller, J. (2013). WSe2 field effect transistors with enhanced ambipolar characteristics. Applied physics letters, 103(10).
[8] Fang, H., Chuang, S., Chang, T. C., Takei, K., Takahashi, T., & Javey, A. (2012). High-performance single layered WSe2 p-FETs with chemically doped contacts. Nano letters, 12(7), 3788-3792.
[9] Pradhan, N. R., Rhodes, D., Memaran, S., Poumirol, J. M., Smirnov, D., Talapatra, S., ... & Balicas, L. (2015). Hall and field-effect mobilities in few layered p-WSe2 field-effect transistors. Scientific reports, 5(1), 8979.
[10] Sunil, K., & Ittyachen, M. A. (1997). The growth and thermodynamical feasibility of tungsten diselenide single crystals using chemical vapour transport technique. Bulletin of materials science, 20(2), 231-238.
[11] Tailor, J. P., Trivedi, D. S., Chaki, S. H., Chaudhary, M. D., & Deshpande, M. P. (2017). Study of chemical vapour transport (CVT) grown WSe1. 93 single crystals. Materials Science in Semiconductor Processing, 61, 11-16.
[12] Huang, Y., Sutter, E., Shi, N. N., Zheng, J., Yang, T., Englund, D., ... & Sutter, P. (2015). Reliable exfoliation of large-area high-quality flakes of graphene and other two-dimensional materials. ACS nano, 9(11), 10612-10620.
[13] Lukose, R., Lisker, M., Akhtar, F., Fraschke, M., Grabolla, T., Mai, A., & Lukosius, M. (2021). Influence of plasma treatment on SiO2/Si and Si3N4/Si substrates for large-scale transfer of graphene. Scientific reports, 11(1), 13111.
[14] Pizzocchero, F., Gammelgaard, L., Jessen, B. S., Caridad, J. M., Wang, L., Hone, J., ... & Booth, T. J. (2016). The hot pick-up technique for batch assembly of van der Waals heterostructures. Nature communications, 7(1), 11894.
[15] Allain, A., Kang, J., Banerjee, K., & Kis, A. (2015). Electrical contacts to two-dimensional semiconductors. Nature materials, 14(12), 1195-1205.
[16] Li, H., Wu, J., Huang, X., Lu, G., Yang, J., Lu, X., ... & Zhang, H. (2013). Rapid and reliable thickness identification of two-dimensional nanosheets using optical microscopy. ACS nano, 7(11), 10344-10353.
[17] Nemes-Incze, P., Osváth, Z., Kamarás, K., & Biró, L. P. (2008). Anomalies in thickness measurements of graphene and few layer graphite crystals by tapping mode atomic force microscopy. Carbon, 46(11), 1435-1442.
[18] Sahin, H., Tongay, S., Horzum, S., Fan, W., Zhou, J., Li, J., ... & Peeters, F. M. (2013). Anomalous Raman spectra and thickness-dependent electronic properties of WSe 2. Physical Review B—Condensed Matter and Materials Physics, 87(16), 165409.
[19] Terrones, H., Corro, E. D., Feng, S., Poumirol, J. M., Rhodes, D., Smirnov, D., ... & Terrones, M. (2014). New first order Raman-active modes in few layered transition metal dichalcogenides. Scientific reports, 4(1), 4215.
[20] Zhao, W., Ghorannevis, Z., Chu, L., Toh, M., Kloc, C., Tan, P. H., & Eda, G. (2013). Evolution of electronic structure in atomically thin sheets of WS2 and WSe2. ACS nano, 7(1), 791-797.
[21] Yun, S. J., Duong, D. L., Ha, D. M., Singh, K., Phan, T. L., Choi, W., ... & Lee, Y. H. (2020). Ferromagnetic order at room temperature in monolayer WSe2 semiconductor via vanadium dopant. Advanced Science, 7(9), 1903076.
[22] Mignuzzi, S., Pollard, A. J., Bonini, N., Brennan, B., Gilmore, I. S., Pimenta, M. A., ... & Roy, D. (2015). Effect of disorder on Raman scattering of single-layer Mo S 2. Physical Review B, 91(19), 195411.
[23] Chernikov, A., Ruppert, C., Hill, H. M., Rigosi, A. F., & Heinz, T. F. (2015). Population inversion and giant bandgap renormalization in atomically thin WS2 layers. Nature Photonics, 9(7), 466-470.
[24] Amani, M., Lien, D. H., Kiriya, D., Xiao, J., Azcatl, A., Noh, J., ... & Javey, A. (2015). Near-unity photoluminescence quantum yield in MoS2. Science, 350(6264), 1065-1068.
[25] Liu, G. B., Shan, W. Y., Yao, Y., Yao, W., & Xiao, D. (2013). Three-band tight-binding model for monolayers of group-VIB transition metal dichalcogenides. Physical Review B—Condensed Matter and Materials Physics, 88(8), 085433.
[26] Li, S. L., Tsukagoshi, K., Orgiu, E., & Samorì, P. (2016). Charge transport and mobility engineering in two-dimensional transition metal chalcogenide semiconductors. Chemical Society Reviews, 45(1), 118-151.
[27] Pham, Y. T. H., Liu, M., Jimenez, V. O., Yu, Z., Kalappattil, V., Zhang, F., ... & Phan, M. H. (2020). Tunable ferromagnetism and thermally induced spin flip in vanadium‐doped tungsten diselenide monolayers at room temperature. Advanced Materials, 32(45), 2003607.
[28] Radisavljevic, B., Radenovic, A., Brivio, J., Giacometti, V., & Kis, A. (2011). Single-layer MoS2 transistors. Nature nanotechnology, 6(3), 147-150.
[29] Liu, W., Kang, J., Sarkar, D., Khatami, Y., Jena, D., & Banerjee, K. (2013). Role of metal contacts in designing high-performance monolayer n-type WSe2 field effect transistors. Nano letters, 13(5), 1983-1990.