| 研究生: |
蔡政翰 Tsai, Cheng-Han |
|---|---|
| 論文名稱: |
製備單晶黃銅礦相加入Sb之Cu(In,B)S2奈米材料與薄膜及其特性分析 Synthesis and Characterization of Chalcopyrite Cu(In,B)S2 Nanocrystals and Films with Different Content of Sb |
| 指導教授: |
高騏
Gau, Chie |
| 學位類別: |
碩士 Master |
| 系所名稱: |
工學院 - 航空太空工程學系 Department of Aeronautics & Astronautics |
| 論文出版年: | 2014 |
| 畢業學年度: | 102 |
| 語文別: | 中文 |
| 論文頁數: | 94 |
| 中文關鍵詞: | 黃銅礦 、銅銦硼硫 、太陽能電池 、多元醇 、奈米粒子 |
| 外文關鍵詞: | CIBS nanocrystals, cost effective, solution process, compound materials for PV |
| 相關次數: | 點閱:73 下載:0 |
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在此研究中,我們利用多元醇法(polyol route)製備出具有單一黃銅礦晶相結構的CuIn1-xBxS2奈米粒子,並且加入Sb,x介於0~0.5之間。此研究之奈米粉體使用氯化銅(CuCl)、氯化銦(InCl3)、氧化硼(B2O3)及硫元素(S) 、氯化銻(SbCl3)藥品所製備,並去討論加入Sb後,在不同反應溫度、反應時間及PVP對CIBS莫耳比對實驗的影響。
在實驗過程中,我們不斷改變各式參數來討論CIBS奈米粒子的成長情況,並發現在這個實驗系統下,在PVP對CIBS的莫耳(mole)比在1:1.5,反應溫度310oC、反應時間6小時等條件下,合成出的奈米粒子其晶粒大小約介於30~40nm之間,輔以XRD及Raman分析鑑定的CIBS具有單一黃銅礦相結構、TEM、SEM影像了解更細微的顯微結構、使用EDS及ESCA光譜來檢驗CIBS的成分及UV-Visible吸收光譜發現製程較好的參數條件下所製備出的Cu(In0.9B0.1)S2薄膜其光能隙值(Band Gap)約為1.65 eV。
SUMMARY
Chalcopyrite of copper indium aluminum sulfur (Cu(In1-xBx)S2; CIBS) nanocrystals for solar cell materials have been successfully synthesized by a relatively simple and cost-effective method, i.e., a modified polyol route. The In/B ratio in the CIBS nanocrystals can be controlled by varying the In/B ratio in the reactants. The use of reactants, CuCl2, InCl3, B2O3 and S powders, in a three-neck flask with tetraethylene glycol as a solvent, spherical CIBS nanoparticles with diameter in the range of 30-40 nm can be obtained at temperatures in the range of 280 - 310oC. The characteristics and average sizes of these nanocrystals are analyzed with sophisticated instruments, such as X-ray diffraction pattern (XRD), transmission electron microscopy (TEM) and energy-dispersive X-ray spectroscopy (EDS). The nanocrystals can be readily dispersed in cyclohexanone with an ultrasound sonication, spin coated on a substrate and annealed at 450oC to form a film with grain growth. The composition of the final film and its optoelectronic properties are analyzed with electron spectroscopy for chemical analysis (ESCA), Hall effect and UV-visible measurements.
Keywords: CIBS nanocrystals, cost effective, solution process, compound materials for PV
INTRODUCTION
Chalcopyrite ternary semiconductors have often been employed as absorber layers in high-efficiency thin film solar cells because of their superior optoelectronic properties such as high mobility, long diffusion length, high absorption coefficient, suitable band gap etc. Increasing the efficiency of AIBIIICVI2 chalcopyrite photovoltaic cells from 14.1% (world record for CuInSe2) [4] by substitutions of In or Se with other elements from the same groups of periodic table have attracted much of the research attention. Photovoltaic cells based on an absorber layer of CuIn(S,Se)2, Cu(In,B)Se2, CuBS2, CuGaSe2, Cu(In,Ga)S2 and many other combinations have been made. Currently, the greatest energy conversion efficiency of 20.3% has been achieved for CIGS solar cells. Although the band gap of CuIn1-xGaxSe2 (CIGS) system is tunable in the range from 1.04 eV (CuInSe2) to 1.69 eV (CuGaSe2), further increasing of Eg towards to an optimum value of 1.37 eV leads to losses in fill factor and open circuit voltage, and a decrease in cell performance. Moreover, gallium is a rare and expensive element and selenium is a toxic material, replacing indium with boron and selenium with sulfur may be a first step to reduce the cost and make the solar cells user friendly. In addition, the optical band gap of CuInS2 and CuBS2 was 1.5 and 3.8 eV, respectively. Therefore it can be expected that the partial replacement of In by B can properly control the optical band gap and serves as another candidate of solar cell material, or as a top cell of the tandem solar cell when the bandgap is relatively large. In fact, fabrication of CIASe solar cells using sequential deposition of Cu, In, and Al with a final selenization process has been made that an energy conversion efficiency of 16.9% has been achieved. It appears that the success in fabrication of a good quality CIASe absorber to make a high efficiency of solar cell promotes the interest of study of CIAS and CIBS film made by a low cost solution process.
MATERIALS AND METHODS
For synthesis of the CIBS nanocrystals in the polyol process, a typical reaction can be made with 1 mmol of CuCl2, 0.9 mmol of InCl3, 0.1 mmol of B2O3, 2 mmol of elemental S and 0.1 mmol of SbCl3 in a 100-mL three-neck flask with attached condenser. the solution in the flask is then heated to 280-310 oC for 6h under vigorous stirring. Then, PVP dissolved in 20-mL of tetraethylene glycol was poured into the three-necked flask after reaction is complete. The use of PVP is to cap the nanoparticles so that not only it avoids aggregation of nanoparitcles, but also it can restrict diffusion of reactants into nanoparticles and significantly reduce the growth rate and size of the nanoparticles. After cooled to the room temperature, isopropyl alcohol is added into the solution to precipitate the CIBS nanocrystals. Purification is made initially by a centrifugation with a speed at 13,000 rpm for 5 min. Then, the brown-colored supernatant is decanted and the remaining solids are washed with isopropyl alcohol. The compositions and morphologies of the nanocrystals were determined by energy-dispersive X-ray spectroscopy (EDS) and transmission electron microscopy (TEM) using an acceleration voltage of 160 kV, respectively. Whereas the structural properties were determined by the X-ray diffraction (XRD) technique using CuK radiation (λ = 0.15418 nm). Finally the precipitates were dispersed in cyclohexanone with an ultrasound sonication to form a stable ink with a concentration of ~100 mg/ml. The cyclohexanone dispersed with CIBS nanocrystals can be spin coated on a quartz glass and annealed at 450 oC for 30 min in a graphite box to enhance grain growth. The thickness of the spin coated CIBS film is approximately 1.2 μm. Measurements of the optoelectronic properties for the CIBS thin film obtained can be made and provided for solar cell applications.
RESULTS AND DISCUSSION
Typical result of the nanoparticles from the XRD measurements is shown in Fig. 1, for B at different content and the diffraction peaks shift to higher 2θs with increasing the B content, due to the decreased lattice spacing with the smaller B atoms substituting for the larger In atoms. The TEM images of the CIBS nanoparticles formed is shown in Fig. 2. The size and morphology of the CIBS nanoparticles synthesized at 310oC for 6 h were further examined, as shown in Fig. 2 for both the TEM image of the CIBS nanoparticles. Figure 2 shows that the CIBS nanoparticles are poly-dispersed in both size and shape with particle sizes in the range of 30~40 nm. After spin coating the CIBS nanoparticles and formation into film by annealing, the grain size of the film with addition of Sb is much greater than the grain size of the film without Sb, as shown in Fig. 3. It appears that the Sb in the compound acts only as catalyst to promote grain growth during the annealing process.
The concentration and mobility of charge carries in the CIBS film are in the range from 3.5132 x 1013 to 4.1215 x 1012cm-3, and from 28.86 to 86.31 cm2/(V s), respectively in the Hall effect. The concentration and mobility of charge carriers in the CuInS2 film are 3.1521 x 1013 cm-3 and 31.58 cm2/(V s), respectively. It appears that slight addition of B into the CIS material, e.g. CI0.9B0.1S2, can increase carrier concentration but decrease the mobility of charge carriers. The variations of both carrier concentration and mobility with the molar ratio of B/(In+B) are shown in Fig. 4. When the molar ratio of B/(In+B) is greater than 0.1, the carrier concentration decreases with increasing the B contents whereas mobility increases with the B contents. The bandgap of the materials can be estimated from linear extrapolation of the curve for versus photo energy, as shown in Fig. 5 for the CIBS film with x=0.1 and the bandgap of 1.65 eV.
CONCLUSION
Chalcopyrite CIBS nanopcrystals for solar cell materials are successfully synthesized by using a relatively simple and convenient modified polyol route in three-neck flask with tetraethylene glycol as a solvent. The CIBS nanocrystals with diameters in the range of from 30 to 40 nm are obtained with increasing the B content from the reduction reactions of the chlorides of Cu, In, B, and elemental S powders under the temperatures at 310oC for 6h. The characteristics of these nanoparticles produced were analyzed with different analytical techniques. It appears that the reaction processes presented have advantages of short period, without sealing the container and requiring only cheap and simple precursors. The polyol solution acts as both a solvent and a reducing agent and is nontoxic ,and Sb is added with a modified surface structure. Formation of the nanocrystals synthesized into CIBS thin films with different contents of B can have good optoelectronic properties that are suitable for solar cell fabrication. The method proposed is user friendly and suitable for mass production.
[1] Udai P. Singha, William N. Shafarmanb, Robert W. Birkmireb, “Surface sulfurization studies of Cu(InGa)Se2 thin film,” Solar Energy Materials & Solar Cells., 90, p.623-630. (2006)
[2] 邱秋燕, 廖曰淳, 郭豐綱, “低成本銅銦鎵硒(CIGS)太陽電池技術發展” 工業材料, 276, p.58-68. (2009)
[3] A.S. Kindyak, V.V. Kindyak, V.F. Gremenok, “Energy-gap variations in thin laser-deposited Cu(In,Ga)Se2 films,” Materials Letters., 28, p.273-275. (1996)
[4] Arturo Morales-Acevedo, “Effective absorption coefficient for graded band-gap semiconductors and the expected photocurrent density in solar cells,” Solar Energy Materials & Solar cells., 93, P.41-44. (2009)
[5] M. A. Contreras, M. J. Romero, R. Noufi, “Characterization of Cu(In,Ga)Se2 materials used in record performance solar cells,” Thin Solid Films, 511-512, p.51-54. (2006)
[6] I. Repins, M.A. Contreras, B Egaas, C. DeHart, J. Scharf, C.L. Perkins, B. Yo, R. Noufi, “19.9%-efficient ZnO/CdS/CuInGaSe2 solar cell with 81.2% fill factor,” Progress in Photovoltaics., 16, P235.(2008)
[7] 何孟穎, “CIGS薄膜太陽電池技術優勢與研發進展” 光連雙月刊, 80, p.8-14. (2009)
[8] 徐如人, 龐文琴, “無機合成與製備化學” 五南圖書出版股份有限公司, p.733-742. (2004)
[9] 林琬蓉, “FePt合金粒子之製備與性質研究” 國立成功大學材料科學研究所碩士論文, p.5-8. (2007)
[10] C. B. Murray, D. J. Noms, and M. G. Bawendi, “Synthesis and characterization of nearly monodisperse CdE (E=S, Se, Te) semiconductor nanocrystallites,” J. Am. Chem. Soc., 115, p.8706-8715. (1993)
[11] 利宗倫, “以溶熱法合成Ⅰ-Ⅲ-Ⅵ 族CuInS2奈米 粒子及其特性探討” 國立成功大學化學工程研究所碩士論文, p.12-13. (2008)
[12] L. S. Li, N. Pradhan, Y. Wang, and X. Peng, “High quality ZnSe and ZnS nanocrystals formed by activating zinc carboxylate precursors,” Nano Letters., 4, p.2261-2264. (2004)
[13] M. A. Hines, G. S. Philippe, “Bright UV-blue luminescent colloidal ZnSe nanocrystals,” J. Phys. Chem. B, 102, p. 3655–3657. (1998)
[14] L. Qu, Z. A. Peng, and X. Peng, “Alternative routes toward high quality CdSe nanocrystals,” Nano Letters, 1, p.333-337. (2001)
[15] W. W. Yu, L. Qu, W. Guo, and X. Peng, “Experimental determination of the extinction coefficient of CdTe, CdSe, and CdS nanocrystals,” Chem. Mater, 15, p.2854-2860. (2003)
[16] W. W. Yu and X. Peng, “Formation of high-quality CdS and other II-VI semiconductor nanocrystals in noncoordinating solvents: tunable reactivity of monomers,” Angew. Chem. Int. Ed, 41, p.2368-2371. (2002)
[17] Z. A. Peng and X. Peng, “Nearly monodisperse and shape - controlled CdSe nanocrystals via alternative routes: nucleation and growth,” J. Am. Chem. Soc, 124, p.3343-3353. (2002).
[18] W. W. Yu, Y. A. Wang, and X. Peng, “Formation and stability of size-, shape-, and structure-controlled CdTe nanocrystals: ligand effects on monomers and nanocrystals,” Chem. Mater, 15, p. 4300-4308. (2003)
[19] N. Gaponik, D. V. Talapin, A. L. Rogach, K. Hoppe, E. V. Shevchenko, A. Kornowski, A. Eychmüller, H. Weller, “Thiol-capping of CdTe nanocrystals: an alternative to organometallic synthetic routes,” J. Phys. Chem. B, 106, p. 7177-7185. (2002)
[20] M. Shim, G. S. Philippe, “Organic-capped ZnO nanocrystals: synthesis and n-type character,” J. Am. Chem. Soc., 123, p.11651-11654. (2001)
[21] Dr. Rodney J. Soukup, Natale J. Ianno, Chad A. Kamler , Jiři Olejníček, Scott A. Darveau, and Christopher L. Exstrom, “Thin Films of CuInxB1-xSe2 as Absorbers for CIBS Solar Cells,” ECS Meet. Abstr., MA2009-02, p.761. (2009)
[22] R. J. Soukup, et. al., “Reaction Pathway Insights into the Solvothermal Preparation of Culn1-xGaxSe2 Nanocrystalline Materials,” Proc. 33 rd IEEE Photovoltaic Specialists Conference, 978-1-4244-1641-7/08, paper 191. (2008)
[23] Y. G. Chun, K. H. Kim, K. H. Yoon, “Synthesis of CuInGaSe2 nanoparticles by solvothermal route,” Thin Solid Films., 480-481, p.46-49. (2005)
[24] C. H. Chang, J. M. Ting, “Phase, morphology, and dimension control of CIS powders prepared using a solvothermal process,” Thin Solid Films., 517, p.4174-4178. (2009
[25] M. G. Panthani, V. Akhavan, B. Goodfellow, J. P. Schmidtke, L. Dunn, A. Dodabalapur, P. F. Barbara, B. A. Korgel, “Synthesis of CuInS2, CuInSe2, and Cu(InxGa1-x)Se2 (CIGS) nanocrystal “inks” for printable photovoltaics,” J. AM. Chem. SOC, 130, p.16770-16777. (2008)
[26] H. Grisaru, O. Palchik, A. Gedanken, “Microwave-assisted polyol synthesis of CuInTe2 and CuInSe2 nanoparticles,” Inorg. Chem., 42, p.7148-7155. (2003)
[27] J. Tang, S. Hinds, S. O. Kelley, E. H. Sargent, “Synthesis of colloidal CuGaSe2, CuInSe2, and Cu(InGa)Se2 nanoparticles,” Chem. Mater., 20, p.6906-6910. (2008)
[28] S. Ahn, K. Kim, Y. Chun, K. Yoon, “Nucleation and growth of Cu(In,Ga)Se2 nanoparticles in low temperature colloidal process,” Thin Solid Films., 515, p.4036-4040. (2007)
[29] J. D. Wu, L. T. Wang, C. Gau, “Synthesis of CuInGaSe2 nanoparticles by modified polyol route,” Solar EnergyMaterials&SolarCells, 98, p.404-408.(2012)
[30] F. Fievet, J. P. Lagier, B. Blin, “Homogeneous and heterogeneous nucleations in the polyol process for the preparation of micron and submicron size metal particles,” Solid State Ionics, 32-33, p. 198-205.(1989)
[31] P. Y. Silvert, R. Urbina, K. Elhsissen, “Preparation of colloidal silver dispersions by the polyol process,” J. Mater. Chem., 7, p.293-299.(1997)
[32] 王鉦源, “以化學還原法製備奈米級銀鈀微粉” 國立成功大學化學工程研究所碩士論文.(2008)
[33] G. Schmid, V. Maihack, F. Lantermann, S. Peschel, “Ligand-stabilized metal clusters and colloids: properties and applications,” J. Chem. Soc., 5, p.589-595.(1996)
[34] 任鏘諭, “奈米金屬微粒之製備及其特性研究” 國立清華大學化學工程研究所碩士論文.(1998)
[35] Yunbin He, “CuInS2 Thin Films for Photovoltaic:RF Reactive Sputter Deposition and Characterization,” Justus-Liebig-Universität Gießen Dissertation, p.1-119. (2003)
[36] S.-H.Wei and A. Zunger, “Predicted band-gap pressure coefficients of all diamond and zinc-blende semiconductors: Chemical trends,” Phys. Rev. B., 60, p.5404-5411. (1999)
[37] S.H. Wei, L.G. Ferreira, and A. Zunger, “First-principles calculation of the order-disorder transition in chalcopyrite semiconductors,” Phys.Rev.B., 45, p.2533-2536. (1992)
[38] Wei S.H., Zhang S.B., and Zunger A., “Band structure and stability of zinc-blende-based semiconductor polytypes,” Phys.Rev.B, 59, p.2478-2481. (1999)
[39] Alvarez-Garcia J, Pérez-Rodríguez A, Barcones B., Romano-Rodríguez A and Morante J.R., Scheer R., Janotti A. and Wei S.H., “Polymorphism in CuInS2 epilayers: origin of additional Raman modes,” Appl. Phys. Lett., 80, p.562-564. (2002)
[40] J.J.M. Binsma, L.J. Giling, J. Bloem, “Phase relations in the system Cu2S-In2S3,” Journal of Crystal Growth, 50, p.429-436. (1980)
[41] Krunksa M, Bijakina O, Varema T, Mikli V, Mellikov E, “Structural and optical properties of sprayed CuInS2 films,” Thin Solid Films, 338, p.125-130. (1999)
[42] S.C. Abrahams, J.L. Bernstein, “Piezoeletric nonlinear optic CuGaS2 and CuInS2 crystal structure: Sublattice distortion in AⅠBⅢCⅥ2 and AⅡBⅣCⅤ2 type chalcopyrites,” J. Chem. Phys., 59, p.5415-5422. (1973)
[43] A. Rockett and R. W. Birkmire, “CuInSe2 for photovoltaic applications,” J. Appl. Phys., 70, p.81-97. (1991)
[44] H.J. Lewerenz, “Development of copperindiumdisulfide into a solar material,” Sol. Energy Mater. Sol. Cells, 83, p.395-407. (2004)
[45] F. Abou-Elfotouh, D. J. Dunlavy, T. J. Coutts, “Intrinsic defect states in CuInSe2 single crystals,” Solar Cells, 27, p.237-245. (1989)
[46] A. Slaoui and R. T. Collins, “Advanced inorganic materials for photovoltaics,” MRS Bull., 32, p.211-218. (2007)
[47] P. D. Paulson, M. W. Haimbodi, S. Marsillac, R. W. Birkmire and W. N. Shafarman, “CuIn1-xAlxSe2 thin films and solar cells,” J. Appl. Phys., 91, p.10153-10156. (2002)
[48] I. Repins, M. A. Contreras, B. Egaas, C. DeHart, J. Scharf, C. L. Perkins, B. To and R. Noufi, “19.9%-efficient ZnO/CdS/CuInGaSe2 solar cell with 81.2% fill factor,” Progr. Photovolt.: Res. Appl., 16, p.235-239. (2008)
[49] S. Marsillac, P. D. Paulson, M. W. Haimbodi, R. W. Birkmire and W. N. Shafarman, “High-efficiency solar cells based on Cu(InAl)Se2 thin films,” Appl. Phys. Lett., 81, p.1350-1352. (2002)
[50] A. Katerskia, A. Merea, V. Kazlauskieneb, J. Miskinisb, A. Saarc, L. Matisenc, A. Kikasc, M. Krunksa, “Surface analysis of spray deposited copper indium disulfide films,” Thin Solid Films, 516, p. 7110–7115.(2008)
[51] G.H. Yue, X. Wang, L.S. Wang, W. Wang, D.L. Peng, “Synthesis of single crystal CuAlS2 nanowires via a low temperature direct polyol route,” Phys. Lett. A, 372, P. 5995–5998.(2008)
[52] S.H. Wei and A. Zunger, “Band offsets and optical bowings of chalcopyrites and Zn-based II-VI alloys,” J. Appl. Phys., 78, p.3846-3856. (1995)
[53] 李俊賢”Fabrication of CuInSe2:Sb Thin Flim Solar Cell”國立中山大學材料科學研究所(2004)
[54] Min Yuan, David B. Mitzi, Wei Liu,Andrew J. Kellock, S. Jay Chey, and Vaughn R.eline “Optimization of CIGS-Based PV Device through Antimony Doping,” Mater, 22,285–287,285, (2010)
[55] 林麗娟, “X光繞射原理及其應用”工業材料, 86, p.100-109. (1994)
[56] N.J.Ianno, R.J. Soukup, T. Santero, C. Kamler, J. Huguenin-Love, S.A. Darveau, J. Olejnicek, and C. Exstrom, “Copper-Indium-Boron-Diselenide Absorber Materials,” Mater. Res. Soc. Symp. Proc., 1012, Y03-21-Y03-26. (2007)
[57] S. Ahn, C. Kim, Y. Chun, J. Yun, J. Lee, “Effects of heat treatments on the properties of Cu(In,Ga)Se2 nanoparticles,” Solar Energy Materials & Solar Cells., 91, p.1836-1841. (2007)
[58] S. Ahn, K. H. Kim, J. H. Yun, K. H. Yoon, “Effects of selenization conditions on densification of Cu(In,Ga)Se2 (CIGS) thin films prepared by spray deposition of CIGS nanoparticles,” Journal of Applied Physics., 105, p.113533-113533-7. (2009)
[59] Lin-Jer Chen, Jiunn-Der Liao, Yu-Ju Chuang, and Yaw-Shyan Fu, “Synthesis and Characterization of Cu(InxB1-x)Se2 Nanocrystals for Low-Cost Thin Film Photovoltaics,” J. Am. Chem. Soc., 133, p.3704-3707. (2011)
[60] Q. Guo, G. M. Ford, H. W. Hillhouse and R. Agrawal, “Sulfide Nanocrystal Inks for Dense Cu(In1−xGax)(S1−ySey)2 Absorber Films and Their Photovoltaic Performance,” Nano Lett., 9(8), p.3060-3065. (2009)
[61] D. Pan, X. Wang, Z. H. Zhou, W. Chen, C. Xu and Y. Lu, “Synthesis of Quaternary Semiconductor Nanocrystals with Tunable Band Gaps,” Chem. Mater., 21, p.2489-2493. (2009)
[62] Chongyin Yang, Yaoming Wang, Shaotang Li, Dongyun Wan, Fuqiang Huang, “CuSbSe2-assisted sintering of CuInSe2 at low temperature,” J Mater Sci , 47:7085–7089, (2012)
[63] Bodnar I. V., Tsyrelchuk I. N. and Victorov I .A., “Preparation and analysis of the CuAlxInl-xSe2 solid solutions,” J. Mater. Sci. Lett., 13, p.762-764. (1994)
[64] B. J. Stanbery, “Copper Indium Selenides and Related Materials for Photovoltaic Devices,” Crit. Rev. Solid State Mat. Sci., 27(2), p.73-113. (2002)
[65] B. D. Cullity, “Elements of Xray Diffraction”, Addison Wesley, p284. (1978)
[66] J. Lo´pez-Garcı´a, C. Maffiotte, C.Guille´n, “Wide-bandgap CuIn1-xAlxSe2 thin films deposited on transparent conducting oxides,” Solar Energy Materials & Solar Cells, 94, p. 1263-1269.(2010)
[67] A. Katerski, A. Mere, V. Kazlauskiene, J. Miskinis, A. Saar,L. Matisen, A. Kikas, M. Krunks , “Surface analysis of spray deposited copper indium disulfide films,” Thin Solid Films, 516, p. 7110-7115.(2008)
[68] T.Schulmeyer, R.Kniese, R.Hunger, W.Jaegermann, M.Powalla, A.Klein, “Influence of Cu(In,Ga)Se2 band gap on the valence band offset with CdS,” Thin Solid Films, 451-452, p.420-423.(2004)
[69] S. Marsillac, J.C. Bernede, C. El Moctar, J. Pouzet, “Physico-chemical characterization of CuAlSe2 films obtained by reaction, induced by annealing, between Se vapour and Al/Cu/AI…Cu/Al/Cu thin films sequentially deposited,” Materials Science and Engineering, 45, p.69-75.(1997)
[70] D. Q. Yang and E. Sacher, “Core/Shell Formation of Gold Nanoparticles Induced on Exposure to N, N-Dimethylformamide: Chemical and Morphological Changes,” J. Phys. Chem. C, 111, p. 14320-14326. (2007)
[71] L.L. kazmerski, “Photovoltaics: A review of cell and module technologies,” Renewable and sustainable energy review, 1, p.71-171. (1997)
[72] I.V. Bodnar, L.V. Golubev, V.G. Plotnichenko, E.A. Smolyaninova, “Raman Scattering in CuGaSe2,” Phys. Status Solidi B, 105, K111- K114. (1981)
[73] C. Guillen, J. Herrero, M.t. Gutierrez, F. Briones, “Structure, morphplogy and optical properties of CuInS2 thin films prepared by modulated fiux deposition,” Thin Solid Films, 480, p.19-23. (2005)
[74] B. Barcones, A. Pérez-Rodríguez, L. Calvo-Barrio, A. Romoano-Rodríguez, J.R. Morante, E.Rudigier, I.Luck, J.Djordjevic, R. Scheer, “In situ and ex situ characterization of thermally induced crystallization of CuInS2 thin films for solar cell,” Thin Solid Films, 408-481, p.362-366. (2005)
[75] J. Álvarez-García, J. Marcos-Ruzafa, A. Pérez-Rodríguez , A. Romano-Rodríguez, J.R. Morante , R. Scheer, “MicroRaman scattering from polycrystalline CuInS2 films,” Thin Solid Films, 361-362, p.208-212. (2000)
[76] D. Papadimitriou, N. Esser, and C. Xue, “Structural properties of chalcopyrite thin films studied by Raman spectroscopy,” phys. stat. sol. (b), 242, p.2633-2643. (2005)
[77] J. Olejníček , C.A. Kamler , A. Mirasano , A.L. Martinez-Skinner , M.A. Ingersoll , C.L. Exstrom ,S.A. Darveau , J.L. Huguenin-Love , M. Diaz , N.J. Ianno , R.J. Soukup, “A non-vacuum process for preparing nanocrystalline CuIn1-xGaxSe2 materialsinvolving an open-air solvothermal reaction,” Solar Energy Materials and Solar Cells, 94, p.8-11. (2010)
[78] S. Theodoropoulou, D. Papadimitriou, N. Rega, S. Siebentritt, M.Ch. Lux-Steiner, “Raman and photoreflectance study of CuIn1-xGaxSe2 epitaxial layers,” Thin Solid Films, 511-512, p.690-694. (2006)
[79]Shu Zhang, Lu Wu, Ruoyu Yue, Zongkai Yan, Haoran Zhan, Yong Xiang“Effects of Sb-doping on the grain growth of Cu(In, Ga)Se2 thin films fabricated by means of single-target sputtering,” Thin Solid Films ,527,137–140,(2013)
校內:2019-08-27公開