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1.
张超  敖建平  姜韬  孙国忠  周志强  孙云 《物理学报》2013,62(7):78801-078801
使用等离子体活化硒源对电沉积制备的Cu-In-Ga金属预制层进行了硒化处理时, 发现等离子体功率对Cu(In1-xGax)Se2(CIGS)晶粒的生长有重要影响, 当等离子体功率为75 W时, 制备出单一Cu(In0.7Ga0.3)Se2相的CIGS薄膜. 通过对不同衬底温度的等离子体活化硒源硒化的CIGS 薄膜进行了研究与分析, 并与普通硒化后的薄膜进行对比, 发现高活性硒在低温下会促进Ga-Se二元相的生成, 从而有利于Cu(In0.7Ga0.3)Se2单相的生长. 对等离子体硒化后的CIGS薄膜进行了电池制备, 发现单相CIGS薄膜没有显著提高电池性能. 通过优化工艺, 所制备的CIGS电池效率达到了9.4%. 关键词: 0.7Ga0.3)Se2')" href="#">Cu(In0.7Ga0.3)Se2 电沉积 Cu-In-Ga金属预制层 等离子体活化硒  相似文献   

2.
李志国  刘玮  何静婧  李祖亮  韩安军  张超  周志强  张毅  孙云 《物理学报》2013,62(3):38803-038803
研究了三步法第二步沉积速率对低温生长Cu(In,Ga)Se2薄膜结构、 电学特性和器件特性的影响. 通过改变第二步沉积速率发现, 提高沉积速率可以显著促进薄膜晶粒生长, 提高晶粒紧凑程度降低晶界复合, 同时有效改善两相分离现象, 提高电池的开路电压和短路电流, 有助于Cu(In,Ga)Se2电池光电转换效率的提高. 但同时研究表明, 随着第二步沉积速率的增加, 会促进暂态Cu2-xSe晶粒的生长, 引起Cu(In,Ga)Se2薄膜表面粗糙度增大, 并阻碍Na向Cu(In,Ga)Se2薄膜表面的扩散, 造成施主缺陷钝化效应降低, 薄膜载流子浓度下降和电阻率升高, 且过高的沉积速率会引起电池内部复合增加并产生分流路径, 造成开路电压下降进而引起电池效率恶化. 最终, 通过最佳化第二步沉积速率, 在衬底温度为420℃时, 得到最高转换效率为11.24%的Cu(In,Ga)Se2薄膜太阳电池.  相似文献   

3.
分别在苏打石灰玻璃、Mo箔、无择优取向的Mo薄膜以及(110)择优取向的Mo薄膜四种不同衬底上,采用共蒸发工艺沉积约2 μm厚的Cu(In,Ga)Se2薄膜,用X射线衍射仪测量薄膜的织构,研究衬底对Cu(In,Ga)Se2薄膜织构的影响.在以上四种衬底上沉积的Cu(In,Ga)Se2薄膜的(112)衍射峰强度依次逐渐减弱,(220/204)衍射峰从无到有且强度逐渐增强.在苏打石灰玻璃和Mo箔衬底上的Cu(In,Ga)Se2关键词: 择优取向 Cu(In 2薄膜')" href="#">Ga)Se2薄膜 太阳电池  相似文献   

4.
敖建平  杨亮  闫礼  孙国忠  何青  周志强  孙云 《物理学报》2009,58(3):1870-1878
采用电沉积法获得了接近化学计量比的贫铜和富铜的Cu(In1-xGax)Se2(CIGS)预置层,研究比较了两种预置层及其硒化处理后的成分和结构特性.得到了明确的实验证据证明,硒化后富铜薄膜中的CuxSe相会聚集凝结成结晶颗粒分散在表面.研究表明:在固态源硒化处理后,薄膜成分基本不变;当预置层中原子比Cu/(In+Ga)<11时,硒化后薄膜表面存在大量的裂纹;而当Cu/(In+Ga) >12时,可以消除裂纹的产生,形成等轴状小晶粒;富铜预置层硒化时蒸发沉积少量In,Ga和Se后,电池效率已达到68%;而贫铜预置层硒化后直接制备的电池效率大于2%,值得进一步深入研究. 关键词: 1-xGax)Se2薄膜')" href="#">Cu(In1-xGax)Se2薄膜 电沉积 硒化处理 贫铜或富铜薄膜  相似文献   

5.
研究了金属预制层制备过程中溅射气压对Cu(In1-xGax)Se2(CIGS)薄膜及电池器件性能的影响.通过调节溅射气压改变预制层的结晶状态及疏松度与粗糙度,在合适的预制层结构下,活性硒化热处理过程中,可使Ga有效地掺入到薄膜中形成优质的CIGS固溶体.高溅射气压会使预制层过于致密,呈现非晶态趋势.经活性硒化热处理后,CIGS薄膜容易产生CIS与CGS"两相分离"现象,从而导致CIGS薄膜太阳电池的开路电压和填充因子降低,电池转换效率由10.03%降低到5.02%.  相似文献   

6.
刘芳芳  张力  何青 《物理学报》2013,62(7):77201-077201
CIGS薄膜的结晶相是制备高质量薄膜的关键问题. 本文采用共蒸发"三步法"工艺沉积Gu(In, Ga)Se2 (CIGS) 薄膜, 通过X射线衍射仪 (XRD) 和X射线荧光光谱仪 (XRF)、扫描电镜 (SEM) 结合的方法详细研究了"三步法"工艺的相变过程, 并制备出转换效率超过15% 的 CIGS 薄膜太阳电池. 关键词: CIGS薄膜 共蒸发三步法 相变过程  相似文献   

7.
研究了110~180 ℃(2 min)下的快速热退火对Cu(In,Ga)Se2(CIGS)薄膜特性及CIGS太阳电池性能的影响.结果表明:对于不同成分比例的CIGS(正常、富Cu、高Ga)电池来说,150 ℃,2 min的快速退火最利于电池性能及二极管特性的增加.其中,退火对富Cu电池的开路电压Voc改善最大,这是因为快速热退火对消除部分CIGS薄膜中的CuSex有积极作用,从薄膜的电阻率有少量提高,器件的短路电流Jsc有少量下降可以得到验证|而对于高Ga电池来说,填充因子FF的改善最大,这是因为高Ga样品的缺陷较多,退火会消除薄膜内部的部分缺陷,从而薄膜的迁移率及Jsc都有所提高,使得FF有较大的增加.  相似文献   

8.
张超  敖建平  毕金莲  姚立勇  孙国忠  周志强  何青  孙云 《物理学报》2013,62(23):238801-238801
以H2S气体作为硫源、固态蒸发硒蒸气作为硒源对电沉积Cu-In-Ga金属预制层进行硒硫化处理. 通过电沉积Cu-In-Ga金属预制层在不同衬底温度下硒化、硫化和硒硫化的对比实验,发现CuInS2相和CuIn(S,Se)2相优先生成,抑制了CuInSe2相的生成,促使InSe相薄膜向内部扩散,减弱了薄膜两相分离现象. 采用先硒化后硒硫化处理工艺优化了Cu(In,Ga)(S,Se)2薄膜的制备工艺,在250 ℃预硒化得到了开路电压为570 mV的太阳电池,在更高的预硒化温度得到了较大短路电流的太阳电池,最终优化得到了效率达到10.4%的电池器件. 关键词: 电化学沉积 Cu-In-Ga金属预制层 硒硫化处理 2薄膜')" href="#">Cu(In,Ga)(S,Se)2薄膜  相似文献   

9.
采用射频等离子体辅助分子束外延技术生长得到了In组分精确可控且高质量的InxGa1-xN (x ≤ 0.2) 外延薄膜. 生长温度为580 ℃的In0.19Ga0.81N薄膜(10.2) 面非对称衍射峰的半高宽只有587弧秒, 背景电子浓度为3.96× 1018/cm3. 在富金属生长区域, Ga束流超过N的等效束流时, In组分不为零, 即Ga并没有全部并入外延层; 另外, 稍微增加In束流会降低InGaN的晶体质量. 关键词: InGaN 外延薄膜 射频等离子体辅助分子束外延 In 并入 晶体质量  相似文献   

10.
张坤  刘芳洋  赖延清  李轶  颜畅  张治安  李劼  刘业翔 《物理学报》2011,60(2):28802-028802
通过直流反应磁控溅射技术,原位生长制备了太阳电池用Cu2ZnSnS4(CZTS)薄膜.采用X射线能量色散谱仪、扫描电镜、X射线衍射仪、紫外可见分光光度计和霍尔效应测试系统对薄膜进行了表征.结果表明,原位生长的CZTS薄膜具有均质、致密和平整的形貌,且由贯穿整个薄膜厚度的柱状颗粒组成.不同基底温度下生长所得薄膜的Cu/(Zn+Sn) 值均约为1,而Zn/Sn值均大于1且随着基底温度升高而减小.所得薄膜在(112)方向上择优取向明显,且结构特征受基底温度和Cu/(Zn+Sn)的共同影响.所得薄膜均具有高达104cm-1的光吸收系数,其带隙宽度随着生长温度的增加而降低,并且在500℃时为(1.51±0.01)eV.薄膜的导电类型均为p型,且具有与器件级Cu(In,Ga)Se2(CIGS)相当的载流子浓度. 关键词: 2ZnSnS4')" href="#">Cu2ZnSnS4 直流反应磁控溅射 原位生长 太阳电池  相似文献   

11.
The electrical and structural properties of polycrystalline Cu(In, Ga)Se2 films grown on polyimide (PI) substrates below 400℃ via one-stage and three-stage co-evaporation process have been investigated by x-ray diffraction spectra (XRD), scanning electron microscopy (SEM) and Hall effect measurement. As shown by XRD spectra, the stoichiometric CIGS films obtained by one-stage process exhibit the characteristic diffraction peaks of the (In0.68Ga0.32)2Se3 and Cu(In0.7Ga0.3)2Se. It is also found that the film structures indicate more columnar and compact than the three-stage process films from SEM images. The stoichiometric CIGS films obtained by three-stage process exhibit the coexistence of the secondary phase of (In0.68Ga0.32)2Se3, Cu2-xSe and Cu(In0.7Ga0.3)2Se. High net carrier concentration and sheet conductivity are also observed for this kind of film, related to the presence of Cu2-xSe phase. As a result, when the CIGS film growth temperature is below 400℃, the three-stage process is inefficient for solar cells. By using the one-stage co-evaporation process, the flexible CIGS solar cell on a PI substrate with the best conversion efficiency of 6.38% is demonstrated (active area 0.16cm^2).  相似文献   

12.
Intense pulsed light (IPL) technique has been proposed to make large grains Cu(In0.7Ga0.3)Se2 (CIGS) film using CIGS particles. The proposed process is non-vacuum based and performed at room temperature without selenization treatment. Melting and recrystallization of CIGS particles to larger grains without structural deformation and phase transformation are proved with adequate characterization evidences. X-ray powder diffraction (XRD), scanning electron microscopy (SEM) and energy dispersion analysis (EDS) were used to characterize the prepared films. Melting of the CIGS particles and recrystallization to larger grains by light energy in 20 ms short reaction time could be the reason for no structural deformation and secondary phase generation during the process. The CIGS film prepared from its constituent nanoparticles by IPL treatment has great potential for use as absorber layer for solar cell application and is expected to have large impact on cell fabrication process in terms of cost reduction and simplified processing.  相似文献   

13.
This work reports unexpected crystallization and segregation behavior of CuIn0.7Ga0.3Se2 (CIGS) thin films deposited on flexible Cu foils by pulsed laser deposition. A composite-type microstructure containing nanometer-scaled CIGS crystallites embedded in amorphous Cu-rich matrix is observed even at the high temperature of 500 °C. The findings are attributed to very fast condensation of the ablated species and random nucleation induced from the amorphous matrix. Cu-rich particulates tend to precipitate on the film surface, and their average size, shape, number density and composition exhibit a strong dependence on the substrate temperature up to 500 °C. The similar crystallization properties of the films on Cu foils and glass substrates are noticeable to the use of Cu foils for flexible solar cells.  相似文献   

14.
We report the effect of Cr impurity barrier on Cu(In,Ga)Se2 (CIGS) thin-film solar cells prepared on flexible substrates. The Cr films with varying the thickness (tCr) were deposited on stainless steel substrates using direct-current magnetron sputtering. The solar cell performance was improved by increasing tCr since the diffusion of Fe impurities from the substrate to CIGS was suppressed. Although the elemental composition, grain size, and strain of CIGS film showed little change with varying Fe content, the fill factor and the short-circuit current density increased as decreasing Fe. The Fe increased the series resistance, shunt paths, and saturation current density. The reduction of Fe caused a steeper bandgap grading in CIGS which enhances current collection due to higher electric fields in bulk CIGS. CIGS solar cells with 1000 nm-thick Cr barrier showed the best conversion efficiency of 9.05%.  相似文献   

15.
刘芳芳  孙云  何青 《物理学报》2014,63(4):47201-047201
传统制备Cu(In,Ga)Se2(CIGS)手段之一是共蒸发三步法,工艺中通过Cu,In,Ga,Se 4种元素相互扩散、作用形成抛物线形的Ga梯度分布.本文通过调整Ga源温度制备了Ga梯度分布不同的CIGS薄膜及电池.利用多种测试方法,研究了Ga梯度分布不同对CIGS薄膜表面及背面结构性质及电性质的影响,计算分析了表面导带失调值及背面电场对电池性能的影响,从而获得了合适的Ga梯度分布,提高了电池光谱相应,获得了较好的电池性能参数.  相似文献   

16.
Cu(In,Ga)Se2 (CIGSe) thin film solar cells were fabricated by direct inkjet printing of Cu(In,Ga)S2 (CIGS) nanoparticles followed by rapid thermal annealing under selenium vapor. Inkjet printing is a low-cost, low-waste, and flexible patterning method which can be used for deposition of solution-based or nanoparticle-based CIGS films with high throughput. XRD and Raman spectra indicate that no secondary phase is formed in the as-deposited CIGS film since quaternary chalcopyrite nanoparticles are used as the base solution for printing. Besides, CIGSe films with various Cu/(In + Ga) ratios could be obtained by finely tuning the composition of CIGS nanoparticles contained in the ink, which was found to strongly influence the devices performance and film morphology. To date, this is the first successful fabrication of a solar device by inkjet printing of CIGS nanoparticles.  相似文献   

17.
Thin films of Cu(In, Ga)Se2 (CIGS) with a Ga/(Ga + In) ratio of ~0.27 corresponding to the standard elemental composition for solar-energy transducers were grown on Mo-coated glass substrates by the Cu, In, Ga, and Se co-evaporation technique from different sources. Transmission (T), photoluminescence (PL), and photoluminescence excitation (PLE) spectra at 4.2 K were used to analyze electronic properties in the asgrown and electron-irradiated CIGS films. The band-gap energy (Eg) of the CIGS films measured using both transmission and PLE methods was found to be about 1.28 eV at 4.2 K. Two deep bands in the PL spectra of the irradiated CIGS films, P1 at ~0.91 eV and P2 at ~0.77 eV, have been detected. These bands are tentatively associated with copper atoms substituting indium (CuIn) and indium vacancies VIn, respectively, as the simplest radiation-induced defects.  相似文献   

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