| 查看: 561 | 回复: 2 | |||
| 本帖产生 1 个 翻译EPI ,点击这里进行查看 | |||
[交流]
求助物理方面英译汉一段
|
|||
|
As mentioned above, besides high conductivity (~106 S), effective TCO thin films should have a very low absorption coefficient in the near UV-VIS-NIR region. The transmission in the near UV is limited by Eg, as photons with energy larger than Eg are absorbed. A second transmission edge exists at the NIR region, mainly due to reflection at the plasma frequency. Ideally, a wide band gap TCO should not absorb photons in the transmission “window” in the UV-VIS-NIR region. However, there are no “ideal” TCOs thin films, and even if such films could be deposited, reflection and interference would also affect the transmission. Hence, 100% transparency over a wide region cannot be obtained. The optical properties of TCOs transmission T, reflection R, and absorption A, are determined by its refraction index n, extinction coefficient k, band gap Eg, and geometry. Geometry includes film thickness, thickness uniformity, and film surface roughness. T, R and, A are intrinsic, depending on the chemical composition and solid structure of the material, whereas the geometry is extrinsic. There is a negative correlation between the carrier density and the position of the IR absorption edge, but positive correlation between the carrier density and the UV absorption edge, as Eg increases at larger carrier density (Moss-Burstein effect). As a result, the TCO transmission boundaries and conductivity are interconnected. The width of the VIS transmission window of a TCO film with thickness deposited on a transparent substrate is affected not only by the optical parameters of the TCO film but also by the optical properties of the substrate. The refractive index nsub of the most common substrates are ~1.45 for fused silica and ~1.6 for various glasses. The extinction coefficient of the substrate (ksub) is generally < 10-7, hence any light absorption would take place in the film, where generally kfilm> ksub. For films thicker than 100 nm, several interference bands could be formed, producing maximal and minimal values of T when either the wavelength or thickness is varied. When kfilm 0, the peak transmission (Tmax) is equal to the transmission of the substrate. Hence, assuming that the sample is in air, Tmax = 90% and 93% for films deposited on glass and fused silica, respectively. The minimum sample transmission (Tmin) in air is expressed by: As most TCO films have values of n in the VIS in the range 1.8 – 2.8, Tmin will be in the range 0.8 – 0.52. Tmin is closely approximated by the relation: Tmin = 0.051n2-0.545n+1.654. As n in the VIS decreases with wavelength, Tmin increases with wavelength, but will not exceed ~0.8. When the film extinction coefficient is not negligible and affects the transmission, Tmax < Tsub, and Tmin also decreases. By decreasing the TCO film thickness, T is increased but the sheet resistance decreases. Combining together the optical and electrical properties of the film, the fraction of the flux absorbed in a film (A) is given by the expression: Fig. 1 presents plots of the fraction of the absorbed power at wavelength of 400 nm and k ~0.02 as a function of the conductivity for three representative values of RS. For a given low values of RS necessitate using thick films, and lower conductivity requires the use of even thicker films, resulting in an increase in the loss of radiative power. The dependence of film thickness on the conductivity for three values of Rs is presented in Fig. 2. Using the same film conductivity, applications requiring the lowest RS will be thicker and, and the absorbed fraction will be higher. At present, only high quality ITO is compatible at present with the condition that the absorbed power fraction be lower than 10% and RS = 10 At lower extinction coefficient (k) films with lower conductivities can be used, e.g., when k = 0.002 instead of 0.02, the absorbed power A is lower by a factor of ~8, and allows the use of thicker films. The combination of film thickness, conductivity, and extinction coefficient determine the absorption of the radiation flux. However, when the total transmission T is considered, reflection and interference must be considered, which depend on the refractive indices of the substrate and the film, and the film thickness. A general formula for T and R was given by Cisneros. |
» 猜你喜欢
26申博求博导推荐-遥感图像处理方向
已经有5人回复
国家级人才课题组招收2026年入学博士
已经有6人回复
免疫学博士有名额,速联系
已经有7人回复
多组分精馏求助
已经有5人回复
交叉科学部支持青年基金,对三无青椒是个机会吗?
已经有7人回复
青椒八年已不青,大家都被折磨成啥样了?
已经有15人回复
国家基金申请书模板内插入图片不可调整大小?
已经有6人回复
Fe3O4@SiO2合成
已经有6人回复
» 抢金币啦!回帖就可以得到:
哈尔滨工程大学青岛创新发展基地招聘青年教师
+1/473
南方科技大学周友运课题组诚聘博士后、科研助理
+1/175
“超分子材料交叉研究团队”联合诚聘博士后 [清华/吉大/复旦/北大]
+1/79
【2026/2027 哈工大计算机类博士招生】
+1/78
诚聘 有机光电材料计算方向 博士后、科研助理、访问学生
+1/77
“超分子材料交叉研究团队”联合诚聘博士后 [清华/吉大/复旦/北大]
+1/76
【2026/2027 哈工大计算机类博士/硕士招生】
+1/74
广东工业大学自动化学院鲁仁全教授团队刘勇华老师招收2026年博士研究生(申请制)
+1/73
时隔多年再次回到小木虫,有一番感慨
+1/59
大连工业大学 超临界流体技术团队(纺材学院)招收2026级“申请-考核制”博士生
+1/55
意大利米兰理工大学急聘CSC公派留学博士生(物理或无机材料科学方向)
+2/32
以色列理工-生物质塑料等催化转化及流体力学方向---全奖博士研究生和科研助理
+2/16
美国密苏里大学堪萨斯城分校(UMKC)生物材料诚聘全奖博士
+1/11
复旦大学化学系凡勇教授/张凡教授团队招聘博士后
+1/8
法国斯特拉斯堡大学有机光伏全奖博士招聘
+1/7
以色列理工-生物质塑料等催化转化及流体力学方向---全奖博士研究生和科研助理
+2/4
中山大学柔性电子学院黄维院士团队诚招博士后(柔性可穿戴电子或相关方向)
+1/3
华南理工大学宋波教授招聘材料和化学方向博士后(长期有效)
+1/2
澳科大诚招2026年秋季全奖博士研究生(药剂学/生物材料方向)
+1/2
中山大学柔性电子学院黄维院士团队诚招柔性可穿戴电子方向博士生(2026年9月入学)
+1/1
zhengbiju1833(金币+1, 翻译EPI+1): 2011-03-22 13:26:59
|
不行,翻了一点儿发现有些专业符号不认识。。。 纠结。。。 As mentioned above, besides high conductivity (~106 S), effective TCO thin films should have a very low absorption coefficient in the near UV-VIS-NIR region. The transmission in the near UV is limited by Eg, as photons with energy larger than Eg are absorbed. 如上所述,除了高电导率(〜106 S)外,有效的TCO薄膜还应该在近紫外-可见-近红外吸收光谱区域有一个非常低的吸收系数。在近紫外区域的发射受到EG的限制,结果导致能量大于EG的光子被吸收。 |
2楼2011-03-16 17:19:32
3楼2011-03-16 17:27:12













回复此楼