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1.
采用固相法和真空烧结技术制备了5at%Yb3+,2at%Er3+:YAG透明陶瓷.在1760 ℃真空烧结30 h后, 陶瓷样品具有较高透过率.SEM观察表明制备的透明陶瓷在晶粒和晶界处无气孔、第二相的存在.样品的吸收光谱和荧光光谱的测试结果表明: Yb3+在940nm波长处有具有较强的吸收系数.样品在1030nm波长的荧光寿命仅为0.274 ms,以及在1.5μm波段的荧光衰减寿命曲线中,初始的荧光强度呈上升趋势,这些表明了Yb,Er:YA
关键词:
Er
Yb:YAG透明陶瓷
1.5 μm荧光光谱
Judd-Ofelt理论 相似文献
2.
对一种低温易烧结的Yb:Y2-2xLa2xO3激光透明陶瓷的光谱性能进行了初步研究,Yb:Y2-2xLa2xO3激光透明陶瓷具有宽的吸收带和大的吸收截面,在最强的吸收峰977nm处吸收截面达4.0×10-20cm2;其荧光发射寿命为1.1ms,发射截面在1033nm处为1.0×10-20cm2,在1077nm处为0.7×10-20cm2.Yb:Y2-2xLa2xO3陶瓷的各项光学性能指标接近或达到单晶的指标.
关键词:
氧化镧钇
激光陶瓷
低温烧结
光谱性能 相似文献
3.
研究了衬底温度对MOCVD技术制备的ZnO薄膜的微观结构和光电特性影响. XRD和SEM的研究结果表明,衬底温度对ZnO薄膜的微观结构有显著影响,明显的形貌转变温度大约发生在175℃,低于175℃,薄膜呈镜面结构,晶粒为球状,高于177℃的较高温度范围,薄膜从“类金字塔”状的绒面结构演化为“岩石”状显微组织;随着温度增加,薄膜的晶粒尺寸明显增大.绒面结构的未掺杂ZnO薄膜具有17.96 cm2/V·s的高迁移率和3.28×10-2 Ω·cm的低电阻率,对ZnO薄膜的进一步掺杂和结构优化有望应用于Si薄膜太阳电池的前电极.
关键词:
MOCVD
ZnO薄膜
透明导电氧化物
太阳电池 相似文献
4.
对透光性良好的Cr3+:Al2O3透明多晶陶瓷的光谱性能 进行了研究,其吸收光谱中吸收峰与单晶红宝石相一致,按吸收光谱和Tanabe-Sugano能级 图,算出其晶场强度参数Dq及Racah参数B分别为1792cm-1, 689cm -1,Dq/B=2.6,陶瓷中Cr3+离子所处格位的晶体场强 比单晶弱一些,但Cr3+:Al2O3透明陶瓷仍属于强场晶 体材料;当Cr3+掺杂浓度到达0.8wt%时,陶瓷的发射谱仍保持较好的R线发射 ;随Cr3+掺杂浓度的增大,激发峰位发生“红移”.在Cr3+:Al2O3透明多晶陶瓷的荧光谱上,发现一个波长为670nm的发射峰,经激发 谱确认为Cr3+的发射峰.
关键词:
氧化铝
透明陶瓷
离子格位
光谱性质 相似文献
5.
采用传统无压烧结工艺制备Cr:Al2O3透明多晶陶瓷.测定了其退火前后的吸收光谱和荧光光谱,发现在Al2O3六配位的八面体结构中,Cr4+的荧光发射也处在1100—1600nm波段的红外区间,荧光发射峰位于1223nm附近,类似Cr4+在四面体中的发光行为.同时由于氧化铝晶格常数较小,晶体场强较强,使Cr4+:Al2O3<
关键词:
4+')" href="#">Cr4+
2O3透明陶瓷')" href="#">Cr:Al2O3透明陶瓷
光谱性质
八面体 相似文献
6.
采用传统无压烧结工艺制备了Nd3+掺杂的Y2-2xLa2xO3(x=0.08)透明陶瓷并对其光谱性能进行了研究. 结果表明:Nd3+:Y1.84La0.16O3透明陶瓷在780—850 nm的波长范围内有较宽的吸收带. 当Nd3+掺杂量为1.5at%时,在820 nm和激光二极管抽运的808 nm处的吸收截面分别为σabs(820 nm)=1.81×10-20 cm2,σabs(808 nm)=1.54×10-20 cm2. 最强的发射峰位于1078 nm处,并具有荧光寿命长、发射带宽宽、量子效率高等特点. 加入La2O3后,基质的光谱品质参数XNd由1.6减小到0.46,因此和4F3/2—4I11/2跃迁相对应的荧光分支比βJ,11/2增大为56.82%. Nd3+:Y1.84La0.16O3透明陶瓷的这些性质有利于高效率的激光输出和超短锁模激光脉冲的实现.
关键词:
氧化镧钇透明陶瓷
光谱性能
3+')" href="#">Nd3+ 相似文献
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11.
H. Kim A. Cepler C. Cetina D. Knies M. S. Osofsky R. C. Y. Auyeung A. Piqué 《Applied Physics A: Materials Science & Processing》2008,93(3):593-598
Present p-type ZnO films tend to exhibit high resistivity and low carrier concentration, and they revert to their natural n-type state
within days after deposition. One approach to grow higher quality p-type ZnO is by codoping the ZnO during growth. This article describes recent results from the growth and characterization
of Zr–N codoped p-type ZnO thin films by pulsed laser deposition (PLD) on (0001) sapphire substrates. For this work, both N-doped and Zr–N
codoped p-type ZnO films were grown for comparison purposes at substrate temperatures ranging between 400 to 700 °C and N2O background pressures between 10−5 to 10−2 Torr. The carrier type and conduction were found to be very sensitive to substrate temperature and N2O deposition pressure. P-type conduction was observed for films grown at pressures between 10−3 to 10−2 Torr. The Zr–N codoped ZnO films grown at 550 °C in 1×10−3 Torr of N2O show p-type conduction behavior with a very low resistivity of 0.89 Ω-cm, a carrier concentration of 5.0×1018 cm−3, and a Hall mobility of 1.4 cm2 V−1 s−1. The structure, morphology and optical properties were also evaluated for both N-doped and Zr–N codoped ZnO films. 相似文献
12.
The properties of transparent conducting molybdenum-doped ZnO films grown by radio frequency magnetron sputtering 下载免费PDF全文
Transparent conducting molybdenum-doped zinc oxide films are prepared by radio frequency(RF) magnetron sputtering at ambient temperature.The MoO3 content in the target varies from 0 to 5 wt%,and each film is polycrystalline with a hexagonal structure and a preferred orientation along the c axis.The resistivity first decreases and then increases with the increase in MoO3 content.The lowest resistivity achieved is 9.2 × 10-4.cm,with a high Hall mobility of 30 cm2.V-1.s-1 and a carrier concentration of 2.3×1020 cm-3 at an MoO3 content of 2 wt%.The average transmittance in the visible range is reduced from 91% to 80% with the increase in the MoO3 content in the target. 相似文献
13.
Effects of hydrogen flow on properties of hydrogen doped ZnO thin films prepared by RF magnetron sputtering 总被引:1,自引:0,他引:1
Yuehui Hu Yichuan Chen Jun Chen Xinhua Chen Defu Ma 《Applied Physics A: Materials Science & Processing》2014,114(3):875-882
The hydrogen doped ZnO (ZnO:H) thin films were deposited on quartz glass substrates by radio frequency magnetron sputtering. The doping characteristics of ZnO:H thin films with varied hydrogen flow ratio were investigated. At low hydrogen flow ratio (H2/(H2+Ar)≤0.02), the ZnO:H thin films exhibited dominant (002) peaks from X-ray diffraction and the lattice constants became smaller. The particles were mainly a columnar structure. The particles’ size became smaller, and the island-like structure appeared on the thin films surface. In addition, the low resistivity properties of ZnO:H thin films was ascribed to the increase of the carriers concentration and carriers mobility; When the hydrogen flow ratio was more than 0.02 (M≥0.02), two absorption bands at 1400–1800 cm?1 and 3200–3900 cm?1 were observed from the FT-IR spectra, which indicated that the ZnO:H thin films had typical Zn–H bonding, O–H bonding (hydroxyl), and Zn–H–O bonding (like-hydroxyl). The scanning electron microscope (SEM) results show that a large number of hydroxyl agglomeration formed an island-like structure on the thin films surface. The absorption peak at about 575 cm?1 in the Raman spectra indicated that oxygen vacancies (VO) defects were produced in the process of high hydrogen doping. In this condition, the low resistivity properties of ZnO:H thin films were mainly due to the increasing electron concentration resulted from VO. Meanwhile, the Raman absorption peaks at approximately 98 cm?1 and 436 cm?1 became weaker, and the (002) XRD diffraction peak quenched and the lattice constants increased, which shows that the ZnO:H thin films no longer presented a typical ZnO hexagonal wurtzite structure. With the increasing of hydrogen flow ratio, the optical transmittance of ZnO:H thin films in the ultraviolet band show a clear Burstein–Moss shift effect, which further explained that electron concentration was increased due to the increasing VO with high hydrogen doping concentration. Moreover, the optical reflectance of the thin films decreased, indicating the higher roughness of the films surface. It was noteworthy that etching effect of H plasma was obvious in the process of heavy hydrogen doping. 相似文献
14.
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采用脉冲直流磁控溅射法,以WO3:ZnO陶瓷靶为溅射靶材,通过在溅射气氛中引入H2的方式,在室温条件下制备了低电阻率、高可见和近红外光区透过率的H,W共掺杂ZnO (HWZO)薄膜.系统地研究了H2流量对所制备的HWZO薄膜的结构、组分、元素价态、光电特性的影响.结果表明:掺入的H可促进Zn的氧化,改善薄膜的结晶质量,提高薄膜透过率.H引入之后薄膜的载流子浓度增加,电阻率降低.在H2流量为6mL/min时制备的HWZO薄膜性能最优,电阻率为7.71×10-4 Ω·m,光学带隙为3.58 eV,400-1100 nm的平均透过率为82.4%. 相似文献
16.
Ping Ding Xinhua Pan Zhizhen Ye Haiping He Honghai Zhang Wei Chen Chongyu Zhu Jingyun Huang 《Applied Physics A: Materials Science & Processing》2013,112(4):1051-1055
High-quality ZnO thin films were grown on a-plane sapphire substrates by plasma-assisted molecular beam epitaxy. X-ray diffraction and transmission electron microscopy reveal that the ZnO films have high structural quality and an atomically sharp ZnO/Al2O3 interface. The full width at half maximum values of the 0002 and $30\bar{3}2$ ZnO ω-rocking curves are 467.8 and 813.5 arc sec for a 600 nm thick ZnO film. A screw dislocation density of 4.35×108 cm?2 and an edge dislocation density of 3.38×109 cm?2 are estimated by X-ray diffraction. The surface of the ZnO epilayers contains hexagonal pits, which can be observed in the Zn-polar ZnO. The films have a resistivity of 0.119 Ω?cm, an electron concentration of 6.85×1017 cm?3, and a mobility of 76.5 cm2?V?1?s?1 at room temperature. Low temperature photoluminescence measurements show good optical properties comparable to ZnO single crystals. 相似文献
17.
Q. Q. Fang W. N. Wang J. G. Li Q. Q. Ding C. Wang W. J. Huang H. M. Zhang Q. P. Zhang 《Applied Physics A: Materials Science & Processing》2012,106(4):871-876
The positive temperature coefficient of resistance (PTCR) characteristics of Na2Ti6O13 (NT)-doped 0.94BaTiO3–0.06(Bi0.5Na0.5)TiO3 (BBNT) ceramics were investigated in order to evaluate the effect of NT as a new additive for lead-free PTCR thermistor application.
The BBNT ceramic sintered at 1325°C exhibited a relatively high Curie temperature (T
C
) of 158°C while its PTCR characteristic was not satisfactory for thermistor application. However, doping with NT significantly
influenced the PTCR behavior of BBNT ceramic. It is considered that NT was responsible for grain growth of the BBNT by forming
a liquid phase during sintering due to its low melting temperature of 1300°C. The grain growth resulted in the enhanced PTCR
characteristics of BBNT ceramic. In particular, 0.1 mol% NT doped BBNT ceramic exhibited excellent PTCR performance of low
resistivity at room temperature (1.6×102 Ω cm), resistivity increase near T
C
(1.28×104) and high T
C
of 158°C, suitable for lead-free PTCR thermistor application. 相似文献
18.
采用超声喷雾热分解法在石英衬底上以醋酸锌水溶液为前驱体,以硝酸银水溶液为Ag掺杂源生长了Ag掺杂ZnO(ZnO:Ag)薄膜.研究了衬底温度对所得ZnO:Ag薄膜的晶体结构、电学和光学性质的影响规律.所得ZnO:Ag薄膜结构良好,在室温光致发光谱中检测到很强的近带边紫外发光峰,透射光谱中观测到非常陡峭的紫外吸收截止边和较高的可见光区透过率,表明薄膜具有较高的晶体质量与较好的光学特性.霍尔效应测试表明,在500℃下获得了p型导电的ZnO:Ag薄膜,载流子浓度为5.30×1015cm关键词:
ZnO:Ag薄膜
p型掺杂
超声喷雾热分解
霍尔效应 相似文献
19.
Silver-clad Bi1·7Pb0·4Sr1·8Ca2Cu3·5O
x
(BPSCCO) tapes have been fabricated using low purity (98–99%) starting materials and following the powder-in-tube technique.
MaximumJ
c
values of 6·14 × 103 A·cm−2 at 77 K and 1·4 × 105 A·cm−2 at 4·2 K have been obtained in tapes subjected to the process of intermediate rolling and sintering. The bulk superconducting
material used for the tape-fabrication contains both 2223 and 2212 phases in the ratio 60:40. A pure phase material and the
optimization of the sintering parameters are expected to yield much higherJ
c
values at 77 K. It is possible that the copper-rich phase(s) and/or a small amount of iron impurity (60 ppm) present in CuO
might be acting as flux pinning sites and could be responsible for highJ
c
values. 相似文献
20.