共查询到20条相似文献,搜索用时 62 毫秒
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一、引言用~(60)Co源γ射线辐照的LiF晶体,不仅是一种激光材料,而且也是一种良好的被动调Q元件。F_2~-心在室温下很稳定,长期放置不易褪色。随辐照剂量和原材料中杂质成分不同,一般F_2~-心寿命可达3~8年。LiF:F_L~-心晶体被动Q开关,与常用KDP和LiNbO_3等晶体主动开关相比,不需要复杂的供电电源,不存在KDP的潮解现象,插入损耗低,操作简单,导热性高,加工简便,抗损伤阈值高,毫微秒脉冲可达40GW/cm~2和成本低廉等。使用时只需放入谐振腔内即可。和五甲川染料相 相似文献
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众所周知,用γ射线辐照的纯LiF晶体,会产生各种类型的色心——F,F_2,F_2~ 和F_2~-等。其中F_2、F_2~ 和F_2~-具有类似的四能级结构,并已产生可调谐的激光输出。 相似文献
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在近红外光谱区,将脉冲固体激光辐射转变成可调谐辐射的效率大大提高的途经之一是采用新型的激活介质。尤其是,具有辐照色心的碱卤晶体乃是这种激活介质。这种介质具有广阔的实际应用前景与LiF:F_2~ 和LiF:F_2~-晶体室温下振荡辐射有关。这种介质激光器可以连续地复盖0.84~1.15μm(F_2~ )和1.08~1.26μm(F_2~-)光谱区。迄今为止,都是采用型工业用激光器作为色心晶体激光器的泵浦源。在此情况下LiF:F_2~-晶体激光器的振荡能量于非选择腔 相似文献
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众所周知,含有色心的碱卤晶体是实现可调谐激光的重要固体工作物质。LiF晶体则是这类材料中具有突出优点的一种。首先,LiF晶体中的色心在室温下有较高的荧光量子效率,故可在室温下实现激光振荡,这对很多实际应用无疑有着重要意义。其次,LiF晶体在空气中放置不易潮解,这就不必来用额外的防潮措施。第三,LiF晶体有高的热导率(0.103W/cm.℃)及高的破坏阈值(在1.06μm处为20GW/cm~2),这很适合用在高功率或高重复频率激光系统中。到目前为止,LiF晶体中的F_2、F_2~ 及F_2~-心均已获得可调谐激光振荡。 相似文献
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Wei-Chou Hsu Dong-Hai Huang Yu-Shyan Lin Yeong-Jia Chen Jun-Chin Huang Chang-Luen Wu 《Electron Devices, IEEE Transactions on》2006,53(3):406-412
This paper proposes a In/sub 0.5/Al/sub 0.5/As/In/sub x/Ga/sub 1-x/As/In/sub 0.5/Al/sub 0.5/As (x=0.3-0.5-0.3) metamorphic high-electron mobility transistor with tensile-strained channel. The tensile-strained channel structure exhibits significant improvements in dc and RF characteristics, including extrinsic transconductance, current driving capability, thermal stability, unity-gain cutoff frequency, maximum oscillation frequency, output power, power gain, and power added efficiency. 相似文献
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《Electronics letters》1990,26(1):27-28
AlGaAs/GaInAs/GaAs pseudomorphic HEMTs with an InAs mole fraction as high as 35% in the channel has been successfully fabricated. The device exhibits a maximum extrinsic transconductance of 700 mS/mm. At 18 GHz, a minimum noise figure of 0.55 dB with 15.0 dB associated gain was measured. At 60 GHz, a minimum noise figure as low as 1.6 dB with 7.6 dB associated gain was also obtained. This is the best noise performance yet reported for GaAs-based HEMTs.<> 相似文献
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A 12 /spl times/ 12 In/sub 0.53/Ga/sub 0.47/As-In/sub 0.52/Al/sub 0.48/As avalanche photodiode array
Zheng X.G. Hsu J.S. Sun X. Hurst J.B. Li X. Wang S. Holmes A.L.Jr. Campbell J.C. Huntington A.S. Coldren L.A. 《Quantum Electronics, IEEE Journal of》2002,38(11):1536-1540
We report a 12 /spl times/ 12 In/sub 0.53/Ga/sub 0.47/As-In/sub 0.52/Al/sub 0.48/As avalanche photodiode (APD) array. The mean breakdown voltage of the APD was 57.9 V and the standard deviation was less than 0.1 V. The mean dark current was /spl sim/2 and /spl sim/300 nA, and the standard deviation was /spl sim/0.19 and /spl sim/60 nA at unity gain (V/sub bias/ = 13.5 V) and at 90% of the breakdown voltage, respectively. External quantum efficiency was above 40% in the wavelength range from 1.0 to 1.6 /spl mu/m. It was /spl sim/57% and /spl sim/45% at 1.3 and 1.55 /spl mu/m, respectively. A bandwidth of 13 GHz was achieved at low gain. 相似文献
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S. Privitera F. Wang P. Dumont-Girard K. Liu C. Bongiorno 《Microelectronic Engineering》2010,87(3):430-433
SixCryCzBv thin films with several compositions have been studied for integration of high precision resistors in 0.8 μm BICMOS technology. These resistors, integrated in the back-end of line, have the advantage to provide high level of integration and attractive electrical behavior in temperature, for analog devices. The film morphology and the structure have been investigated through transmission electron microscopy analysis and have been then related to the electrical properties on the base of the percolation theory. According to this theory, and in agreement with experimental results, negative thermal coefficient of resistance (TCR) has been obtained for samples with low Cr content, corresponding to a crystalline volume fraction below the percolation threshold.Samples with higher Cr content exhibit, instead, a variation of the TCR as a function of film thickness: negative TCR values are obtained for thickness lower than 5 nm, corresponding to a crystalline volume fraction below the percolation threshold; positive TCR are obtained for larger thickness, indicating the establishment of a continuous conductive path between the Cr rich grains. This property seems to be determinant in order to assure the possibility to obtain thin film resistors almost independent on the temperature. 相似文献
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Yi-Jen Chan Ming-Ta Yang 《Electron Devices, IEEE Transactions on》1995,42(10):1745-1749
The properties of both lattice-matched and strained doped-channel field-effect transistors (DCFET's) have been investigated in AlGaAs/In/sub x/Ga/sub 1-x/As (0/spl les/x/spl les/0.25) heterostructures with various indium mole fractions. Through electrical characterization of grown layers in conjunction with the dc and microwave device characteristics, we observed that the introduction of a 150-/spl Aring/ thick strained In/sub 0.15/Ga/sub 0.85/As channel can enhance device performance, compared to the lattice-matched one. However, a degradation of device performance was observed for larger indium mole fractions, up to x=0.25, which is associated with strain relaxation in this highly strained channel. DCFET's also preserved a more reliable performance after biased-stress testings.<> 相似文献
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Jie Liu Yugang Zhou Rongming Chu Yong Cai Chen K.J. Lau K.M. 《Electron Device Letters, IEEE》2005,26(3):145-147
We report an Al/sub 0.3/Ga/sub 0.7/N-Al/sub 0.05/Ga/sub 0.95/N-GaN composite-channel HEMT with enhanced linearity. By engineering the channel region, i.e., inserting a 6-nm-thick AlGaN layer with 5% Al composition in the channel region, a composite-channel HEMT was demonstrated. Transconductance and cutoff frequencies of a 1 /spl times/100 /spl mu/m HEMT are kept near their peak values throughout the low- and high-current operating levels, a desirable feature for linear power amplifiers. The composite-channel HEMT exhibits a peak transconductance of 150 mS/mm, a peak current gain cutoff frequency (f/sub T/) of 12 GHz and a peak power gain cutoff frequency (f/sub max/) of 30 GHz. For devices grown on sapphire substrate, maximum power density of 3.38 W/mm, power-added efficiency of 45% are obtained at 2 GHz. The output third-order intercept point (OIP3) is 33.2 dBm from two-tone measurement at 2 GHz. 相似文献
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Patrick W. C. Ho Firas Odai Hatem Haider Abbas F. Almuri T. Nandha Kumar 《半导体学报》2016,37(6):064001-13
Nonvolatile memories have emerged in recent years and have become a leading candidate towards replacing dynamic and static random-access memory devices. In this article, the performances of TiO2 and TaO2 nonvolatile memristive devices were compared and the factors that make TaO2 memristive devices better than TiO2 memristive devices were studied. TaO2 memristive devices have shown better endurance performances (108 times more switching cycles) and faster switching speed (5 times) than TiO2 memristive devices. Electroforming of TaO2 memristive devices requires~4.5 times less energy than TiO2 memristive devices of a similar size. The retention period of TaO2 memristive devices is expected to exceed 10 years with sufficient experimental evidence. In addition to comparing device performances, this article also explains the differences in physical device structure, switching mechanism, and resistance switching performances of TiO2 and TaO2 memristive devices. This article summarizes the reasons that give TaO2 memristive devices the advantage over TiO2 memristive devices, in terms of electroformation, switching speed, and endurance. 相似文献
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Zhiqun Cheng Jie Liu Yugang Zhou Yong Cai Chen K.J. Lau K.M. 《Electron Device Letters, IEEE》2005,26(8):521-523
We report broadband microwave noise characteristics of a high-linearity composite-channel HEMT (CC-HEMT). Owing to the novel composite-channel design, the CC-HEMT exhibits high gain and high linearity such as an output third-order intercept point (OIP3) of 33.2 dBm at 2 GHz. The CC-HEMT also exhibits excellent microwave noise performance. For 1-/spl mu/m gate-length devices, a minimum noise figure (NF/sub min/) of 0.7 dB and an associated gain (G/sub a/) of 19 dB were observed at 1 GHz, and an (NF/sub mi/) of 3.3 dB and a G/sub a/ of 10.8 dB were observed at 10 GHz. The dependence of the noise characteristics on the physical design parameters, such as the gate-source and gate-drain spacing, is also presented. 相似文献