用PECVD法在金属衬底上沉积氮化硅薄膜

采用等离子体增强化学气相沉积（ＰＥＣＶＤ）方法在４０Ｃｒ钢（含Ｃｒ０．８％～１．１％）或铜等金属基片上沉积氨化硅薄膜。沉积温度为２５０℃时，制备的薄膜厚度为０．２～０．４μｍ，电阻率为８×１０￣（１６）Ω·ｃｍ，介质击穿场强达到１×１０￣７Ｖ／ｃｍ。用ＸＰＳ谱研究了薄膜的结构和成分，并分析了沉积时不同的工艺参数对薄膜绝缘耐压性能的影响。     

ArF准分子激光立方氮化硼薄膜的制备

采用ＡｒＦ准分子脉冲激光沉积方法（ＰＬＤ），以六方氮化硼（ｈ－ＢＮ）作靶在Ｓｉ（１００）衬底上制备氮化硼薄膜。ＸＲＤ及ＦＴＩＲ透射谱测量表明生成的氮化硼薄膜是含有少量六方氮化硼结构的立方氮化硼（Ｃ－ＢＮ）．ＡＥＳ测量表明不同条件下生成的薄膜中Ｎ与Ｂ的相对含量是不同的，最大比例近乎为１：１，薄膜的维氏显微硬度ＨＶ最大值为１５８０ｋｇ／ｍｍ２。     

γ-Al_2O_3/Si(100)薄膜高真空MOCVD异质外延生长

本文作者在自己组装的立式ＭＯＣＶＤ设备上，成功地应用高真空生长技术，于１０５０℃的高温条件下，在硅上外延生长了γ－Ａｌ２Ｏ３薄膜．从ＲＨＥＥＤ看到（１００）硅上生长的薄膜是（１００）立方单晶γ－Ａｌ２Ｏ３的衍射图样；平移样品，图样并不发生变化．Ｘ射线双晶衍射看到，除了硅的（４００）峰和（２００）峰以外，只在２θ为４５°处有一个低而宽的小峰．ＸＰＳ谱给出氧的１ｓ峰位为５３２．３ｅＶ，Ａｌ的２ｐ峰位为７５．４ｅＶ，将他们与α－Ａｌ２Ｏ３比较，对应峰位移动了约３．５ｅＶ．俄歇谱说明其铝氧组分比近于γ－Ａｌ２Ｏ３     

CdS多晶薄膜的电学性质

用化学池沉积方法（ＣＢＤ）制备了ＣｄＳ多晶薄膜，并对薄膜进行了退火处理，测量了不同ＣｄＳ薄膜光电导、暗电导和电导－温度关系，计算了电导激光活能。结果表明：刚沉积的ＣｄＳ暗电导率为１０＾－６Ω＾－１．ｃｍ＾－１比光电导率低二个数量级，退火后，电导升高，电导激活能减小。Ｘ射线衍射分析表明，经退火后，ＣｄＳ薄膜发生相变，由立方结构变成六方结构。对上述结果进行了讨论。     

YBCO薄膜红外探测器研究的新进展

用ＹＢＣＯ／ＬａＡｌＯ＿３薄膜制成的１ｍｍ红外探测器，经技术保护之后，寿命已达３年。其Ｄ（５００，１０，１）＝３．７×１０￣９ｃｍＨｚ￣（１／２）Ｗ￣（－１），ＮＥＰ（５００，１０，１）＝２．４×１０￣（－１１）ＷＨｚ￣（－１／２）；超导微桥（５０μｍ×１０μｍ）红外探测器，其Ｄ（５００，１０，１）＝１×１０￣９ｃｍＨｚ￣（１／２）Ｗ￣（－１），ＮＥＰ（５００，１０，１）＝２．３×１０￣（－１２）ＷＨｚ￣（－１／２）。     

纳米硅薄膜结构特性研究

在电容式耦合等离子体化学气相沉积系统中，使用高氢稀释硅烷为反应气体制备出了晶粒尺寸为２～１０ｎｍ的纳米微晶相结构的硅薄膜，使用高分辨电子显微镜（ＨＲＥＭ），Ｘ射线衍射谱（ＸＲＤ），Ｘ射线光电子能谱（ＸＰＳ）和红外光谱（ＩＲ）等结构分析手段检测了其结构特征．结果表明，纳米硅薄膜的晶格结构为畸变的金刚石结构．Ｘ射线衍射谱表明除了Ｓｉ（１１１）的２θ＝２８．５°和Ｓｉ（２２０）的２θ＝４７．３°处的衍射峰外，在２θ＝３２．５°处存在着一个强的异常峰．ＨＲＥＭ结果表明存在新的Ｓｉ结晶学结构与ＸＲＤ异常峰相关联．     

ECR－PECVD制备Si_3N_4薄膜的特性及其应用的研究

本文利用ＥＣＲ－ＰＥＣＶＤ技术在不同沉积温度下制备了Ｓｉ３Ｎ４薄膜，利用Ｓｉ３Ｎ４薄膜的透射光强度曲线计算了Ｓｉ３Ｎ４薄膜的折射率和膜厚，计算结果与实测值符合较好。结果表明，随着沉积温度的提高，Ｓｉ３Ｎ４薄膜的折射率增大，致密性提高，Ｓｉ３Ｎ４薄膜厚度在６０ｍｍ直径范围内不均匀度小于５％。测定了Ｓｉ３Ｎ４薄膜的显微硬度。利用荧光分光光度计测定了Ｓｉ３Ｎ４薄膜的光致发光效应。初步进行了Ｓｉ３Ｎ４薄膜的超高频大功率晶体管器件中作为钝化膜的应用研究。     

复合物p—C6H4F2...NH3（ND3）外部振动的共振双光子电离光谱

利用共振光电离技术和飞行时间质谱技术,观察到了复合物ｐ－Ｃ６Ｈ４Ｆ２．．．ＮＨ３（ＮＤ３）的共振双光子电离光谱。光谱分析表明,复合物分子间的伸 振动频率为８６．４ｃｍ＾－１;由复合物光解离机理以及伸缩模的失谐参数与键有的关系。获得了复合物电子激发态Ｓ１和基态Ｓ０的键能信息。Ａｂｉｎｉｔｉｏ计算表明,ｐ－Ｃ６Ｈ４Ｆ２．．．ＮＨ３（ＮＤ）复合物的几何结构是：ＮＨ３分子中的Ｎ原子位于垂直ｐ－Ｃ６Ｈ４Ｆ２     

用XPS对CdTe（111）面进行化学特性分析

用ＸＰＳ化学位移和定量分析方法，研究了露于室温空气中的ＣｄＴｅ（１１１）面的化学特征。首次报道了经机械抛光表面上形成的表面化合物为ＴｅＯ２（Ｔｅ３ｄ５／２５７５．８ｅＶ，Ｏ１ｓ５３０．１ｅＶ）和Ｃｄ（ＯＨ）２（Ｃｄ３ｄ５／２４０５１ｅＶ．Ｏ１ｓ５３１．４ｅＶ）。并与基体里的ＣｄＴｅ共存；经２％Ｂｒ－乙醇溶液化学抛光，表面上形成的化合物为ＣｄＴｅＯ４（Ｃｄ３ｄ５／２４０５．３ｅＶ，Ｔｅ３ｄ５／２５７６５ｅＶ，Ｏ１ｓ５３１．２ｅＶ）和ＴｅＯｘ（ｘ＜１）（Ｔｅ３ｄ５／２５７４～５７５ｅＶ，Ｏ１ｓ５２８１ｅＶ），并且ＸＰＳ谱中没有基体里的ＣｄＴｅ的特征，其中ＴｅＯＸ为Ｔｅ氧化物的过渡态。结果表明，在相同氧化环境中，表面上形成的化合物强烈依赖表面状况。     

ECR—PECVD制备Si3N4薄膜的特性及其应用的研究

本文利用ＥＣＲ－ＰＥＣＶＤ技术在不同沉积温度下制备了Ｓｉ３Ｎ４薄膜，利用Ｓｉ３Ｎ４薄膜的透射光学强度曲线计算了Ｓｉ３Ｎ４薄膜的折射率和膜厚，计算结果与实测值符合较好。结果表明，随着帝积温度的提高，Ｓｉ３Ｎ４薄膜的折射率增大，致密性提高，Ｓｉ３Ｎ４薄膜厚度在６０ｍｍ直径范围内不均匀度小于５％，测定了Ｓｉ３Ｎ４薄膜的显微硬度，利用荧光分光光度计测定了Ｓｉ３Ｎ４薄膜的光致发光效应，初步进行了Ｓｉ３Ｎ４薄     

In0.52Al0.48As/In0.53Ga0.47As/In0.52Al0.48As abrupt double-heterojunction bipolar transistors

In0.52Al0.48As/In0.53Ga0.47As/In0.52Al0.48As n-p-n abrupt double-heterojunction bipolar transistors grown by molecular beam epitaxy (MBE) have been realized for the first time. DC current gains in excess of 300 have been measured on devices operated in the emitter-up configuration. DC current gains around 50 are obtained on device structures with Be+ implanted extrinsic base regions operated in the emitter-down configuration. The carrier injection and collection behavior of the abrupt InGaAs/InAlAs heterojunctions is discussed.     

Characteristics of metal-ferroelectric-insulator-semiconductor structure using Sr0.8Bi2.2Ta2O9 and Sr0.8Bi2.2Ta2O9-BaZrO3 for ferroelectric gates

Characteristics of BaZrO₃ (BZO) modified Sr_0.8Bi_2.2Ta₂O₉ (SBT) thin films fabricated by sol-gel method on HfO₂ coated Si substrates have been investigated in a metal-ferroelectric-insulator-semiconductor (MFIS) structure for potential use in a ferroelectric field effect transistor (FeFET) type memory. MFIS structures consisting of pure SBT and doped with 5 and 7 mol% BZO exhibited memory windows of 0.81, 0.82 and 0.95 V with gate voltage sweeps between −5 and +5 V, respectively. Leakage current density levels of 10⁻⁸ A/cm² for BZO doped SBT gate materials were observed and attributed to the metallic Bi on the surface as well as intrinsic defects and a porous film microstructure. The higher than expected leakage current is attributed to electron trapping/de-trapping, which reduces the data retention time and memory window. Further process improvements are expected to enhance the electronic properties of doped SBT for FeFET.     

Beat-frequency between measurements between C12O216and C12O218lasers

Several beat frequencies in the range below 6 GHz have been measured using a C¹²O2¹⁶laser and a C¹²O2¹⁸laser operating on several pairs of closely spaced lines in the 9.3-μm region.     

Some new FIR laser lines of optically pumped12CH316OH,12CH316OD, and12CH3I,12CH3Br,12CD2Cl2absorption spectroscopy of water and acetonitrile

The wavelength, polarization, and output power of several lines of the optically pumped CW FIR¹²CH3¹⁶OH (methanol) and¹²CH3¹⁶OD (1-D deuterated methanol), methyl iodide, methyl bromide, and deuterated methylene chloride lasers have been determined. In addition to lines already reported in the literature, seven strong lines have been observed. Optimum performance of the laser system is achieved by means of an improved coupling of the CO2pump power into the resonator and extraction of the FIR power from the resonator. Measurements on the power absorption coefficient of water using the laser indicate thatalpha(bar{nu})rises to almost 1100 Np ċ cm^-1at 170 cm^-1, and then shows a gradual fall with an increase in frequency. A strong temperature dependence of the 200 cm^-1peak inalpha(bar{nu})is predicted, with a decrease in the frequency of maximum power absorption coefficient with an increase in temperature. The range of measurements for acetonitrile is extended to lower frequencies so as to overlap with those determined from other millimeter wave techniques. For highly power-absorbing liquids,alpha(bar{nu})is estimated to be within ± 5 percent.     

Laser4F3/2→4I9/2and4F3/2→4I13/2transitions in KY(WO4)2:Nd3+

We report the observation of lasing at 0.9137 μm and 1.3545 μm in neodymium-doped KY(WO4)2at 77 K. Transition cross sections, fluorescent line width, and branching ratios are given.     

Al0.25In0.75P/Al0.48In0.52As/Ga0.35In 0.65As graded channelpseudomorphic HEMT's with high channel-breakdown voltage

A new Al_0.25In_0.75P/Al_0.48In_0.52 As/Ga_0.35In 0_.65As pseudomorphic HEMT where the InAs mole fraction of the Ga_1-xIn_xAs channel was graded (x=0.53→0.65→0.53) is described. The modification of the quantum well channel significantly improved breakdown characteristics. In addition, use of an Al_0.25In_0.75P Schottky layer increased the Schottky barrier height. Devices having 0.5 μm gate-length showed g_m of 520 mS/mm and I_max of 700 mA/mm. The gate-drain (BV_g-d) and source-drain (BV_d-s ) breakdown voltages were as high as -14 and 13 V, respectively. An f_T of 70 GHz and f_max of 90 GHz were obtained     

选频~(14)CO_2-~(12)CO_2同位素激光器

我们研制了一台~(14)CO_2-~(12)CO_2同位素激光器,测量到激光谱线80条,其中40条是~(14)CO_200°1-(10°0,02°0)_I带的激光跃迁谱线,强线输出功率达4.0W以上;实验还观察到同位素的竞争效应,发现即使~(14)CO_2成份低于~(12)CO_2,其激光辐射仍占优势.     

Waveguide In0.53Ga0.47As-In0.52Al0.48As avalanche photodiode

A high-speed waveguide In_0.53Ga_0.47As-In_0.52Al_0.48 As separate absorption, charge, and multiplication avalanche photodiode suitable for operation at 1.55 μm has been demonstrated, a unity-gain bandwidth of 27 GHz was achieved with a gain-bandwidth product of 120 GHz     

An In0.52Al0.48As/n+-In0.53Ga0.47As MISFET with a modulation-doped channel

A heterostructure metal-insulator-semiconductor field-effect transistor (MISFET) with a modulation-doped channel is proposed. In this device, a very thin undoped subchannel is located between the undoped wide-bandgap insulator and a thin heavily doped channel. In the depletion mode of operation, electron transport takes place along the heavily doped channel. When the device enters the accumulation mode of operation, electrons pile up against the heterointerface in the high-mobility undoped subchannel. This results in markedly improved transport characteristics at the onset of accumulation. The concept is demonstrated in the In_0.52Al_0.48As/In_0.53 Ga_0.47As system on InP. A 1.5-μm-gate-length MISFET shows a unity current-gain cutoff frequency of 37 GHz     

Temporal stability of circulating current in thin film Tl2Ba2CaCu2O8 and YBa2Cu3O7

The temporal stability of trapped transport current in annular thin film Tl₂Ba₂CaCu₂O₈ (TBCCO) and YBa₂Cu₃O₇ (YBCO) wafers has been accurately measured and has been found to be of suitable quality for the stringent requirements of nuclear magnetic resonance (NMR) magnets. No detectable decay, to the limit of the experimental apparatus (2*10^-14 Ω), was detected in those wafers with transport current at or below the critical current density J_c. The critical current density, as previously determined from 12 μm meander lines, was confirmed in a wafer with a width of 1.9 cm. The profile of trapped magnetic field resulting from induced current was modeled in order to assess its effect on the uniformity of an NMR magnet