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1.
A simple kinetic model of the Ne-H2 Penning-Plasma Laser (PPL) (NeI 585.3 nm) is proposed. The negative glow of a hollow cathode discharge at intermediate pressures is considered as the active medium. The balance equations for the upper and lower laser levels, electrons, ions and electron energy are solved. The dependences of the laser gain on the discharge conditions (Ne and H2 partial pressures, discharge current) are calculated and measured. The calculated values are in a good agreement with the experimental data.  相似文献   

2.
Continuous-time core-level photon-stimulated desorption (PSD) spectroscopy was used to investigate the monochromatic soft x-ray photoreactions of CF(2)Cl(2) adsorbed on Si(111)-7 × 7 near the F(1s) edge (681-704 eV). Sequential F(+) PSD spectra were observed as a function of photon exposure at the CF(2)Cl(2)-covered surface (dose = 2.0 × 10(14) molecules cm(-2), ~0.75 monolayer). The F(+) PSD and total electron yield (TEY) spectra of solid CF(2)Cl(2) near the F(1s) edge were also measured. Both F(+) PSD and TEY spectra depict three features in the energy range of 687-695 eV, and are assigned to the excitations of F(1s) to (13a(1) + 9b(2))[(C-Cl)(?)], (7b(1) + 14a(1))[(C-F)?] antibonding and 5p Rydberg orbitals, respectively. Following the Auger decay process, two holes are created in the C-F bonding orbitals producing the 2h1e final state which results in the F(+) desorption. This PSD mechanism, responsible for the F(+) PSD of solid CF(2)Cl(2), is used to explain the first F(+) PSD spectrum in the sequential F(+) PSD spectra. The variation of spectral shapes in the sequential F(+) PSD spectra shows the consumption of adsorbed CF(2)Cl(2) molecules and the production of surface SiF species as a function of photon exposure. The photolysis cross section of the adsorbed CF(2)Cl(2) molecules by photons with varying energy (681-704 eV) is deduced from the sequential F(+) PSD spectra and found to be ~6.0 × 10(-18) cm(2).  相似文献   

3.
报道HCl+Xe掺杂CO矩阵晶体中,在308nm激光的激发下,首次观测到准分子Xe+2Cl-的特征辐射荧光谱。双光子诱导电荷转移合作吸收反应:Xe+HCl+2hν→αXe+(HCl)-中,双光子吸收截面大于5×10-42cm4s[6]。  相似文献   

4.
建立了一套针板电极交流放电微等离子发生装置,以氮气作为载气,甲烷为分析气体,放电电压为1.32 kV, 放电距离为3 mm, Pt丝和Pt/MWNT复合纳米粒子修饰FTO电极为放电电极,放电频率为30 kHz,功率消耗为13 W,利用发射光谱法检测放电过程中产生的微等离子体发射光谱,用于在室温下检测甲烷气体。在交流电压下,检测到甲烷的谱线有CH,C2和Hα,以C2谱线作为甲烷分析线,发现C2谱线强度与甲烷浓度在0.5%~4.0%(φ)的范围内呈线性,检出限(S/N=3)为0.19%。以Hα谱线为分析线,Hα谱线强度与甲烷浓度在0.1%~3.0 %(φ)范围内呈线性, 检测限(S /N=3)为0.03%(φ)。对于3.2%的甲烷气体,平行测定11次,在Pt/MWNT/FTO电极上以C2谱线为分析线和以Hα谱线为分析线的相对标准偏差分别为 1.3%和1.9%。说明Pt/MWNT 纳米复合材料修饰电极提高了分析方法的重现性和精密度。以空气混合气体为稀释气体,甲烷气体放电行为与纯氮气中放电行为有较大差异,C2峰消失,只有Hα峰存在。Hα峰强度与甲烷浓度在0.5%~4%范围内有线性相关性。与其他的光发射光谱检测系统相比,该系统装置尺寸小,制备简单且在室温下操作。  相似文献   

5.
 对Cl/HN3/I2产生NCl(a)/I激光的过程进行了化学动力学计算,主要考察了Cl,HN3和I2的初始粒子数密度及其配比对小信号增益系数的影响。结果发现,当温度为400K, 初始Cl粒子数密度为1×1015,1×1016和1×1017cm-3时,小信号增益系数分别达到1.6×10-4,1.1×10-3和1.1×10-2cm-1,获得最佳小信号增益系数的HN3和I2的初始粒子数密度分别为初始Cl粒子数密度的1~2倍和2%~4%。同时,对Cl,HN3和I2配比对小信号增益系数和增益持续时间的影响进行了讨论。  相似文献   

6.
Using a modified ABCD-matrix approach accounting for nonlinear refraction in active medium,the ranges of cavity parameters that provide a mode-locking of Yb∶KYW-laser in usual z-fold cavity configuration are determined.Taking the cavity parameters that provide a most efficient mode locking and based on fluctuation model,a numerical simulation of laser operation is performed.In the calculations the side-band pump power of 6W at 982 nm is used in 1 cm length KYW crystal with 1 cm×0.005 cm beam cross section.Calculations show that self-starting operation is possible with these parameters and dispersion compensation allows for bandwidth-limited ultrashort pulse generation.The shortest pulse duration was determined to be about 200 fs with self-starting buid-up time of 130 μs.Such a built-up time is comparable and even shorter than that one for the lasers with semiconductor saturable absorbers.The region of negative dispersion provided by prism pair for a stable ultrashort pulse generation was determined to be (-17000~-42000)fs2.  相似文献   

7.
 应用遗传算法,以输出激光功率为目标函数,优化确定了普通CO2激光器五种工作气体(CO2, N2, He, Xe, H2)的最佳充气量。对1.2m长谐振腔,在15kV放电条件下,优化的充气量分别为pCO2=1.15×133.3Pa, pN2=7.32×133.3Pa, pHe=12.95×133.3Pa, pXe=0.36×133.3Pa和pH2=0.01×133.3Pa。优化后激光功率比未优化前可提高1.27倍。  相似文献   

8.
We present the characterization of an apparatus generating XUV radiation by a high peak value (20–40) kA and short rise time (≈ 20 ns) current pulse in a capillary discharge channel (up to 20 cm in length) filled by argon gas. The apparatus has been developed with the purpose of production of an intensive spontaneous emission in the spectral region of (2–50) nm and study of the z-pinch conditions for obtaining the laser generation in the Nelike Ar at 46.9 nm. The current pulses are generated by the direct discharge of a 7 nF water dielectric capacitor resonantly charged up to 400 kV by a six-stages Marx generator. The XUV radiation emitted during the radial compression of the plasma column is measured using calibrated PIN diodes, filters and multilayer mirrors in order to test the z-pinch plasma collapse and to measure the conversion efficiency of the electrical energy into the XUV radiation. This work is supported by the Italian National Institute of Nuclear Physics and in part by the Italian National Institute of Matter Physics.  相似文献   

9.
We report on the first generation of 5.5-7.5 MeV protons by a moderate-intensity short-pulse laser (~5×10(17) W/cm(2), 40 fsec) interacting with frozen H(2)O nanometer-size structure droplets (snow nanowires) deposited on a sapphire substrate. In this setup, the laser intensity is locally enhanced by the snow nanowire, leading to high spatial gradients. Accordingly, the nanoplasma is subject to enhanced ponderomotive potential, and confined charge separation is obtained. Electrostatic fields of extremely high intensities are produced over the short scale length, and protons are accelerated to MeV-level energies.  相似文献   

10.
We studied the ionization and dissociation of polyatomic molecule methane in an intense femtosecond laserfield with wavelength of 810 nm and intensities ranging from 1.4×10~(14)to 2.6×10~(15) W/cm~2 by massspeetroscopy.Abundant fragment inos were observed in addition to the strong parent ion.The effect offrequency chirp was investigated and it was found that the negatively chirped pulses dramatically enhancedthe dissociation probability,which might be used to control the dissociation pathways.  相似文献   

11.
利用光学发射谱技术对直流辉光放电等离子体增强的化学气相沉积氮化碳薄膜过程中的等离子体进行了原位诊断,结果表明主要的辐射有N2的第二正系跃迁、N2^ 的第一负系跃迁、CN和NH的紫外跃迁。研究了气源中氢气含量、放电电流及沉积气压的变化对N2(337.1nm),N2^ (391.4nm)和CN(388.3nm)辐射强度的影响,并在此基础上探讨了这几种跃迁的激发机制,其结果为氮化碳合成中优化沉积参数、控制实验过程提供了依据。  相似文献   

12.
本文报道国内建成的远红外激光磁共振 (FIRLMR)光谱仪的技术特点和工作原理。该谱仪采用CO2 激光横向泵浦远红外激光 ,样品吸收池置于远红外激光谐振腔内 ,由聚丙烯薄膜与远红外激光增益池隔开以获得很高的灵敏度 ,从而对寿命很短的自由基分子进行研究。利用该光谱仪在远红外波段测量得到了多个瞬态自由基分子CCH ,CF和CH2 的光谱 ,这些自由基分子由微波放电产生的氟原子与甲烷CH4 反应生成。  相似文献   

13.
Using a laser interferometric technique changes in the refractive index at 633 nm of the pulsed discharge of a TEA CO2-N2-He laser amplifier have been observed. Heating of the medium by the discharge reduces the density and hence the refractive index of the gas. The peak temperature was found to be reached between 0.15 and 0.25 msec after the current pulse. For values of voltage and pressure typical for 10.6 μm laser operation a temperature of ~430 K was measured. The system returned to thermal equilibrium after 23 and 27 msec. Thermal diffusion time calculations indicate that the heating is confined to within 3 to 4 mm of the central axis.  相似文献   

14.
High-resolution (Deltavarsigma = 2.3 and 2.9 x 10(-3) cm(-1)) FTIR spectra of natural and (35)Cl monoisotopic CH(3)CF(2)Cl have been recorded at -70 degrees C in the 600-1400 cm(-1) range. The bands nu(7), nu(8), and nu(15) have been rotationally analyzed for both isotopic varieties. With the help of predictions based on nu(8) parameters, the millimeter-wave spectrum of the (35)Cl species in the v(8) = 1 state has been observed and jointly fitted with the IR data. Only a small number of local perturbations have been detected in the spectra. Altogether more than 8000 IR transitions have been fitted with an experimental precision of ca. 3 x 10(-4) cm(-1). Copyright 2000 Academic Press.  相似文献   

15.
Z Hu  Z Li  L Zhu  F Liu  Y Lv  X Zhang  Y Wang 《Optics letters》2012,37(15):3072-3074
An ultraviolet photodetector was fabricated based on Mg0.07Zn0.93O heterojunction. N, N'-bis (naphthalen-1-y1)-N, N'-bis(pheny) benzidine was selected as the hole transporting layer. I-V characteristic curves of the device were measured in the dark and under the illumination of 340?nm UV light with density of 1.33 mW/cm2. The device showed a low dark current of about 3×10-10 A and a high photo-dark current ratio of 1×105 at -2 V bias. A narrowband photoresponse was observed from 300 to 400?nm and centered at 340?nm with a full width at half-maximum of only 30?nm. The maximum peak response is at 340?nm, which is 0.192 A/W at the bias of -1 V.  相似文献   

16.
Chen JM  Lu KT 《Physical review letters》2001,86(14):3176-3179
State-specific desorption for SiCl4 adsorbed on a Si(100) surface at approximately 90 K with variable coverage following the Cl 2p and Si 2p core-level excitations has been investigated using synchrotron radiation. The Cl+ yields show a significant enhancement following the Cl 2p-->8a*1 excitation. The Cl- yields are notably enhanced at the 8a*1 resonance at both Cl 2p and Si 2p edges. The enhancement of the Cl- yield occurs through the formation of highly excited states of the adsorbed molecules. These results provide some new dissociation processes from adsorbates on surfaces via core-level excitation.  相似文献   

17.
激光烧蚀Al热原子与CF4,CCl4,CH2Br2反应中激发态C2的形成   总被引:1,自引:1,他引:0  
脉冲激光烧蚀平面铝靶产生的热原子与气相CF4,CCl4,CH2Br2的碰撞反应中,在430~600nm之间观测到激发态C2分子的发光光谱,它们可归属为Swan带的d^3Ⅱg=a^3Ⅱu跃迁中△v=2,1,0,-1,-2五个振动序列(v′≤6)。谱强度分析表明,C2激发态可很好的用热平衡描述,其振动温度达6000K左右。同时在△v=0和-1的振动带间观测到振荡的谱峰,它们是转动谱线叠加的结果。激光烧蚀Al产生的等离子体在膨胀中产生的激波及其本身的动能与反应气体碰撞使其解离产生C,然后复合形成C2。C2激发态d可能是通过激发态的Al(^2S)经近共振传能产生,也不排除在有足够碰撞能下优先形成C2激发态b,再通过与d态的v′=6能级交叉无辐射跃迁而进入d态。  相似文献   

18.
横流CWCO2激光器电子密度的研究   总被引:2,自引:1,他引:1  
毛英立  程兆谷 《光学学报》1990,10(2):19-123
用Langmuir静电探针测量5kW横流CO_2激光器放电等离子体,根据P.R.Smy流动等离子体厚鞘理论进行分析,表明在工作气压力为42Torr、放电电流为10~20A的情况下,电子密度约为(1.7~3.1)x10~(11)cm~(-3)的范围内,并沿流向成非均匀分布,其极大值出现在距阳极板上游边沿3cm处.电子的连续性方程给实验结果以解释,理论与实验较好地符合.  相似文献   

19.
Yi H  Liu K  Chen W  Tan T  Wang L  Gao X 《Optics letters》2011,36(4):481-483
We applied for the first time, to our knowledge, broadband off-beam quartz-enhanced photoacoustic spectroscopy (BB-OB-QEPAS) to trace NO2 detection using a broadband blue laser diode centered at 450?nm. A detection limit of 18?ppbv (parts in 10(9) by volume) for NO2 in N2 at atmospheric pressure was achieved with an average laser power of 7?mW at a 1?s integration time, which corresponds to a 1?σ normalized noise equivalent absorption coefficient of 4.1×10(-9) cm(-1)?W=Hz(1=2). An Allan variance analysis was performed to investigate the long-term stability of the BB-OB-QEPAS-based NO2 sensor.  相似文献   

20.
利用介质阻挡放电实验系统测量了空气介质阻挡放电的发射光谱,研究了氩气含量对空气介质阻挡放电发射光谱的影响.在280~500 nm波长范嗣内,发现了氮分子第二正带系N2(C3∏u-B3∏g)的谱线和氮分子离子的第一负带系N2+(B3∑u+-X2∑g+)的谱线.在相同条件下加入10%氩气后,起始放电电压由26kV降低到23...  相似文献   

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