共查询到17条相似文献,搜索用时 156 毫秒
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利用飞行时间谱,研究了在飞秒强激光场(60 fs,2×1016 W/cm2)作用下,大尺寸氩原子团簇Arn(n—=3×103—3×106原子/每团簇)的电离爆炸过程,测量了 团簇爆炸所产生的氩离子的平均能量与团簇尺寸(气体背压)的关系.实验发现,随着气体 背压的升高(团簇尺寸增大),氩离子的平均能量也相应升高.通过分析两个不同几何尺寸 锥形超声喷嘴所产生团簇爆炸后的离子能量,结合Hagena团簇尺寸规律,发现在激光参数保 持不变的情况下,离子的平均能量由团簇尺寸唯一确定.分析表明,团簇尺寸在3×105原 子/每团簇以下时,团簇膨胀的主要机理是库仑爆炸.随着团簇尺寸的进一步增大,团簇膨胀 机理将由库仑爆炸向流体动力学膨胀过渡,在3×105关键词:
原子团簇
飞秒强激光
库仑爆炸
流体动力学膨胀 相似文献
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本文通过对高背压(50 bar, 1 bar = 1.0×105 Pa)氩气经长锥型喷嘴(长度L=30 mm)向真空绝热膨胀所形成的超声气体团簇喷流的数值模拟, 分析比较了由喷嘴喉口起沿喷流方向在喷流中心轴线上团簇平均尺寸的演化情况. 结果表明: 沿喷流方向团簇平均尺寸显示先增长后趋于饱和的变化趋势, 具有较大尺寸团簇的区域出现在距离喷嘴喉口大约20 mm. 据此本文再结合关于喷流中原子密度沿喷流方向变化的模拟结果开展了锥形喷嘴长度的优化研究. 针对由常见构型的锥形喷嘴(喉径~ 0.5 mm, 半张角~ 8.5°)在高背压下形成的团簇喷流, 20 mm左右的长度为锥形喷嘴的适宜长度. 相似文献
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具有液氮温度和适度压强的氢气通过S99阀门Laval喷嘴进入真空,经超声绝热膨胀形成团簇。本实验用瑞利散射法测量氢团簇尺寸随阀门背压强的变化曲线。当背压为1.0MPa时,每个氢团簇平均包含250个氢原子。 相似文献
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利用瑞利散射方法研究了超声喷流Ar-CH4混合团簇和超声喷流Ar-H2混合团簇的特性.通过测量不同混合比例和不同背压下所形成混合团簇的散射信号发现,当用Ar气和CH4的混合气体进行超声喷流时很容易形成Ar-CH4混合团簇,当Ar气含量为50%时混合团簇尺度最大且大于相同气压下纯Ar团簇尺度和纯CH4团簇尺度.实验发现,与纯H2团簇只能在低温条件下获得不同,常温下即可形成Ar-H2混合团簇,实现了常温下含氢团簇的获取,从而有效降低了制备成本.在H2含量大于40%时混合团簇开始形成并在60%时达到最大尺度.含氢(氘)混合团簇在氢(氘)团簇的基础上引入了更重的异核Ar元素,在激光氘团簇聚变实验中它将进一步加速氘离子从而获得更高的能量,并具有更高的中子产额和聚变效率. 相似文献
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根据超声膨胀原理,n(10-10^4)个气体原子可以绝热冷却后凝聚在一起形成团簇,经过离化后,形成带一个电荷量的团簇离子,比如Arn^+.当团簇离子与固体材料相互作用时,由于平均每个原子携带的能量(~eV)较低,仅作用于材料浅表面区域,因此,气体团簇离子束是材料表面改性的优良选择.本文介绍了一台由武汉大学加速器实验室自主研制的气体团簇离子束装置,包括整体构造、工作原理及实验应用.中性团簇束由金属锥形喷嘴(F=65-135μm,q=14°)形成,平均尺寸为3000 atoms/cluster,经离化后,其离子束流达到了50μA.Ar团簇离子因其反应活性较低,本文运用Ar团簇离子(平均尺寸为1000 atoms/cluster)进行了平坦化和自组装纳米结构的研究.单晶硅片经Ar团簇离子束处理后,均方根粗糙度由初始的1.92 nm降低到0.5 nm,同时观察到了束流的清洁效应.利用Ar团簇离子束的倾斜(30°-60°)轰击,在宽大平坦的单晶ZnO基片上形成了纳米波纹,而在ZnO纳米棒表面则形成了有序的纳米台阶,同时,利用二维功率谱密度函数分析了纳米结构在基片上的表面形貌和特征分布,并计算了纳米波纹的尺寸和数量. 相似文献
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An Experimental Observation of Axial Variation of Average Size of Methane Clusters in a Gas Jet 下载免费PDF全文
Axial variation of average size of methane clusters in a gas jet produced by supersonic expansion of methane through a cylindrical nozzle of 0.8 mm in diameter is observed using a Rayleigh scattering method. The scattered light intensity exhibits a power scaling on the backing pressure ranging from 16 to 50bar, and the power is strongly Z dependent varying from 8.4 (Z = 3mm) to 5.4 (Z = 11mm), which is much larger than that of the argon cluster. The scattered light intensity versus axial position shows that the position of 5mm has the maximum signal intensity. The estimation of the average cluster size on axial position Z indicates that the cluster growth process goes forward until the maximum average cluster size is reached at Z - 9 mm, and the average cluster size will decrease gradually for Z 〉 9 mm. 相似文献
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The energy absorption efficiency of high-intensity (~10^{16}W/cm^2) femtosecond laser pulses in a dense jet of large rare-gas clusters has been measured. Experimental results show that the energy absorption efficiency is strongly dependent on the cluster size and can be higher than 90%. The measurement of the ion energy indicates that the average ion energies of argon and xenon can be as high as 90 and 100keV, respectively. The dependence of the average energy of the ions on the cluster size is also measured. At comparatively low gas backing pressure, the average ion energies of argon and xenon increase with increasing gas backing pressure. The average ion energy of argon becomes saturated gradually with further increase of the gas backing pressure. For xenon, the average ion energy drops a little after the gas backing pressure exceeds 9 bar (3.2×10^5 atoms/cluster). The result showing the existence of a maximum average ion energy has been interpreted within the framework of the microplasma sphere model. 相似文献
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LEI Anle NI Guoquan ZHOU Rufang ZHAI Huajin LIU Bincheng ZHANG Shengjia XU Zhizhan 《中国光学快报(英文版)》1999,8(6)
A pulsed gas jet of large size noble gas atomic clusters as targets for high intensity femtosecond laser pulses is reported. The jet can work for gas stagnation pressure in excess of 40 atmospheres and with a repetition rate of 10 Hz to fit 10 Hz table-top terrawatt femtosecond Ti∶Sapphire laser. The scaling law indicates that the monomer argon clusters produced in the jet can be as large as 22,000 atoms/cluster at room temperature. Preliminary experiments for argon ionic kinetic energy spectrum indicated that the argon clusters are produced in the jet. 相似文献
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LEI Anle NI Guoquan ZHOU Rufang ZHAI Huajin LIU Bincheng ZHANG Shengjia XU Zhizhan 《Chinese Journal of Lasers》1999,8(6):520-524
1 Introduction Muchprogresshasbeenmadeinunderstandingtheintenselaserinteractionswithmatterinrecentyears.Theultrashortlaserpulsesbasedonchirpedpulseamplification(CPA)haveapeakintensityof1014~1019Wcm-2andpulsedurationshorterthan100femtoseconds[1,2].Th… 相似文献
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YAO Lianghua FENG Beibing CHEN Chengyuan NI Guoquan LU Halyang RAN Hong 《核工业西南物理研究院年报(英文版)》2006,(1):41-42
The hydrogen clusters are produced at liquid nitrogen temperature in a supersonic adiabatic expansion of moderate backing pressure gases into vacuum through a Laval nozzle and their averaged size are measured by Rayleigh scattering. The average cluster size N^-c is about 250 hydrogen atoms at a backing pressure 1.0 MPa in these measurements. 相似文献
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Wentao Wang Jiansheng Liu Ming Yang Yi Cai Cheng Wang Guoquan Ni Ruxin Li Zhizhan Xu 《Laser Physics》2009,19(5):974-979
By employing linearly chirped spectral scattering technique, the time-resolved formation processes of argon clusters have been investigated. The redshifts of scattering spectra as a function of backing pressure as well as the time delay between the laser and the firing switch of the cluster flow have been measured. It has been found that very large-size cluster sources with very low gas density can be produced by adiabatic expansion of gases at low pressures through a conical nozzle into vacuum. It can be used as clean and important cluster target. 相似文献