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河北省自然科学基金(A2012205072)

作品数:8 被引量:8H指数:1
相关作者:张连珠赵国明孟秀兰高书侠张素更多>>
相关机构:河北师范大学更多>>
发文基金:河北省自然科学基金更多>>
相关领域:理学机械工程更多>>

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8 条 记 录,以下是 1-8
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PIC/MCC Simulation of Radio Frequency Hollow Cathode Discharge in Nitrogen被引量:1
2016年
A two-dimensional PIC/MCC model is developed to simulate the nitrogen radio frequency hollow cathode discharge(rf-HCD).It is found that both the sheath oscillation heating and the secondary electron heating together play a role to maintain the rf-HCD under the simulated conditions.The mean energy of ions(N+_2,N+)in the negative glow region is greater than the thermal kinetic energy of the molecular gas(N2),which is an important characteristic of rf-HCD.During the negative portion of the hollow electrode voltage cycle,electrons mainly follow pendulum movement and produce a large number of ionization collisions in the plasma region.During the positive voltage of the rf cycle,the axial electric field becomes stronger and its direction is pointing to the anode(substrate),therefore the ions move toward the anode(substrate)via the axial electric field acceleration.Compared with dc-HCD,rf-HCD is more suitable for serving as a plasma jet nozzle at low pressure.
韩卿王敬张连珠
N_2-H_2容性耦合等离子体电非对称效应的particle-in-cell/Monte Carlo模拟
2014年
H_2-N_2混合气体电容性耦合射频放电在有机低介电系数材料刻蚀中具潜在研究意义.采用paxticle-incell/Monte Carlo模型模拟了双频(13.56 MHz/27.12 MHz)电压源分别接在结构对称的两个电极上的H_2-N_2容性耦合等离子体特征,研究了其电非对称效应.模拟结果表明,通过调节两谐波间的相位角θ,可以改变其电场、等离子体密度、离子流密度的轴向分布及离子轰击电极的能量分布.当相位角θ为0°时,低频电极(晶片)附近主要离子(H_3^+)的密度最小,离子(H_3^+,H_2^+,H^+)轰击低频电极的流密度及平均能量最高;当θ从0°变化90°时,低频电极的自偏压从-103V到106V近似线性增加,轰击电极的离子流密度变化约±18%,H^+离子轰击低频电极的最大能量约减小2.5倍,轰击电极的平均能量约变化2倍,表明氢离子能量和离子流几乎能独立控制.
郝莹莹孟秀兰姚福宝赵国明王敬张连珠
关键词:PARTICLE-IN-CELLMONTE
N_2射频放电带电粒子(e,N_2^+,N^+)的PIC-MC模拟被引量:1
2012年
采用PIC-MC自洽模型,模拟了氮气电容性耦合射频放电的微观等离子体过程及带电粒子(e,N2+,N+)的行为。结果表明,离子(N2+,N+)的运动状态滞后瞬时射频电场的变化;在两极附近,N2+具较高密度,但能量较低,N+具较低的密度但能量较高,两者的密度差6倍左右。两种离子轰击射频电极的能量分布变化规律类似,随放电参数变化,离子(N2+,N+)能量变化显著,其密度变化不明显。模拟的电子能量几率分布与测量结果一致。
杨莹付东儒张连珠
关键词:射频放电
Effect of Addition of Nitrogen to a Capacitively Radio-Frequency Hydrogen Discharge
2014年
A hybrid PIC/MC model is developed in this work for H2-xN2 capacitively coupled radio-frequency (CCRF) discharges in which we take into account 43 kinds of collisions reaction processes between charged particles (e-, H3+, H+, H+, N+, N+) and ground-state molecules (H2, H+ N2). In addition, the mean energies and densities of electrons and ions ( 3, H+, H+), and electric field distributions in the H2-N2 CCRF discharge are simulated by this model. Furthermore, the effects of addition of a variable percentage of nitrogen (0-30%) into the H2 discharge on the plasma processes and discharge characteristics are studied. It is shown that by increasing the percentage of nitrogen added to the system, the RF sheath thickness will narrow, the sheath electric field will be enhanced, and the mean energy of hydrogen ions impacting the electrodes will be increased. Because the electron impact ionization and dissociative ionization rates increase when N2 is added to the system, the electron mean density will increase while the electron mean energy and hydrogen ion density near the electrodes will decrease. This work aims to provide a theoretical basis for experimental studies and technological developments with regard to H2-N2 CCRF plasmas.
张连珠姚福宝赵国明郝莹莹孙倩
The Effect of Gas Flow Rate on Radio-Frequency Hollow Cathode Discharge Characteristics被引量:1
2014年
It is known that gas flow rate is a key factor in controlling industrial plasma processing. In this paper, a 2D PIC/MCC model is developed for an rf hollow cathode discharge with an axial nitrogen gas flow. The effects of the gas flow rate on the plasma parameters are calculated and the results show that: with an increasing flow rate, the total ion(N+2, N+) density decreases, the mean sheath thickness becomes wider, the radial electric field in the sheath and the axial electric field show an increase, and the energies of both kinds of nitrogen ions increase;and, as the axial ion current density that is moving toward the ground electrode increases, the ion current density near the ground electrode increases. The simulation results will provide a useful reference for plasma jet technology involving rf hollow cathode discharges in N2.
赵国明孙倩赵书霞高书侠张连珠
N_2-Ar射频放电表面氮化的等离子体特性模拟
2012年
N2-Ar射频放电等离子体广泛应用于微电子工业的刻蚀、氮化物薄膜的制备及金属表面氮化等技术领域。开发了N2-Ar混合气体容性耦合射频放电PIC/MC自洽模型,模型主要描述了e-,N2+,N+,Ar+等主要带电粒子的行为分布。等离子体的碰撞过程分别考虑了带电粒子(e-,N2+,N+,Ar+)与基态中性N2分子和Ar原子的21种碰撞反应过程。模拟结果表明,在纯N2及N2-Ar混合气体容性耦合射频放电中,各种带电粒子的数密度都在等离子体区达到最大值,且氮分子离子为主要粒子;在N2容性耦合射频放电中,加入10%氩气时,N+平均能量有所增加,在射频电极处两种氮离子(N2+,N+)高能粒子所占比例增加。本研究对认识N2-Ar射频放电等离子体过程微观机理具重要意义。
孙倩杨莹赵海涛郝莹莹张连珠赵国明
N_2微空心阴极放电特性及其阴极溅射的PIC/MC模拟被引量:5
2013年
采用两维PIC/MCC模型模拟了氮气微空心阴极放电以及轰击离子(N+2,N+)的钛阴极溅射.主要计算了氮气微空心阴极放电离子(N+2,N+)及溅射原子Ti的行为分布,并研究了溅射Ti原子的热化过程.结果表明:在模拟条件下,空心阴极效应是负辉区叠加的电子震荡;在对应条件下,微空心较传统空心放电两种离子(N+2,N+)密度均大两个量级,两种离子的平均能量的分布及大小几乎相同;在放电空间N+的密度约为N+2的1/6,最大能量约大2倍;在不同参数(P,T,V)下,轰击阴极内表面的氮离子(N+2,N+)的密度近似均匀,其平均能量几乎相等;从阴极溅射出的Ti原子的初始平均能量约6.8eV,离开阴极约0.15mm处几乎完全被热化.模拟结果为N2微空心阴极放电等离子体特性的认识提供了参考依据.
张连珠孟秀兰张素高书侠赵国明
关键词:PIC
N_2/Ti微空心阴极放电等离子体阴极溅射模拟
2013年
采用Monte Carlo方法模拟N2/Ti微空心阴极放电等离子体阴极溅射过程,其中,氮离子(N2+,N+)轰击阴极表面采用PIC/MC模型模拟.计算溅射钛原子的热化过程、钛原子的密度及其平均能量分布.结果表明,沿各方向溅射出的90%金属Ti原子所带的初始能量小于30 eV,其散射角主要分布在30°和60°之间;溅射Ti原子在离微空心阴极壁约0.04 mm处出现热化极大值.
高书侠张素孟秀兰张连珠
关键词:阴极溅射
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