期刊文献+
共找到58篇文章
< 1 2 3 >
每页显示 20 50 100
The effect of nitrogen concentration on the properties of N-DLC prepared by helicon wave plasma chemical vapor deposition
1
作者 Yan YANG Tianyuan HUANG +5 位作者 Maoyang LI Yaowei YU Jianjun HUANG Bin YU Xuemei WU Peiyu JI 《Plasma Science and Technology》 SCIE EI CAS CSCD 2022年第10期98-104,共7页
Nitrogen-doped diamond-like carbon(N-DLC)films were synthesized by helicon wave plasma chemical vapor deposition(HWP-CVD).The mechanism of the plasma influence on the N-DLC structure and properties was revealed by the... Nitrogen-doped diamond-like carbon(N-DLC)films were synthesized by helicon wave plasma chemical vapor deposition(HWP-CVD).The mechanism of the plasma influence on the N-DLC structure and properties was revealed by the diagnosis of plasma.The effects of nitrogen doping on the mechanical and hydrophobicity properties of DLC films were studied.The change in the ratio of precursor gas flow reduces the concentration of film-forming groups,resulting in a decrease of growth rate with increasing nitrogen flow rate.The morphology and structure of N-DLC films were characterized by scanning probe microscopy,Raman spectroscopy,and X-ray photoemission spectroscopy.The mechanical properties and wettability of N-DLC were analyzed by an ultra-micro hardness tester and JC2000DM system.The results show that the content ratio of N^(+)and N_(2)^(+)is positively correlated with the mechanical properties and wettability of N-DLC films.The enhancement hardness and elastic modulus of N-DLC are attributed to the increase in sp3 carbon–nitrogen bond content in the film,reaching 26.5 GPa and 160 GPa respectively.Water contact measurement shows that the increase in the nitrogen-bond structure in N-DLC gives the film excellent hydrophobic properties,and the optimal water contact angle reaches 111.2°.It is shown that HWP technology has unique advantages in the modulation of functional nanomaterials. 展开更多
关键词 N-DLC helicon wave plasma microstructure HARDNESS HYDROPHOBICITY
在线阅读 下载PDF
Synthesis of SiC/graphene nanosheet composites by helicon wave plasma
2
作者 Jia-Li Chen Pei-Yu Ji +2 位作者 Cheng-Gang Jin Lan-Jian Zhuge Xue-Mei Wu 《Chinese Physics B》 SCIE EI CAS CSCD 2021年第7期339-344,共6页
We report an approach to the rapid, one-step, preparation of a variety of wide-bandgap silicon carbide/graphene nanosheet(Si C/GNSs) composites by using a high-density helicon wave plasma(HWP) source. The microstructu... We report an approach to the rapid, one-step, preparation of a variety of wide-bandgap silicon carbide/graphene nanosheet(Si C/GNSs) composites by using a high-density helicon wave plasma(HWP) source. The microstructure and morphology of the Si C/GNSs are characterized by using scanning electron microscopy(SEM), Raman spectroscopy, x-ray diffraction(XRD), x-ray photoelectron spectroscopy(XPS), and fluorescence(PL). The nucleation mechanism and the growth model are discussed. The existence of Si C and graphene structure are confirmed by XRD and Raman spectra.The electron excitation temperature is calculated by the intensity ratio method of optical emission spectroscopy. The main peak in the PL test is observed at 420 nm, with a corresponding bandgap of 2.95 e V that indicates the potential for broad application in blue light emission and ultraviolet light emission, field electron emission, and display devices. 展开更多
关键词 helicon wave plasma SiC/graphene nanosheet x-ray photoelectron spectroscopy(XPS) FLUORESCENCE
原文传递
Mechanism of high growth rate for diamond-like carbon films synthesized by helicon wave plasma chemical vapor deposition
3
作者 季佩宇 於俊 +4 位作者 黄天源 金成刚 杨燕 诸葛兰剑 吴雪梅 《Plasma Science and Technology》 SCIE EI CAS CSCD 2018年第2期166-171,共6页
A high growth rate fabrication of diamond-like carbon(DLC)films at room temperature was achieved by helicon wave plasma chemical vapor deposition(HWP-CVD)using Ar/CH4gas mixtures.The microstructure and morphology ... A high growth rate fabrication of diamond-like carbon(DLC)films at room temperature was achieved by helicon wave plasma chemical vapor deposition(HWP-CVD)using Ar/CH4gas mixtures.The microstructure and morphology of the films were characterized by Raman spectroscopy and scanning electron microscopy.The diagnosis of plasma excited by a helicon wave was measured by optical emission spectroscopy and a Langmuir probe.The mechanism of high growth rate fabrication for DLC films by HWP-CVD has been discussed.The growth rate of the DLC films reaches a maximum value of 54μm h^-1at the CH4flow rate of 85 sccm,which is attributed to the higher plasma density during the helicon wave plasma discharge.The CH and Hαradicals play an important role in the growth of DLC films.The results show that the Hαradicals are beneficial to the formation and stabilization of C=C bond from sp^2to sp^3. 展开更多
关键词 helicon wave plasma diamond-like carbon film sp^3 content Raman spectra
在线阅读 下载PDF
The properties of N-doped diamond-like carbon films prepared by helicon wave plasma chemical vapor deposition 被引量:4
4
作者 Jiali CHEN Peiyu JI +2 位作者 Chenggang JIN Lanjian ZHUGE Xuemei WU 《Plasma Science and Technology》 SCIE EI CAS CSCD 2019年第2期78-82,共5页
In this paper, N-doped diamond-like carbon(DLC) films were deposited on silicon substrates by using helicon wave plasma chemical vapor deposition(HWP-CVD) with the Ar/CH_4/N_2 mixed gas. The surface morphology, struct... In this paper, N-doped diamond-like carbon(DLC) films were deposited on silicon substrates by using helicon wave plasma chemical vapor deposition(HWP-CVD) with the Ar/CH_4/N_2 mixed gas. The surface morphology, structural and mechanical properties of the N-doped DLC films were investigated in detail by scanning electron microscopy(SEM), x-ray photoelectron spectroscopy(XPS), Raman spectra, and atomic force microscopy(AFM). It can be observed from SEM images that surface morphology of the films become compact and uniform due to the incorporation of N. The maximum of the deposition rate of the films is 143 nm min^(-1), which is related to the high plasma density. The results of XPS show that the N incorporates in the films and the C-C sp^3 bond content increases firstly up to the maximum(20%) at 10 sccm of N_2 flow rate, and then decreases with further increase in the N_2 flow rate. The maximum Young's modulus of the films is obtained by the doping of N and reaches 80 GPa at 10 sccm of N_2 flow rate, which is measured by AFM in the scanning probe microscope mode. Meanwhile, friction characteristic of the N-doped DLC films reaches a minimum value of 0.010. 展开更多
关键词 N-DOPED DLC helicon wave plasma Young’s MODULUS FRICTION COEFFICIENT
在线阅读 下载PDF
Comparison of heating mechanisms of argon helicon plasma in different wave modes with and without blue core 被引量:2
5
作者 崔瑞林 张天亮 +3 位作者 袁倩 何锋 韩若愚 欧阳吉庭 《Plasma Science and Technology》 SCIE EI CAS CSCD 2023年第1期53-66,共14页
In this work,we investigated the discharge characteristics and heating mechanisms of argon helicon plasma in different wave coupled modes with and without blue core.Spatially resolved spectroscopy and emission intensi... In this work,we investigated the discharge characteristics and heating mechanisms of argon helicon plasma in different wave coupled modes with and without blue core.Spatially resolved spectroscopy and emission intensity of argon atom and ion lines were measured via local optical emission spectroscopy,and electron density was measured experimentally by an RFcompensated Langmuir probe.The relation between the emission intensity and the electron density was obtained and the wavenumbers of helicon and’Trivelpiece-Gould’(TG)waves were calculated by solving the dispersion relation in wave modes.The results show that at least two distinct wave coupled modes appear in argon helicon plasma at increasing RF power,i.e.blue core(or BC)mode with a significant bright core of blue lights and a normal wave(NW)mode without blue core.The emission intensity of atom line 750.5 nm(lArⅠ750.5nm)is related to the electron density and tends to be saturated in wave coupled modes due to the neutral depletion,while the intensity of ion line 480.6 nm(IArⅡ480.6nm)is a function of the electron density and temperature,and increases dramatically as the RF power is increased.Theoretical analysis shows that TG waves are strongly damped at the plasma edge in NW and/or BC modes,while helicon waves are the dominant mechanism of power deposition or central heating of electrons in both modes.The formation of BC column mainly depends on the enhanced central electron heating by helicon waves rather than TG waves since the excitation of TG waves would be suppressed in this special anti-resonance region. 展开更多
关键词 argon helicon plasma wave coupled mode optical emission spectroscopy helicon waves TG waves
在线阅读 下载PDF
Development of a helicon-wave excited plasma facility with high magnetic field for plasma-wall interactions studies 被引量:2
6
作者 Guilu ZHANG Tianyuan HUANG +3 位作者 Chenggang JIN Xuemei WU Lanjian ZHUGE Hantao JI 《Plasma Science and Technology》 SCIE EI CAS CSCD 2018年第8期112-118,共7页
The high magnetic field helicon experiment system is a helicon wave plasma(HWP)source device in a high axial magnetic field(B0)developed for plasma–wall interactions studies for fusion reactors.This HWP was reali... The high magnetic field helicon experiment system is a helicon wave plasma(HWP)source device in a high axial magnetic field(B0)developed for plasma–wall interactions studies for fusion reactors.This HWP was realized at low pressure(5×10^-3-10 Pa)and a RF(radio frequency,13.56 MHz)power(maximum power of 2 k W)using an internal right helical antenna(5 cm in diameter by 18 cm long)with a maximum B0of 6300 G.Ar HWP with electron density~10^18–10^20m^-3 and electron temperature~4–7 e V was produced at high B0 of 5100 G,with an RF power of 1500 W.Maximum Ar^+ion flux of 7.8×10^23m^-2s^-1 with a bright blue core plasma was obtained at a high B0 of 2700 G and an RF power of 1500 W without bias.Plasma energy and mass spectrometer studies indicate that Ar^+ ion-beams of 40.1 eV are formed,which are supersonic(~3.1cs).The effect of Ar HWP discharge cleaning on the wall conditioning are investigated by using the mass spectrometry.And the consequent plasma parameters will result in favorable wall conditioning with a removal rate of 1.1×10^24N2/m^2 h. 展开更多
关键词 helicon wave plasma high magnetic field wall conditioning
在线阅读 下载PDF
Wave field structure and power coupling features of blue-core helicon plasma driven by various antenna geometries and frequencies 被引量:1
7
作者 王超 刘佳 +3 位作者 苌磊 卢凌峰 张世杰 周帆涛 《Chinese Physics B》 SCIE EI CAS CSCD 2024年第3期480-487,共8页
This paper deals with wave propagation and power coupling in blue-core helicon plasma driven by various antennas and frequencies.It is found that compared to non-blue-core mode,for blue-core mode,the wave can propagat... This paper deals with wave propagation and power coupling in blue-core helicon plasma driven by various antennas and frequencies.It is found that compared to non-blue-core mode,for blue-core mode,the wave can propagate in the core region,and it decays sharply outside the core.The power absorption is lower and steeper in radius for blue-core mode.Regarding the effects of antenna geometry for blue-core mode,it shows that half helix antenna yields the strongest wave field and power absorption,while loop antenna yields the lowest.Moreover,near axis,for antennas with m=+1,the wave field increases with axial distance.In the core region,the wave number approaches to a saturation value at much lower frequency for non-blue-core mode compared to blue-core mode.The total loading resistance is much lower for blue-core mode.These findings are valuable to understanding the physics of blue-core helicon discharge and optimizing the experimental performance of blue-core helicon plasma sources for applications such as space propulsion and material treatment. 展开更多
关键词 helicon plasma helicon wave helicon discharge radio frequency plasma source
原文传递
Modification of exposure conditions by the magnetic field configuration in helicon antenna-excited helium plasma 被引量:1
8
作者 Tianyuan HUANG Peiyu JI +2 位作者 Jianjun HUANG Bin YU Xuemei WU 《Plasma Science and Technology》 SCIE EI CAS CSCD 2021年第1期63-69,共7页
Modification of exposure conditions downstream in the diffusion chamber has been performed in helicon antenna-excited helium plasma by adjusting the magnetic field(intensity and geometry).In the inductively coupled mo... Modification of exposure conditions downstream in the diffusion chamber has been performed in helicon antenna-excited helium plasma by adjusting the magnetic field(intensity and geometry).In the inductively coupled mode(H mode),a reduction in ion and heat fluxes is found with increasing magnetic field intensity,which is further explained by the more highly magnetized ions off-axis around the last magnetic field lines(LMFL).However,in helicon wave mode(W mode),the increase in magnetic field intensity can dramatically increase the ion and heat fluxes.Moreover,the effect of LMFL geometry on exposure conditions is investigated.In H mode with contracting LMFL,off-axis peaks of both plasma density and electron temperature profiles shift radially inwards,bringing about a beam with better radial uniformity and higher ion and heat fluxes.In W mode,although higher ion and heat fluxes can be achieved with suppressed plasma cross-field diffusion under converging LMFL,the poor radial uniformity and a small beam diameter will limit the size of samples suitable for plasma irradiation experiments. 展开更多
关键词 helicon wave plasma plasma source magnetized plasma plasma diagnostics
在线阅读 下载PDF
The application of a helicon plasma source in reactive sputter deposition of tungsten nitride thin films
9
作者 Yan YANG Peiyu JI +5 位作者 Maoyang LI Yaowei YU Jianjun HUANG Bin YU Xuemei WU Tianyuan HUANG 《Plasma Science and Technology》 SCIE EI CAS CSCD 2022年第6期157-163,共7页
A reactive helicon wave plasma(HWP)sputtering method is used for the deposition of tungsten nitride(WNx)thin films.N_(2)is introduced downstream in the diffusion chamber.The impacts of N_(2)on the Ar-HWP parameters,su... A reactive helicon wave plasma(HWP)sputtering method is used for the deposition of tungsten nitride(WNx)thin films.N_(2)is introduced downstream in the diffusion chamber.The impacts of N_(2)on the Ar-HWP parameters,such as ion energy distribution functions(IEDFs),electron energy probability functions(EEPFs),electron temperature(Te)and density(ne),are investigated.With the addition of N_(2),a decrease in electron density is observed due to the dissociative recombination of electrons with N_(2)^(+).The similar IEDF curves of Ar+and N_(2)^(+) indicate that the majority ofN_(2)^(+) stems from the charge transfer in the collision between Ar+and N_(2).Moreover,due to the collisions between electrons and N_(2)ions,EEPFs show a relatively lower Tewith a depletion in the high-energy tail.With increasing negative bias from 50 to 200 V,a phase transition from hexagonal WN to fcc-WN0.5is observed,together with an increase in the deposition rate and roughness. 展开更多
关键词 helicon wave plasma reactive sputtering tungsten nitride plasma diagnosis
在线阅读 下载PDF
HL-3托卡马克装置D-T等离子体运行模式的螺旋波辅助电流驱动
10
作者 王森 资道政 +1 位作者 程泽厚 李新霞 《原子能科学技术》 北大核心 2025年第12期2763-2770,共8页
D-T等离子体放电是堆级托卡马克装置的重要运行模式。本文针对HL-3托卡马克装置,通过理论分析螺旋波阻尼系数与等离子体参数的关系,获得了HL-3装置典型的D-T等离子体放电模式下螺旋波优化的波参数范围;同时,耦合GENRAY/CQL3D计算程序开... D-T等离子体放电是堆级托卡马克装置的重要运行模式。本文针对HL-3托卡马克装置,通过理论分析螺旋波阻尼系数与等离子体参数的关系,获得了HL-3装置典型的D-T等离子体放电模式下螺旋波优化的波参数范围;同时,耦合GENRAY/CQL3D计算程序开展了波传播轨迹、波功率沉积和驱动电流等的数值模拟计算。研究结果表明:螺旋波能直接传播到芯部等离子体区域,并且在较宽的径向范围内高效地离轴驱动等离子体电流,其驱动电流约85 kA/MW,无量纲电流驱动效率约为0.36,而T离子的份额对螺旋波驱动电流及其剖面分布基本无影响。此外,基于CQL3D程序,计算获得了螺旋波注入后的电子相空间分布函数,证实了更多的捕获粒子变成了通行粒子,从而高效驱动等离子体电流。研究结果表明,螺旋波在HL-3装置中有潜在的、重要的应用前景。 展开更多
关键词 HL-3托卡马克装置 螺旋波电流驱动 D-T等离子体 数值模拟
在线阅读 下载PDF
螺旋波等离子体功率沉积特性的数值模拟研究
11
作者 崔瑞林 《力学学报》 北大核心 2025年第7期1611-1617,共7页
螺旋波等离子体凭借其高电离率、高密度等优势,在半导体制造与电推进领域具有重要应用价值.针对现有研究难以解析实验中多波耦合模式下功率沉积机制这一科学难题,本研究基于HELIC数值模拟,系统探究Trivelpiece-Gould(TG)波与Helicon(H)... 螺旋波等离子体凭借其高电离率、高密度等优势,在半导体制造与电推进领域具有重要应用价值.针对现有研究难以解析实验中多波耦合模式下功率沉积机制这一科学难题,本研究基于HELIC数值模拟,系统探究Trivelpiece-Gould(TG)波与Helicon(H)波的本征模式竞争规律及其在低、高阶波耦合模式下的功率沉积特性.通过构建参数化径向密度剖面模型(梯度参数s=2.1~3.4,峰化参数t=1.8~2.5),并结合自洽求解Maxwell-Boltzmann耦合方程组的数值方法,实现了多波模式跳变过程的动态重构.结果表明:在低阶波模式(W1,n_(e)=2.0×10^(12) cm^(-3))下,TG波通过径向电场局域化机制贡献61.8%的边界电子加热效率,而H波中心区功率沉积占比仅38.2%;当激发高阶本征模(W2-W4,ne=4.0×10^(12)~1.1×10^(13) cm^(-3))时,TG波边缘阻尼效应导致其功率占比骤降至16.5%,此时H波通过轴向驻波共振实现中心区83.5%的功率沉积主导,并诱导等离子体密度分布从边缘峰化(s=2.1)向中心聚集(s=3.4)的模态转变.研究结果为精确调控螺旋波等离子体参数分布及模式选择提供了重要理论支撑,对优化半导体刻蚀均匀性和电推进器比冲性能具有直接指导意义. 展开更多
关键词 螺旋波等离子体 TG-H 波耦合 本征模式 功率沉积
在线阅读 下载PDF
高密度螺旋波等离子体源的应用进展 被引量:8
12
作者 柏洋 赵岩 +3 位作者 金成刚 余涛 吴雪梅 诸葛兰剑 《微纳电子技术》 CAS 北大核心 2011年第11期739-743,共5页
首先介绍了螺旋波的定义、螺旋波等离子体源产生等离子体所需条件的工作范围以及螺旋波等离子体源主要的一些应用。按照所加磁场范围的不同(分为在磁感应强度为100~1 600Gs和在强磁场中两部分),分别进一步讨论了国内外各研究小组研制... 首先介绍了螺旋波的定义、螺旋波等离子体源产生等离子体所需条件的工作范围以及螺旋波等离子体源主要的一些应用。按照所加磁场范围的不同(分为在磁感应强度为100~1 600Gs和在强磁场中两部分),分别进一步讨论了国内外各研究小组研制的等离子体源的运行参数及技术特点。随后介绍了螺旋波等离子体源在刻蚀、薄膜沉积和火箭推进三个方面的应用进展。其中重点介绍了螺旋波等离子体火箭推进。最后简单展望了螺旋波等离子体源的应用前景,并指出其发展中尚待解决的一些问题。 展开更多
关键词 螺旋波 等离子体源 磁场 刻蚀 薄膜沉积 火箭推进
原文传递
低温低压氢等离子体的光谱分析 被引量:7
13
作者 邓红艳 王加扣 +2 位作者 吴卫东 程新路 杨向东 《原子与分子物理学报》 CAS CSCD 北大核心 2005年第2期256-259,共4页
采用螺旋波激发氢等离子体,测得氢的Balmer线系前三条谱线的强度。利用二谱线法求电子温度Te,并由Hβ的Stark展宽得到电子密度Ne,简要分析了Te、Ne以及强度与各种参数之间的关系。
关键词 电子温度 电子密度 Balmer线系 螺旋波等离子体
在线阅读 下载PDF
HWP-CVD氮化硅薄膜的结构和光学特性 被引量:5
14
作者 于威 侯海虹 +2 位作者 何杰 王华英 傅广生 《无机材料学报》 SCIE EI CAS CSCD 北大核心 2004年第4期907-911,共5页
采用傅立叶红外吸收谱和紫外-可见透射谱研究了螺旋波等离子体增强化学气相沉积法制备的氢化非晶氮化硅薄膜的原子间键合结构和光学特性。结果表明,在不同硅、氮活性气体配比冗下,薄膜表现出不同的Si/N比和H原子键合方式,富氮样品中H原... 采用傅立叶红外吸收谱和紫外-可见透射谱研究了螺旋波等离子体增强化学气相沉积法制备的氢化非晶氮化硅薄膜的原子间键合结构和光学特性。结果表明,在不同硅、氮活性气体配比冗下,薄膜表现出不同的Si/N比和H原子键合方式,富氮样品中H原子主要和N原子结合,而富硅样品中主要和Si原子结合。随着R的增加,薄膜的光学带隙Eg和E04逐渐减小,此结果关联于薄膜结构无序性程度的增加,而薄膜的(E04-Eg)和Tauc斜率B值之间存在着相互制约关系。 展开更多
关键词 氮化硅薄膜 光学特性 螺旋波等离子体增强化学气相沉积
在线阅读 下载PDF
螺旋波激发氢等离子体的电子温度及密度研究 被引量:7
15
作者 朱永红 吴卫东 +1 位作者 唐永建 孙卫国 《真空科学与技术学报》 EI CAS CSCD 北大核心 2008年第4期308-312,共5页
采用射频调谐朗缪尔单探针方法对螺旋波激发的氢等离子体I-V特性曲线进行了测量。运用Druyvestey方法对氢等离子体的电子能量分布(EEDF)及电子密度ne的变化规律进行了研究,并与发射光谱诊断结果进行了比较。结果表明:ne随着射频功率的... 采用射频调谐朗缪尔单探针方法对螺旋波激发的氢等离子体I-V特性曲线进行了测量。运用Druyvestey方法对氢等离子体的电子能量分布(EEDF)及电子密度ne的变化规律进行了研究,并与发射光谱诊断结果进行了比较。结果表明:ne随着射频功率的增大成线性增大,本实验中最大值可达到1012cm-3量级,电子平均能量E随着射频功率的增大逐渐升高,并逐渐达到饱和;ne随着工作气压的增加而增大并出现峰值,存在一个最佳气压范围(2 Pa^4 Pa)使ne达到最大,E则随着工作气压的增加逐渐减小;氢气流量对ne的影响非常小,当氢气流量达到一定值(12 sccm)后,ne几乎不变化,E随着氢气流量的增加逐渐降低,最后趋于稳定;朗缪尔单探针方法与发射光谱法诊断的结果基本一致。 展开更多
关键词 等离子体诊断 等离子体参数 射频调谐朗谬尔探针 螺旋波等离子体
在线阅读 下载PDF
氢化非晶氮化硅薄膜的光学特性研究 被引量:3
16
作者 于威 侯海虹 +2 位作者 王保柱 刘丽辉 傅广生 《河北大学学报(自然科学版)》 CAS 2003年第3期253-256,共4页
采用螺旋波等离子体增强化学气相沉积 (HWP -CVD)技术以SiH4 和N2 为反应气体沉积了氮化硅 (SiN)薄膜 ,利用傅里叶红外吸收谱 (FTIR)、紫外 -可见透射谱 (UV -VIS)等对薄膜的键合结构、光学带隙等参量进行了测量与分析 .结果表明 ,采用H... 采用螺旋波等离子体增强化学气相沉积 (HWP -CVD)技术以SiH4 和N2 为反应气体沉积了氮化硅 (SiN)薄膜 ,利用傅里叶红外吸收谱 (FTIR)、紫外 -可见透射谱 (UV -VIS)等对薄膜的键合结构、光学带隙等参量进行了测量与分析 .结果表明 ,采用HWP -CVD技术能在较低的衬底温度下制备低H含量的SiN薄膜 ,所沉积的薄膜主要表现为Si -N键合结构 .适当提高N2 /SiH4 比例将有利于薄膜中H含量的降低 . 展开更多
关键词 氢化非晶氮化硅薄膜 螺旋波等离子体 光学带隙 化学气相沉积 傅里叶红外吸收谱 紫外-可见透射谱
在线阅读 下载PDF
螺旋波等离子体化学气相沉积法制备纳米碳化硅薄膜 被引量:3
17
作者 于威 王保柱 +2 位作者 孙运涛 韩理 傅广生 《人工晶体学报》 EI CAS CSCD 北大核心 2003年第3期272-275,共4页
采用螺旋波等离子体化学气相沉积 (HWP CVD)技术在Si(10 0 )和石英衬底上合成了具有纳米结构的碳化硅薄膜。通过X射线衍射 (XRD)、傅立叶红外透射 (FTIR)和原子力显微镜 (AFM)等技术对所制备薄膜的结构、组分和形貌进行了分析 ,利用光... 采用螺旋波等离子体化学气相沉积 (HWP CVD)技术在Si(10 0 )和石英衬底上合成了具有纳米结构的碳化硅薄膜。通过X射线衍射 (XRD)、傅立叶红外透射 (FTIR)和原子力显微镜 (AFM)等技术对所制备薄膜的结构、组分和形貌进行了分析 ,利用光致发光技术研究了样品的发光特性。分析表明 ,在 70 0℃的衬底温度和 1.33Pa的气压条件下所制备纳米SiC薄膜的平均颗粒度在 3nm以下 ,红外透射谱主要表现为Si C吸收。结果说明HWP CVD为制备高质量纳米SiC薄膜的有效技术 ,所制备样品呈现出室温短波长可见发光特性 ,发光谱主峰位于 395nm附近。 展开更多
关键词 螺旋波等离子体 化学气相沉积法 制备 纳米碳化硅薄膜
在线阅读 下载PDF
不同衬底温度下ZnO外延薄膜的结构及光学特性分析 被引量:2
18
作者 张子生 尹志会 +3 位作者 许贺菊 贾亮 于威 傅广生 《人工晶体学报》 EI CAS CSCD 北大核心 2006年第5期1118-1122,共5页
采用螺旋波等离子体辅助射频溅射沉积技术在A l2O3(0001)衬底上沉积ZnO外延薄膜,通过对其结构及光学性质的分析,探讨了衬底温度对薄膜生长特性的影响。实验结果表明,由于等离子体对反应气体的活化及载能粒子对表面反应的辅助作用,采用... 采用螺旋波等离子体辅助射频溅射沉积技术在A l2O3(0001)衬底上沉积ZnO外延薄膜,通过对其结构及光学性质的分析,探讨了衬底温度对薄膜生长特性的影响。实验结果表明,由于等离子体对反应气体的活化及载能粒子对表面反应的辅助作用,采用该等离子体辅助溅射技术能够在较低的衬底温度下实现较高质量的ZnO薄膜外延生长,然而,较高的衬底温度所引起的表面反应不利于薄膜中的氧空位及锌填隙等缺陷的减少,这将限制薄膜的外延质量及光学特性的进一步提高。 展开更多
关键词 ZNO薄膜 衬底温度 螺旋波等离子体 外延
在线阅读 下载PDF
径向压力和温度分布对螺旋波等离子体波场和能量吸收影响研究 被引量:2
19
作者 张磊 张百灵 +2 位作者 苌磊 李益文 段朋振 《推进技术》 EI CAS CSCD 北大核心 2017年第9期2152-2160,共9页
为了揭示螺旋波等离子体推力器中的等离子体源功率耦合机理,针对气体工质电离后被射频加热的稳态过程,考虑等离子体密度非均匀分布条件,采用三参数压力函数(fa,sp,tp)和温度函数(f_a,s_t,t_t)表示柱状等离子体内压力和温度的径向分布,... 为了揭示螺旋波等离子体推力器中的等离子体源功率耦合机理,针对气体工质电离后被射频加热的稳态过程,考虑等离子体密度非均匀分布条件,采用三参数压力函数(fa,sp,tp)和温度函数(f_a,s_t,t_t)表示柱状等离子体内压力和温度的径向分布,分析了径向压力梯度、温度梯度对螺旋波等离子体内功率沉积、波电场、波磁场和电流密度的影响。考虑梯度为正,梯度为负和梯度为零三种梯度类型。结果发现:压力梯度为正时,螺旋波在等离子体临近壁面处的功率沉积减弱,但射频波透入深度增加,原因是靠近管壁处等离子体密度较低,RF波径向单位长度衰减较少,透入深度增加。温度梯度为负时,柱状等离子体中心处能量沉积变强,原因是管中心位置等离子体密度较大,电子温度较高,与RF波能量耦合增强;横向截面的电磁场、电流密度分布在不同压力和温度梯度下基本不变,证明了m=1模式的稳定性。 展开更多
关键词 径向压力梯度 径向温度梯度 螺旋波 等离子体 功率沉积
原文传递
朗谬尔单探针测量螺旋波等离子体参量 被引量:2
20
作者 刘丽辉 于威 +1 位作者 赵启大 傅广生 《南开大学学报(自然科学版)》 CAS CSCD 北大核心 2004年第3期28-31,共4页
在国内首次引入了一种用朗谬尔单探针测量螺旋波等离子体参数的简单方法,并阐述了测量原理,对实验结果进行了初步的讨论.结果表明测量螺旋波等离子体参量的朗谬尔单探针法简单可行,是一种较好的测量手段.
关键词 螺旋波等离子体 朗谬尔单探针 电子温度 电子密度
在线阅读 下载PDF
上一页 1 2 3 下一页 到第
使用帮助 返回顶部