核技术
覈技術
핵기술
NUCLEAR TECHNIQUES
2000年
10期
689
,共1页
赵渭江%颜莎%乐小云%韩宝玺%薛建明%王宇钢%Remnev G E%Opekounov M S%Isakov I F%Grushin I I
趙渭江%顏莎%樂小雲%韓寶璽%薛建明%王宇鋼%Remnev G E%Opekounov M S%Isakov I F%Grushin I I
조위강%안사%악소운%한보새%설건명%왕우강%Remnev G E%Opekounov M S%Isakov I F%Grushin I I
强脉冲离子束%离子注入%脉冲能量效应%材料表面改性
彊脈遲離子束%離子註入%脈遲能量效應%材料錶麵改性
강맥충리자속%리자주입%맥충능량효응%재료표면개성
tense pulsed ion beam%Ion implantation
在脉冲离子束流密度为15120A/cm2、脉宽为50150ns、加速电压为150260kV范围内,在11014cm-2的低注量水平上,
研究了高功率Cn++H+混合离子束注入45号钢样品的强脉冲能量效应。摩擦磨损和微观硬度测量以及SEM和X射线衍射分析表明,上述低注量强脉冲离子束注入可以改变材料
表面的微观结构和力学特性,而且强烈依赖于单个脉冲离子束的功率密度和能量密度。在相同离子注量条件下,普通C++H+离子注入对45号钢样品表面微硬度和摩擦系数未
见明显影响。直接证明了强脉冲能量效应在离子注入中是相对独立于注入元素掺杂效应的又一可利用的重要效应。基于一维导热模型,讨论了强脉冲能量效应以及脉冲离
子束功率密度对离子束材料表面改性的作用。
在脈遲離子束流密度為15120A/cm2、脈寬為50150ns、加速電壓為150260kV範圍內,在11014cm-2的低註量水平上,
研究瞭高功率Cn++H+混閤離子束註入45號鋼樣品的彊脈遲能量效應。摩抆磨損和微觀硬度測量以及SEM和X射線衍射分析錶明,上述低註量彊脈遲離子束註入可以改變材料
錶麵的微觀結構和力學特性,而且彊烈依賴于單箇脈遲離子束的功率密度和能量密度。在相同離子註量條件下,普通C++H+離子註入對45號鋼樣品錶麵微硬度和摩抆繫數未
見明顯影響。直接證明瞭彊脈遲能量效應在離子註入中是相對獨立于註入元素摻雜效應的又一可利用的重要效應。基于一維導熱模型,討論瞭彊脈遲能量效應以及脈遲離
子束功率密度對離子束材料錶麵改性的作用。
재맥충리자속류밀도위15120A/cm2、맥관위50150ns、가속전압위150260kV범위내,재11014cm-2적저주량수평상,
연구료고공솔Cn++H+혼합리자속주입45호강양품적강맥충능량효응。마찰마손화미관경도측량이급SEM화X사선연사분석표명,상술저주량강맥충리자속주입가이개변재료
표면적미관결구화역학특성,이차강렬의뢰우단개맥충리자속적공솔밀도화능량밀도。재상동리자주량조건하,보통C++H+리자주입대45호강양품표면미경도화마찰계수미
견명현영향。직접증명료강맥충능량효응재리자주입중시상대독립우주입원소참잡효응적우일가이용적중요효응。기우일유도열모형,토론료강맥충능량효응이급맥충리
자속공솔밀도대리자속재료표면개성적작용。
In this paper the intense pulsed energy effects of high power pulsed ion beams (HPIBs) are proved to be v
ery important and useful in ion beam implantation. Three groups of 45# ste el samples were implanted with the pulsed ion beams of Cn++H+ at the accel
eration voltage of 150260kV for the pulse duration of 50150ns with the current density of 15120A/cm2, while a low ion dose of about 11014cm-
2 was kept for all implanted samples. Then their tribological properties as well as microhardness were measured, and their morphology and structure
information were given by using SEM and X-ray diffraction analysis. The results showed that the materials' surface properties and microstructure hav
e been modified due to the HPIB implantation even at such low level of ion dose, and the modifications strongly depended on the pulsed power density
and pulsed energy density of HPIBs. These phenomena were considered as the intense pulsed energy effects and discussed on the basis of one dimensio
nal heat conduction model. Meanwhile, the hardly changed surface microhardness and friction coefficient of 45# steel samples implanted with traditio
nal (C+H) ions at an ion dose of 11014cm-2 was given for a demonstration, in which the intense pulsed energy effects are relatively independen
t of the ion doping effects.