激光杂志
激光雜誌
격광잡지
LASER JOURNAL
2011年
6期
16-17
,共2页
张利平%蔡勤%栾楠楠%程玉锋%戴康%沈异凡
張利平%蔡勤%欒楠楠%程玉鋒%戴康%瀋異凡
장리평%채근%란남남%정옥봉%대강%침이범
能量转移%相干反斯托克斯拉曼谱%能量配置%弛豫率%Li2-H2
能量轉移%相榦反斯託剋斯拉曼譜%能量配置%弛豫率%Li2-H2
능량전이%상간반사탁극사랍만보%능량배치%이예솔%Li2-H2
energy transfer%CARs%energy disposal rate%Li2- He
利用相干反斯托克斯拉曼谱(CArtS)分析了H2与Li2(A^1∑u^+)-H2碰撞的振转态布居分布。扫描cARS谱表明了在能量转移过程中H2的v=1,2,3振转能级上得到布居,由CARS峰值得到两个可能的布居数比值,通过解速率方程组并通过时间分辨CARS轮廓模拟,确定了实际的布居数之比。得到了H2在V=1,2,3能级上的布居数比为0.48,0.36,0.16,平均转移能配置的相对值〈ft〉,(fvib〉,〈fr〉分别为0.50,0.47,0.03,能量主要配置在平动和振动上,支持Li2-H2直线式碰撞传能机制。
利用相榦反斯託剋斯拉曼譜(CArtS)分析瞭H2與Li2(A^1∑u^+)-H2踫撞的振轉態佈居分佈。掃描cARS譜錶明瞭在能量轉移過程中H2的v=1,2,3振轉能級上得到佈居,由CARS峰值得到兩箇可能的佈居數比值,通過解速率方程組併通過時間分辨CARS輪廓模擬,確定瞭實際的佈居數之比。得到瞭H2在V=1,2,3能級上的佈居數比為0.48,0.36,0.16,平均轉移能配置的相對值〈ft〉,(fvib〉,〈fr〉分彆為0.50,0.47,0.03,能量主要配置在平動和振動上,支持Li2-H2直線式踫撞傳能機製。
이용상간반사탁극사랍만보(CArtS)분석료H2여Li2(A^1∑u^+)-H2팽당적진전태포거분포。소묘cARS보표명료재능량전이과정중H2적v=1,2,3진전능급상득도포거,유CARS봉치득도량개가능적포거수비치,통과해속솔방정조병통과시간분변CARS륜곽모의,학정료실제적포거수지비。득도료H2재V=1,2,3능급상적포거수비위0.48,0.36,0.16,평균전이능배치적상대치〈ft〉,(fvib〉,〈fr〉분별위0.50,0.47,0.03,능량주요배치재평동화진동상,지지Li2-H2직선식팽당전능궤제。
Coherent anti - Stokes Raman Spectroscopy ( CARS} ha been used to analyze the vibrotational state distribution of H2 after energy transfer with Li2 (A^1∑u^+).The scanned CARS spectra reveal that during energy transfer processes H2 molecules are produced at the V = 1,2 and 3 vibrational levels. From scanned CARS spectral peaks two possible population ratios are obtained. Through shape simulations of the time resolved CARS profiles under a kineti model, the actual population ratios are determined. The H2 molecules produced by the energy transfer process are O. 48 populated at the V = 1 level, 0.36 at V = 2 and 0.16 at V = 3. The relative fractions ( 〈 fv 〉 , 〈 fvib 〉 , 〈 fr 〉) of average energy disposal are derived as ( 0.50, 0. 47, 0.03 ), having major vibrational and translational energy release. This consequence supports a collinear collision geometry in Li2 - H2 energy transfer.