光子学报
光子學報
광자학보
ACTA PHOTONICA SINICA
2009年
3期
532-535
,共4页
黄才华%薛亦渝%夏志林%赵元安%杨芳芳
黃纔華%薛亦渝%夏誌林%趙元安%楊芳芳
황재화%설역투%하지림%조원안%양방방
激光物理%激光诱导损伤%飞秒激光脉冲%多光子离化%雪崩离化%初始电子密度
激光物理%激光誘導損傷%飛秒激光脈遲%多光子離化%雪崩離化%初始電子密度
격광물리%격광유도손상%비초격광맥충%다광자리화%설붕리화%초시전자밀도
Laser physics%Laser damage%Femtosecond laser pulse%Multi-photon ionization%Avalanche ionization%Initial electron density
基于电子密度演化模型,借助数值方法,研究了飞秒激光作用下光学薄膜内的电子密度演化过程,讨论了初始电子密度Ni和激光脉冲宽度τ对光学薄膜激光损伤阈值Fth的影响,分析了激光诱导薄膜损伤过程中MPI和AI的性质和作用.研究结果表明,对应于一定的脉宽,存在一个临界初始电子密度,当Ni低于这一临界密度时,Fth不受Ni影响;当Ni高于临界密度时,Fth随Ni增加而降低.临界初始电子密度随着脉宽的减小而增加.对于FS和BBS介质薄膜,Fth随脉宽的增加而升高.初始电子密度Ni对BBS中的MPI和AI基本没有影响;同样Ni对FS中的AI基本不产生影响,但当Ni>1011 cm-3时,FS中MPI电子密度随Ni增加而降低.在所研究的脉宽范围τ∈[0.01,5]ps,AI是FS介质激光诱导损伤的主要机制.而对于BBS,当脉宽τ∈[0.03,5]ps,AI是激光诱导损伤的主要机制;当脉宽τ∈[0.01,0.03]ps,MPI在激光诱导损伤中占主导地位.
基于電子密度縯化模型,藉助數值方法,研究瞭飛秒激光作用下光學薄膜內的電子密度縯化過程,討論瞭初始電子密度Ni和激光脈遲寬度τ對光學薄膜激光損傷閾值Fth的影響,分析瞭激光誘導薄膜損傷過程中MPI和AI的性質和作用.研究結果錶明,對應于一定的脈寬,存在一箇臨界初始電子密度,噹Ni低于這一臨界密度時,Fth不受Ni影響;噹Ni高于臨界密度時,Fth隨Ni增加而降低.臨界初始電子密度隨著脈寬的減小而增加.對于FS和BBS介質薄膜,Fth隨脈寬的增加而升高.初始電子密度Ni對BBS中的MPI和AI基本沒有影響;同樣Ni對FS中的AI基本不產生影響,但噹Ni>1011 cm-3時,FS中MPI電子密度隨Ni增加而降低.在所研究的脈寬範圍τ∈[0.01,5]ps,AI是FS介質激光誘導損傷的主要機製.而對于BBS,噹脈寬τ∈[0.03,5]ps,AI是激光誘導損傷的主要機製;噹脈寬τ∈[0.01,0.03]ps,MPI在激光誘導損傷中佔主導地位.
기우전자밀도연화모형,차조수치방법,연구료비초격광작용하광학박막내적전자밀도연화과정,토론료초시전자밀도Ni화격광맥충관도τ대광학박막격광손상역치Fth적영향,분석료격광유도박막손상과정중MPI화AI적성질화작용.연구결과표명,대응우일정적맥관,존재일개림계초시전자밀도,당Ni저우저일림계밀도시,Fth불수Ni영향;당Ni고우림계밀도시,Fth수Ni증가이강저.림계초시전자밀도수착맥관적감소이증가.대우FS화BBS개질박막,Fth수맥관적증가이승고.초시전자밀도Ni대BBS중적MPI화AI기본몰유영향;동양Ni대FS중적AI기본불산생영향,단당Ni>1011 cm-3시,FS중MPI전자밀도수Ni증가이강저.재소연구적맥관범위τ∈[0.01,5]ps,AI시FS개질격광유도손상적주요궤제.이대우BBS,당맥관τ∈[0.03,5]ps,AI시격광유도손상적주요궤제;당맥관τ∈[0.01,0.03]ps,MPI재격광유도손상중점주도지위.
Based on electron density evolution model, the electron density evolution process induced by femtosecond laser pulse in optical dielectric films was studied by means of numerical method. The effects of initial electron density Ni and laser pulse width τ on damage threshold fluence Fth were analyzed respectively. Both the nature of multi-photon ionization (MPI) and the role of avalanche ionization (AI) were also discussed. The numerical analysis results show that, for a certain pulse width τ, there is a critical initial electron density below which Fth is not affected by Ni and above which Fth decreases with the increase of Ni The critical density rises with the decrease of pulse width τ. For the two dielectric films, the damage threshold fluence Fth rises with the increase of τ. Initial electron density Ni has little effect on MPI and AI for BBS. For FS, Ni has likewise little effect on AI, and MPI electron density decreases with the further increase of Ni for Ni>1011cm-3. For FS, the laser-induced-damage is dominated by AI for τ>0.01 ps, while for BBS, and MPI takes over for pulse durationτ below 0.03ps.