飛秒激光強場中高次諧波課件

飛秒激光強場中的高次諧波飛秒激光強場中高次諧波課件高次諧波(High-orderHarmonicGeneration)

概念:

由某一基頻光與非線性物質(zhì)作用而輻射出一系列的頻率是基頻光整數(shù)倍的光。(VUV,EUV,softandhardX-ray)

Theatomessentiallyactsasacatalysttocombinemanylow-energyphotonsfromthedrivinglaserintoasinglehigh-energyphoton意義:高次諧波產(chǎn)生是獲得相干的極紫外和X射線輻射的主要的和最有前途的途徑之一。

產(chǎn)生阿秒(10-18s)脈沖高次諧波(High-orderHarmonicGene一、產(chǎn)生/機制二、特點/規(guī)律三、研究/進展飛秒激光強場中高次諧波飛秒激光強場中高次諧波實驗室產(chǎn)生示意圖IntensefslaserGasjet(Xe)HarmonicgenerationFilterCCDHigh-orderharmonics(A)實驗室產(chǎn)生示意圖IntensefslaserGasje強宏觀……產(chǎn)生/機制強宏觀……產(chǎn)生/機制Corkum,Phys.Rev.Lett.71,1994(1993)Lewenstein,Phys.Rev.A49,2117(1994)三步模型簡介(Instrongfield0ffemtosecondlaser)1.Fieldtunnelionizationofelectron()2.Electronoscillateinlaserfield(accelerate)3.Electronre-collidewithionatom,(recombines)Step1Step2Step3產(chǎn)生/機制Corkum,Phys.Rev.Lett.71,1特點/規(guī)律1.Oddharmonics2.Plateau3.CutoffenergyPhys.Rev.Lett.71,1994(1993)tTL傅立葉變換特點/規(guī)律1.OddharmonicsPhys.Rev.4.Shortlightpulses---Attosecond(10-18s)特點/規(guī)律脈沖寬度小于等于驅(qū)動場4.Shortlightpulses---Attos研究/進展Phys.Rev.Lett.70(6),766(1993)1993更短波長(截止區(qū)）更高的效率（平臺區(qū)）更短脈沖（阿秒脈沖--平臺區(qū)、截止區(qū)）806nm

125fs

1.3x1015W/cm2

Ne109th-7.4nm

研究/進展Phys.Rev.Lett.70(6),7Science,278,661(1997)1997179th-4.4nm更短波長研究/進展短脈沖(5fs)Science,278,661(1997)1997179Nature406,164(2000)27th更高效率研究/進展2000脈沖形狀Nature406,164(2000)27th更高效率Science,302,95(2003)2003更高效率研究/進展相位匹配Science,302,95(2003)2003更高效2005Nature,433,597(2005)Phys.Rev.A71,061840(2005)更短波長更高效率1nm研究/進展NSPM2005Nature,433,597(2005)Phys研究/進展Science,302,1540(2003)更短脈沖-阿秒脈沖的產(chǎn)生2001-2003研究/進展Science,302,1540(2003)Phys.Rev.Lett.94,243901(2005)Phys.Rev.Lett.94,193201(2005)Phys.Rev.Lett.94,173903(2005)Nature,433,596,2005Nature,436,234,2005Phys.

Rev.A71,063807(2005)Phys.

Rev.A72,033817(2005)Phys.

Rev.A73,043411(2006)J.Phys.B:At.Mol.Opt.Phys.39,3983(2006)Science,312,424(2006)研究/進展~200aspulse+fspulse熱Phys.Rev.Lett.94,243901(20飛秒激光強場中的高次諧波飛秒激光強場中高次諧波課件高次諧波(High-orderHarmonicGeneration)

概念:

由某一基頻光與非線性物質(zhì)作用而輻射出一系列的頻率是基頻光整數(shù)倍的光。(VUV,EUV,softandhardX-ray)

Theatomessentiallyactsasacatalysttocombinemanylow-energyphotonsfromthedrivinglaserintoasinglehigh-energyphoton意義:高次諧波產(chǎn)生是獲得相干的極紫外和X射線輻射的主要的和最有前途的途徑之一。

產(chǎn)生阿秒(10-18s)脈沖高次諧波(High-orderHarmonicGene一、產(chǎn)生/機制二、特點/規(guī)律三、研究/進展飛秒激光強場中高次諧波飛秒激光強場中高次諧波實驗室產(chǎn)生示意圖IntensefslaserGasjet(Xe)HarmonicgenerationFilterCCDHigh-orderharmonics(A)實驗室產(chǎn)生示意圖IntensefslaserGasje強宏觀……產(chǎn)生/機制強宏觀……產(chǎn)生/機制Corkum,Phys.Rev.Lett.71,1994(1993)Lewenstein,Phys.Rev.A49,2117(1994)三步模型簡介(Instrongfield0ffemtosecondlaser)1.Fieldtunnelionizationofelectron()2.Electronoscillateinlaserfield(accelerate)3.Electronre-collidewithionatom,(recombines)Step1Step2Step3產(chǎn)生/機制Corkum,Phys.Rev.Lett.71,1特點/規(guī)律1.Oddharmonics2.Plateau3.CutoffenergyPhys.Rev.Lett.71,1994(1993)tTL傅立葉變換特點/規(guī)律1.OddharmonicsPhys.Rev.4.Shortlightpulses---Attosecond(10-18s)特點/規(guī)律脈沖寬度小于等于驅(qū)動場4.Shortlightpulses---Attos研究/進展Phys.Rev.Lett.70(6),766(1993)1993更短波長(截止區(qū)）更高的效率（平臺區(qū)）更短脈沖（阿秒脈沖--平臺區(qū)、截止區(qū)）806nm

125fs

1.3x1015W/cm2

Ne109th-7.4nm

研究/進展Phys.Rev.Lett.70(6),7Science,278,661(1997)1997179th-4.4nm更短波長研究/進展短脈沖(5fs)Science,278,661(1997)1997179Nature406,164(2000)27th更高效率研究/進展2000脈沖形狀Nature406,164(2000)27th更高效率Science,302,95(2003)2003更高效率研究/進展相位匹配Science,302,95(2003)2003更高效2005Nature,433,597(2005)Phys.Rev.A71,061840(2005)更短波長更高效率1nm研究/進展NSPM2005Nature,433,597(2005)Phys研究/進展Science,302,1540(2003)更短脈沖-阿秒脈沖的產(chǎn)生2001-2003研究/進展Science,302,1540(2003)Phys.Rev.Lett.94,243901(2005)Phys.Rev.Lett.94,193201(2005)Phys.Rev.Lett.94,173903(2005)Nature,433,596,2005Nature,436,234,2005Phys.

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