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Method for Generation of femtosecond pulses of laser Light Source, and the same

机译:飞秒激光光源的产生方法及其

摘要

Method for generating femtosecond Light pulses, which comprises at least two stages of optical Parametric amplification (OPA)In the Parametric Amplification is performed in a First Stage OPA conducting optically synchronized Radiation pulses First SEED (9) and First Pumping Radiation (7) to a PFirst non-linear Crystal (3) that overlap in time and Space, satisfying conditions of non collinear Phase matching.Parametric Amplification was performed in a Second Stage OPA conducting optically synchronized Radiation pulses of Second SEED (28) and second Pumping Radiation (10) to a Second CRistal nonlinear (4) that overlap in time and Space satisfying conditions of non collinear Phase matching.Outgoing Radiation Pulse Wave Signal amplified in a final stage of Opa, which is at least the second stage BID, compress to output pulses of femtosecondWhere the first and second Radiation SEED (9, 28) and first and second Pumping Radiation (710) originate from a single laser Source (1) dividing the primary Radiation of ultrashort (11) the primary source of laser (1) with a power divider (12) (13) or radiationN Seed Radiation arm and an arm (14) pumpingThe First Radiation SEED (9) for the first stage OPA is delaying time of the Radiation pulses (13) Arm of seedWhile the first Pumping Radiation (7) for the first stage OPA is Amplifying and Doubling the frequency of the Radiation (14) of the pump arm in a Second GeneratorRmu00f3nico (20),The Second Radiation SEED (28) for the second stage OPA compressing pulses in the form of Long Wave Radiation Amplified Signal (24) in said First non-linear Crystal (3) fOtmar Radiation pulse femtosecond (26) and also by Spectral widening of a portion (30) of the Radiation PULSE GENERATOR (26) a femtosecond White Light (6) to create RadiAtion spectrally Expanded (27) with Band width of not less than 300 nm and heading towards the second nonlinear Crystal (4) directly or through a First pulse Conditioner (33),In this laser Source (1) is a primary source of Low Energy laser Radiation of ultrashort,Characterized by selecting a Central Wavelength of the Radiation u03bb0 ultrashort (11) of the laser Source (1) to superimpose a primary Peak of Stimulated Emission of a medium.Vo High Gain Solid State, and its Spectral width u0394u03bb0 corresponds to a Pulse duration was limited to 1PS 3PS,The formation of the first Radiation SEED (9) (13) of the Radiation ARM further comprises Seed to widen their Spectrum (10u00f720 nm bandwidth)A Spectral bandwidth of the Radiation arm (14) of the pump, which is Amplified during the formation of the first Radiation Pumping (7), not exceeding 1nm,The Second Pumping Radiation (10) to create the pulse duration in the range femtosecondIt is formed from the amplified in the first stage of Opa and compressed pulse femtosecond Radiation (26) Separating part (31) by a power divider (29) and heading towards aSecond Harmonic Generator (32) for Doubling frequencyThe Frequency doubled Radiation towards the second nonlinear Crystal (4) directly or through a Second Conditioning pulses (34)The relationship of pulse durations of pumping and Seed is in a range of 1 to 10, which is achieved by the first and / or second Conditioning pulse (3334) that include pulse Compressors and / or dilators of pulse; Pulse Wave Signal, amplified in the end at least in the second nonlinear Crystal (4),Compressed in time to form output pulses with a duration of 5fs to 100fs.
机译:产生飞秒光脉冲的方法,该方法至少包括两级光学参量放大(OPA)。在第一级OPA中执行参量放大,将光学同步辐射脉冲First SEED(9)和First Pumping Radiation(7)传输到P第一非线性晶体(3)在时间和空间上重叠,满足非共线相位匹配的条件。在第二级OPA中进行参数放大,传导第二SEED(28)的光同步辐射脉冲和第二泵浦辐射(10)到第二CRistal非线性(4),其在时间和空间上重叠,满足非共线相位匹配的条件。在Opa的最后阶段(至少是第二阶段BID)中放大的输出辐射脉冲波信号压缩为飞秒输出的脉冲第一和第二辐射SEED(9,28)以及第一和第二泵浦辐射(710)源自将原色分割的单个激光源(1)超短辐射(11)具有功率分配器(12)(13)或辐射的主要激光源(1)的辐射N种子辐射臂和臂(14)抽运第一级OPA的第一辐射SEED(9)正在延迟辐射脉冲的时间(13)种子臂的时间,同时第一阶段OPA的第一泵浦辐射(7)将第二个发生器中泵臂的辐射(14)的频率放大和加倍Rm u00f3nico(20),第二辐射SEED(28)用于第二级OPA压缩脉冲,其形式为所述第一非线性晶体(3)中的长波辐射放大信号(24)fOtmar辐射脉冲飞秒(26),并且还通过一部分光谱扩展(30)辐射脉冲发生器(26)的飞秒白光(6)产生光谱扩展后的RadiAtion(27),其带宽不小于300 nm,并且直接或通过第一晶体向第二非线性晶体(4)前进脉冲调节器(33),在此激光源(1)是主要光源低能量的超短能量激光辐射的特征,其特征在于选择激光源(1)的辐射的中心波长(11)叠加介质的受激发射主峰。Vo高增益固态及其光谱宽度 u0394 u03bb0对应于一个脉冲持续时间限制为1PS 3PS,辐射ARM的第一个辐射SEED(9)(13)的形成进一步包括种子以扩宽其光谱(10 u00f720 nm带宽)泵的辐射臂(14)的带宽,在第一次辐射泵浦(7)形成期间被放大,不超过1nm,第二次泵浦辐射(10)在飞秒范围内产生脉冲持续时间通过功率分配器(29)在Opa的第一级中放大并压缩飞秒飞秒辐射(26)分离部分(31)并向第二谐波发生器(32)前进以使频率加倍朝向secon的倍频辐射d非线性晶体(4)直接或通过第二调节脉冲(34)抽运与种子的脉冲持续时间之间的关系在1到10的范围内,这是通过第一和/或第二调节脉冲(3334)实现的包括脉冲压缩器和/或脉冲扩张器;最后至少在第二个非线性晶体(4)中放大的脉搏波信号,及时压缩以形成5fs至100fs持续时间的输出脉冲。

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