PL2250 闪光灯泵浦皮秒Nd:YAG激光器
PL2250 闪光灯泵浦皮秒Nd:YAG激光器
PL2250 闪光灯泵浦皮秒Nd:YAG激光器
PL2250 闪光灯泵浦皮秒Nd:YAG激光器
PL2250 闪光灯泵浦皮秒Nd:YAG激光器
PL2250 闪光灯泵浦皮秒Nd:YAG激光器
PL2250 闪光灯泵浦皮秒Nd:YAG激光器
PL2250 闪光灯泵浦皮秒Nd:YAG激光器

¥50万 - 100万

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PL2250

--

欧洲

  • 金牌
  • 第17年
  • 一般经销商
  • 营业执照已审核
核心参数

Features

  • Hermetically sealed DPSS master oscillator

  • Diode pumped regenerative amplifier

  • Flashlamp pumped power amplifier producing up to 100 mJ per pulse at 1064 nm

  • 30 ps pulse duration (20 ps optional)

  • Excellent pulse duration stability

  • Up to 50 Hz repetition rate

  • Streak camera triggering pulse with <30 ps jitter

  • Excellent beam pointing stability

  • Thermo stabilized second, third or fourth harmonic generator options

  • PC control via USB and LabVIEW&trade; drivers (RS232 control is optional)

  • Remote control via keypad

Applications

  • Time resolved spectroscopy

  • SFG/SHG spectroscopy

  • Nonlinear spectroscopy

  • OPG pumping

  • Remote laser sensing

  • Satellite ranging

  • Other spectroscopic and nonlinear optics experiments

 

PL2250 series lasers set a new standard in high pulse energy mode-locked picosecond lasers. Their innovative and cost-effective design improves laser reliability and reduces running and maintenance costs.

Innovative design

The heart of the system is a diode pumped solid state (DPSS) master oscillator placed in a hermetically sealed monolithic block. The flashlamp pumped regenerative amplifier is replaced by an innovative diode  pumped regenerative amplifier. Diode pumping results in negligible thermal lensing, which allows operation of the regenerative amplifier at variable repetition rates, as well as improved long-term stability and maintenance free operation.

The optimized multiple-pass power amplifier is flashlamp pumped and is optimized for efficient amplification of pulse while maintaining a near Gaussian beam profile and low wavefront distortion. The output pulse energy can be adjusted in approximately 1% steps from 1 mJ to nominal output, at the same time as pulse-to-pulse energy stability remains less than 0.8% rms at 1064 nm.

Angle-tuned KD*P and KDP crystals mounted in thermostabilised ovens are used for second, third and fourth harmonic generation. Harmonics separators ensure the high spectral purity of each harmonic directed to different output ports.

Built-in energy monitors continuously monitor output pulse energy. Data from the energy monitor can be seen on the remote keypad or PC monitor. The laser provides several triggering pulses for synchronization of the customer&lsquo;s equipment. The lead or delay of the triggering pulse can be adjusted in 0.25 ns steps from the control pad or PC. Up to 1000 &mu;s lead of triggering pulse is available as a pretrigger option.

Precise pulse energy control, excellent short-term and long-term stability, an up to 50 Hz repetition rate makes PL2250 series lasers an excellent choice for many demanding scientific applications.

Simple and convenient laser control

For customer convenience the laser can be controlled from a user-friendly remote control pad or USB interface. The remote pad allows easy control of all parameters and features a backlit display that is easy to read even while wearing laser safety eyewear.

Alternatively, the laser can be controlled from a personal computer with supplied software for a Windows&trade; operating system. LabVIEW&trade; drivers are supplied as well.

  • An experimental study has been conducted to study the effect of a swirling crossflow on transversely injected liquid jets. In-house designed axial swirlers with vane exit angles of 30&#176;, 45&#176; and 60&#176; were used to generate the swirling crossflow. Laser Doppler Velocimetry (LDV) results indicate that the axial (Ux) and the tangential (U&#952;) components of the crossflow velocity decrease with increasing radial distance from the center. Also, flow angle (&#968;) of the crossflow is lesser than the swirler vane exit angle indicating that the swirlers did not impart sufficient tangential momentum for the flow to be parallel to the vanes at swirler exit. The deficit in flow angle increased with swirler angle. Water jets were injected from a 0.5 mm diameter orifice located on a cylindrical centerbody that protruded through the hub of the swirler. Particle Image Velocimetry (PIV) was used to study the behavior of the jets. PIV measurements were conducted in multiple cross-sectional and streamwise planes. Mie-Scattering images were col-lated to create three-dimensional representation of the jet plume, which was used to study penetration. In cylindrical coordinate system, the penetration can be described in terms of radial and “circumferential” penetration, where cir-cumferential penetration is defined as the difference in the circumferential displacement of the jet and the crossflow over the same streamwise displacement. Increasing the momentum flux ratio (q) resulted in a higher radial penetra-tion. Increasing the swirl angle reduced radial penetration and increased circumferential penetration. PIV results of the cross-sectional and streamwise planes each yielded two velocity components which were merged to obtain three-dimensional droplet velocity distribution. The three-dimensional velocity distribution yielded further insight into the evolution of the jet plume

    其他 2011-02-13

  • 采用立陶宛Ekspla公司研制的由PL2251型脉冲皮秒激光器,和PG501型光学参量发生器为主构成的振动和频光谱(SFG)测量系统,对Cl&#175;, I&#175;, 和 F&#175;等负离子对1-丁醇单层/水界面结构的影响进行了实验测量和理论分析。

    石油/化工 2019-03-04

  • 采用立陶宛Ekspla公司PL2251A型脉冲皮秒Nd:YAG激光器和PG501型光学参量发生器构成的振动和频光谱测量系统(SFG)对花生酸朗缪尔单分子膜与三价离子La3+和Fe3+的相互作用进行了实验研究

    石油/化工 2019-03-07

  • 采用立陶宛Ekspla公司的由脉冲皮秒激光器PL2251-50和皮秒参量激光器PG401构成的振动和频光谱测量系统,对纤维素样品进行的测量分析揭示了纤维素表面层结构。

    石油/化工 2019-02-27

  • An experimental study has been conducted to study the effect of a swirling crossflow on transversely injected liquid jets. In-house designed axial swirlers with vane exit angles of 30&#176;, 45&#176; and 60&#176; were used to generate the swirling crossflow. Laser Doppler Velocimetry (LDV) results indicate that the axial (Ux) and the tangential (U&#952;) components of the crossflow velocity decrease with increasing radial distance from the center. Also, flow angle (&#968;) of the crossflow is lesser than the swirler vane exit angle indicating that the swirlers did not impart sufficient tangential momentum for the flow to be parallel to the vanes at swirler exit. The deficit in flow angle increased with swirler angle. Water jets were injected from a 0.5 mm diameter orifice located on a cylindrical centerbody that protruded through the hub of the swirler. Particle Image Velocimetry (PIV) was used to study the behavior of the jets. PIV measurements were conducted in multiple cross-sectional and streamwise planes. Mie-Scattering images were col-lated to create three-dimensional representation of the jet plume, which was used to study penetration. In cylindrical coordinate system, the penetration can be described in terms of radial and “circumferential” penetration, where cir-cumferential penetration is defined as the difference in the circumferential displacement of the jet and the crossflow over the same streamwise displacement. Increasing the momentum flux ratio (q) resulted in a higher radial penetra-tion. Increasing the swirl angle reduced radial penetration and increased circumferential penetration. PIV results of the cross-sectional and streamwise planes each yielded two velocity components which were merged to obtain three-dimensional droplet velocity distribution. The three-dimensional velocity distribution yielded further insight into the evolution of the jet plume

    其他 2011-02-13

  • We present two-dimensional measurements of the laser-induced plasma development and shock wave evolution in air. The breakdown is induced by a Q-switched Nd:YAG laser (&#955; = 1064 nm) with a pulse duration of 4 ns. To study these fast laser-induced phenomena, we have developed a high-speed, two frame shadowgraph method. It enables 2D visualization of a laser-induced event in two time instances, which are delayed by an arbitrary time interval in the range from 300 ps to 30 ns. The established method is based on 30 ps, green (&#955; = 532 nm), and linearly polarized laser pulse, which is split into two orthogonally polarized illumination pulses for direct and delayed illumination of the breakdown area. Exploiting polarization of the probe pulses, we capture two temporally and spatially separated frames with two CCD cameras. Special attention is given to the subsequent data processing, especially to the minimization of the systematic error due to alignment of both images, and to the determination of 2D velocity distribution from the captured image pairs.

    其他 2016-11-15

  • 采用立陶宛Ekspla公司的皮秒Nd:YVO4激光器,进行皮秒激光烧蚀四极质谱法深度分辨分析探测W7-X石墨组分中的氢成分的实验研究

    能源/新能源 2019-03-14

  • 本文利用EKSPLA-PL2251C (30 ps, 532 nm)激光器, 建立了激光阴影、纹影和干涉的诊断系统.开展了真空中负极性电流脉冲作用下铝单丝电爆炸的实验研究, 得到了不镀膜铝丝电爆炸的能量沉积过程.为了增加金属丝中的沉积能量, 也开展了相应的镀膜铝丝的实验研究.

    钢铁/金属 2018-01-29

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PL2250 闪光灯泵浦皮秒Nd:YAG激光器信息由北京欧兰科技发展有限公司为您提供,如您想了解更多关于PL2250 闪光灯泵浦皮秒Nd:YAG激光器报价、型号、参数等信息,欢迎来电或留言咨询。
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