Avesta YFOA型 飞秒光纤激光器
Avesta YFOA型 飞秒光纤激光器

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YFOA

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YFOA型 飞秒光纤激光器

 

 

YFOA飞秒光纤激光器生产商简介:

      AVESTA公司的超快激光技术引自俄罗斯 P.N.列别捷夫物理研究所量子无线电物理部,该公司于1900年由Basov和Prokhorov两位诺贝尔奖获得者创建,总部位于俄罗斯西南的学术小镇Troitsk。

      公司致力于超快激光技术的发展,并为全球科研及工业客户提供专业产品。产品涵盖飞秒光纤激光器,钛宝石飞秒激光器、放大器,自相关仪,三阶互相关仪,脉冲选择器等。

 

 

YFOA飞秒光纤激光器产品介绍:

      YFOA飞秒光纤激光器专门用来产生稳定的超短激光脉冲序列。该系统包含掺Yb有源光纤,泵浦二极管,偏振控制和色散控制元件,电子电源和控制系统。该型激光器具有可用于触发外部设备的SMA同步输出组件,以及另一个用来控制脉冲模式状态的SMA。

      无论是作为放大系统(如TETA系统)的种子振荡器,或是作为独立的脉冲发生器, YFOA飞秒光纤激光器都具有非常好的可靠性。另外,若有需要,YFOA飞秒光纤激光器还可以扩展为更高的额定平均功率。


YFOA飞秒光纤激光器产品特点

      波长范围:1030-1064nm(固定)

      平均功率最高可达5W

      峰值功率最高可达260 kW

      体积小

      操作简单

      高稳定性


YFOA飞秒光纤激光器技术参数

型号:

YFOA-100

YFOA-200

YFOA-5000

脉宽 (FWHM)

<200 fs

<350 fs

波长*

1030;1040;1053;1064 nm

平均输出功率

>100 mW

>200 mW

>5000 mW

峰值功率

>8.5 kW

>17 kW

>260 kW

重复率(固定)

60±5 MHz

空间模式

TEM00

偏振

线性,水平

输出类型

自由空间

激光器尺寸, mm

200×200×70

200×200×100

350×200×120

电源尺寸, mm

230×200×90

230×200×130

470×385×155

* - 请选择波长,可根据客户要求定制。

 

 

YFOA飞秒光纤激光器产品应用

      种子振荡器

      太赫兹产生和检测

      光学计量

      半导体设备测试

      超连续光谱产生

      光学相干断层扫描成像

      多光子显微镜

    “泵浦-探测”光谱

 

典型用户
用户单位 采购时间
63672部队 2015-03-11
长春新产业光电技术有限公司 2014-12-10
中国科学院上海应用物理研究所 2016-11-18
福州高意通讯有限公司 2016-05-18
售后服务承诺

保修期: 1年

是否可延长保修期:

现场技术咨询:

免费培训: 1

免费仪器保养: 1

保内维修承诺: 1

报修承诺: 1

  • Spectrally correlated photon pairs can be used to improve the performance of long-range fiber-based quantum communication protocols. We present a source based on spontaneous parametric downconversion, which allows one to control spectral correlations within the entangled photon pair without spectral filtering by changing the pump-pulse duration or the characteristics of the coupled spatial modes. The spectral correlations and polarization entanglement are characterized. We find that the generated photon pairs can feature both positive spectral correlations,decorrelation, or negative correlations at the same time as polarization entanglement with a high fidelity of 0.97 (no background subtraction) with the expected Bell state.

    453MB 2017-03-24
  • Multidimensional visible spectroscopy using pulse shaping to produce pulses with stable controllable phases and delays has emerged as an elegant tool to acquire electronic spectra faster and with greatly reduced instrumental and data processing errors. Recent migration of this approach using acoustooptic modulator (AOM) pulse shaping to the mid-infrared region has proved useful for acquiring two dimensional infrared (2D IR) vibrational echo spectra. The measurement of spectral diffusion in 2D IR experiments hinges on obtaining accurate 2D line shapes.

    551MB 2017-03-24
  • We report on the generation of broadband, high-energy femtosecond pulses centered at 1.28 &#956;m by stimulated Raman scattering in a pressurized hydrogen cell. Stimulated Raman scattering is performed by two chirped and delayed pulses originating from a multi-mJ Ti:sapphire amplifier.The Stokes pulse carries record-high energy of 4.4 mJ and is recompressed down to 66 fs by a reflective grating pair. We characterized the short-wavelength mid-infrared source in view of energy stability, beam profile, and conversion efficiency at repetition rates of 100 and 10 Hz. The demonstrated high-energy frequency shifter will benefit intense THz sources based on highly nonlinear organic crystals.

    1552MB 2017-03-24
  • In this work we report a new method for controlling the bandwidth of few-cycle optical pulses, using another femtosecond laser pulses chirped in a neonfilled hollow-core fibre. The observed bandwidth varies from 25 to 234 nm in the optical wavelength region 600–950 nm. The pulse energy has for the first time reached a sub-millijoule frontier at 1 kHz. The input pulses are positively chirped using a chirped-pulse amplifier to acquire the widths 32–56 fs at the entrance of the hollow fibre. Then the pulses are highly dispersed due to a self-phase modulation in a nonlinear medium (a neon gas) followed by a pair of chirped mirrors that compensate the dispersion. We have found that this scheme allows for direct tuning of the output-pulse bandwidth while varying the chirping of the input pulses under different neon-gas pressures.

    893MB 2017-03-24
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