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光纤飞秒激光器
半导体参数分析仪
磁克尔综合测试平台
X射线
镀膜与加工
光学元器件
光纤通信与传感
光谱影像
超快调制与测量
- 超快激光压缩光栅
- 光子晶体光纤
- 超快激光镜片
- 超短脉冲测量仪FROG
- 自相关仪
- 超快激光同步器
- 其他超快调制与测量
- 谐波产生倍频器
- 脉冲选择器
- 半导体可饱和吸收镜SESAM
- 脉冲展宽器脉冲压缩器
- CFBG啁啾光纤光栅
激光调制与测量
传统激光器
皮秒激光器
- 高能量皮秒激光器
- 高功率窄线宽皮激光器
- 高重频固态锁模皮秒激光器
- Microchip微片皮秒激光器
- 可调谐皮激光器OPO
- 皮秒超连续谱激光器
- 高功率皮秒激光器
- 半导体皮秒激光器
- DPSS固态皮秒激光器
- Kanata皮秒激光器
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飞秒激光器
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- TW太瓦飞秒放大系统
- 1.2um飞秒激光器
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- GHz高重频光纤飞秒激光器
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- 飞秒再生放大器
- NKT飞秒光纤激光器
太赫兹器件
- 其他太赫兹元件
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太赫兹设备
详细内容
- 什么是 PPXX 技术
PPXX is an advanced technology for high efficiency and arbitrary wavelength conversion based on making engineered microstructure on the ferroelectric materials.
2. 非线性波长转换
Nonlinear wavelength conversion means the phenomenon that input light generates new wavelength via passing through the nonlinear material. For the common 2nd order nonlinearity, photon energy of the related wavelength is defined to be conserved as the relation below:
Here are the common nonlinear process appellations and its expression of frequency relation respectively.
3. 相位匹配条件
To have high conversion efficiency, the photon momentum should be conserved as well. Otherwise, incorrect phase will lead to destructive interference causing very low efficiency. The relation of photon momentum conservation is shown as below, which is called the phase matching condition.
4.双折射相位匹配(BPM)
Typically, due to the material feature of dispersion, phase matching condition could only be achieved in the birefringence material, which has different refractive index of its o-polarization (perpendicular to the optical axis) and e-polarization (parallel to the optical axis).
The phase matching condition could be achieved by changing temperature or the incident angle on the birefringence material with correct polarization. Two types of phase matching condition are shown as below:
Type I: The polarization of the two low frequency photon is the same,
i.e.
Type II: The polarization of the two low frequency photon is different,
i.e.
5. 准相位匹配(QPM)和周期性极化(PP)
Quasi phase matching is a technique that the photon momentum conservation is achieved through additional artificial structure. The structure could provide an extra vector Kg which matches the momentum conservation as below.
Periodical poling is a special technique to form periodical microstructure on the ferroelectric material with a designed Kg. Not only the spatial walk-off issue in BPM material becomes eliminated through QPM technique but the phase matching temperature could also be designed. Moreover, the type of phase matching condition (Type 0), which is never existing in BPM (Birefringence phase matching) could be demonstrated through QPM. Type 0 is bringing about several tens of times for conversion efficiency enhancement.
6. 什么样的色散方程,我们使用的折射率计算?
We simulate the refractive index according to the reference below, which is the most appropriate function through our experience.
Gayer, O., et al, "Temperature and wavelength dependent refractive index equations for MgO-doped congruent and stoichiometric LiNbO3." Appl. Phys. B 91, 343-348 (2008)
7. 如何计算 QPM 期?
First you will need the information of the refractive index to calculate the wave vector mismatch of the involved wavelength. For example (up-conversion):
Then, the QPM period equals to
Which the final wave vector mismatch is canceled
8. 如何实现*优转换效率?
To achieve the optimal conversion efficiency, the incident light should be focused on the center of the chip with the focusing condition L/b~2.84, where L is the chip length, b is the Gaussian beam focusing parameter. The above condition is for SHG/SFG only and with the assumption of Gaussian beam M2=1. For DFG, the optimal condition is more complicated and will change according to the wavelength, for further study, one can read the reference below.
T. -B. Chu and M. Broyer, "Intracavity cw difference frequency generation by mixing three photons and using Gaussian laser beams." J. Phys. (Paris) 46, 523 (1985)
9. How to know the acceptance of the chip?
The phase matching spectrum is the square of a sinc function
We know that once we design a QPM period for a target wavelength conversion, , and then we could calculate the wave vector mismatch near the designed wavelength to see when the becomes large enough that the square of sinc function becomes smaller than 0.5.
10. 如何实现波长调谐?
There are two ways for wavelength tuning. One is changing the period, the other one is changing the temperature (because the refractive index is a function of temperature).
Typically, the temperature tuning could not have wide tuning range, so we have special structures - multiple and fan-out, to achieve broadband wavelength tuning.
Multiple structure is a chip with multiple channel, each channel has different period, through the change of the incident channel and modifying the temperature, one can achieve large tuning range then a single period chip.
Fan-out structure is a chip with continuous period change in the width. One can tune the phase matching wavelength through moving the chip without changing the temperature.