国产成人综合欧美精品久久,粉嫩av一区二区三区在线看,欧美色图人妻交换,女人羞羞免费视频

全國服務(wù)咨詢熱線:

15618996225

當(dāng)前位置:首頁  >  產(chǎn)品中心  >  光學(xué)元器件  >  光學(xué)晶體  >  PPLN晶體,非線性晶體

晶體,非線性晶體

簡要描述:晶體,非線性晶體基于準相位匹配(QPM),使新的波生成和xx型譜是困難的或不可能的工程實現(xiàn)由傳統(tǒng)的非線性材料。xx型芯片和全譜(LN、LT:氧化鎂:鎂和適當(dāng)?shù)姆蔷€性頻率轉(zhuǎn)換計劃)(DFG SFG,倍頻、OPO,收購,聯(lián)合,一個CAN,等),實現(xiàn)期望的輸出波長(紫外/可見到/從太赫茲光譜反演和特殊功能(),兩個頻譜轉(zhuǎn)換。頻譜工程等)有效。

  • 產(chǎn)品型號:PPLN
  • 更新時間:2025-03-12
  • 訪  問  量:1531

產(chǎn)品簡介

品牌其他品牌供貨周期兩周
應(yīng)用領(lǐng)域環(huán)保,化工,電子/電池

詳細介紹

晶體,非線性晶體基于準相位匹配(QPM),使新的波生成和xx型譜是困難的或不可能的工程實現(xiàn)由傳統(tǒng)的非線性材料。xx型芯片和全譜(LN、LT:氧化鎂:鎂和適當(dāng)?shù)姆蔷€性頻率轉(zhuǎn)換計劃)(DFG SFG,倍頻、OPO,收購,聯(lián)合,一個CAN,等),實現(xiàn)期望的輸出波長(紫外/可見到/從太赫茲光譜反演和特殊功能(),兩個頻譜轉(zhuǎn)換。頻譜工程等)有效。
      HCP提供以下全光譜configurations xx型散裝芯片來滿足你的應(yīng)用要求和規(guī)格。我們可以幫助你設(shè)計結(jié)構(gòu)合適的外加電壓和外加電壓為選定的時間獲得所需的材料/ PPLT極化相匹配的操作溫度和光譜.思考與輸入和輸出功率/能量/脈沖以及它們的光譜特性。請為您的特殊要求,也具有挑戰(zhàn)。
PPXX Bulk Chips
晶體,非線性晶體
HCP PPLN
Ref-1: Materials and Application Wavelength
Materials and Application Wavelength
?Ref-2:  Chip Structure
Chip Structure
Ref-3: Conversion Configuration
Ref-4: Dimension and Surface Specification 
Ref-4: Dimension and Surface Specification
_______________________________________________________________________________________???
  1. 什么是 PPXX 技術(shù)

    PPXX is an advanced technology for high efficiency and arbitrary wavelength conversion based on making engineered microstructure on the ferroelectric materials.

2. 非線性波長轉(zhuǎn)換

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:

公式1 

Here are the common nonlinear process appellations and its expression of frequency relation respectively.

Second Harmonic Generation

3. 相位匹配條件

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.

 相位匹配條件  

4.雙折射相位匹配(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.The polarization of the two low frequency photon is the same

Type II:  The polarization of the two low frequency photon is different,

i.e.The polarization of the two low frequency photon is different


5. 準相位匹配(QPM)和周期性極化(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.

準相位匹配(QPM)和周期性極化(PP) 

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 準相位匹配(QPM)和周期性極化(PP) 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. 什么樣的色散方程,我們使用的折射率計算?

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. 如何計算 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):

什么樣的色散方程,我們使用的折射率計算 

Then, the QPM period equals to

什么樣的色散方程,我們使用的折射率計算 

Which the final wave vector mismatch is canceled

qpm 


8. 如何實現(xiàn)轉(zhuǎn)換效率?


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

 PPLN

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.  如何實現(xiàn)波長調(diào)諧?


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.  


產(chǎn)品咨詢

留言框

  • 產(chǎn)品:

  • 您的單位:

  • 您的姓名:

  • 聯(lián)系電話:

  • 常用郵箱:

  • 省份:

  • 詳細地址:

  • 補充說明:

  • 驗證碼:

    請輸入計算結(jié)果(填寫阿拉伯?dāng)?shù)字),如:三加四=7

全國統(tǒng)一服務(wù)電話

021-62209657

電子郵箱:sales@eachwave.com

公司地址:上海市閔行區(qū)劍川路955號707-709室

業(yè)務(wù)咨詢微信

久久99精品久久久久婷综合| 美女扒开粉嫩尿口桶爽| 欧美成人免费网站一区二区| 一区无码精品色在线观看| 大鸡巴插进美逼无码网站| 一级午夜福利视频免费区| 洗澡岳呻吟求饶| 性欧美另丰满69xxxxx| 美女av免费一区二区三区| 亚洲欧美在线观看免费观看| 亚洲欧美另类日本人人澡| 日产精品一卡2卡三卡4乱码| 我要我们在一起在线观看免费 | 精品国产成人福利免费看| 被添出水全过程视频| 美女脱一光二净18以上| 亚洲乱亚洲乱妇一23p| 一区二区三区羞羞的视频| 青青草青青草青青草| 水野优香一区二区视频| 99av成人精品国语自产拍| 青青草青青草青青草| 日韩 欧美 亚洲 高清 | 少妇搡bbbb搡bbbb搡冒白浆| 亚洲 综合 另类 小说| 久久无码综合| 九九热五十熟妇人妻精品| 亚洲精品国产一区二区电影| 护士的色诱2在线观看免费| 黄页网站在线免费观看骚| 红楼梦听书全集播放免费| 午夜爽爽爽影院| 欧美精品视频在线观亚洲| 老九门二免费观看全集电视剧剧情| 国内精品国产三级KTV| 女王榨精—视频丨vk| 樱花草涩涩www在线播放| 意大利人妻未删减完整| 久久av色欲av久久蜜桃麻豆| 色综合久久网| 精品亚洲区二区中文字幕|