红外与激光工程
紅外與激光工程
홍외여격광공정
INFRARED AND LASER ENGINEERING
2014年
1期
184-189
,共6页
徐明明%江庆五%刘文清%张寅超%陈结祥%曾议
徐明明%江慶五%劉文清%張寅超%陳結祥%曾議
서명명%강경오%류문청%장인초%진결상%증의
双光栅%色散公式%光谱分离%像差校正
雙光柵%色散公式%光譜分離%像差校正
쌍광책%색산공식%광보분리%상차교정
double grating%dispersion formula%spectrum separation%aberration correction
由于所需测量的光谱范围较宽(276~700 nm ),而CCD探测器的接收面尺寸较小(14.3 mm ×10.5 mm),根据所选用的平面光栅元件参数,采用传统的车尔尼-特纳型结构是无法满足的。基于该结构,利用光线相对光栅的入射角和衍射角与光栅转角的关系,提出了使用两块反射式平面光栅进行光谱分离的方法。通过理论计算,确定了两段光谱范围和两光栅的旋转及俯仰角度,采用ZEMAX软件建立多重结构,分别设置两块光栅的位置和波长参数,对光学系统进行了模拟分析和优化。结果表明,在像面上得到了两条谱面线展宽为14 mm,中心间距8 mm的光谱带,光谱分辨率优于1 nm,各像差得到了充分校正,满足设计指标要求,很好地解决了宽光谱和探测器接收面尺寸之间的矛盾。
由于所需測量的光譜範圍較寬(276~700 nm ),而CCD探測器的接收麵呎吋較小(14.3 mm ×10.5 mm),根據所選用的平麵光柵元件參數,採用傳統的車爾尼-特納型結構是無法滿足的。基于該結構,利用光線相對光柵的入射角和衍射角與光柵轉角的關繫,提齣瞭使用兩塊反射式平麵光柵進行光譜分離的方法。通過理論計算,確定瞭兩段光譜範圍和兩光柵的鏇轉及俯仰角度,採用ZEMAX軟件建立多重結構,分彆設置兩塊光柵的位置和波長參數,對光學繫統進行瞭模擬分析和優化。結果錶明,在像麵上得到瞭兩條譜麵線展寬為14 mm,中心間距8 mm的光譜帶,光譜分辨率優于1 nm,各像差得到瞭充分校正,滿足設計指標要求,很好地解決瞭寬光譜和探測器接收麵呎吋之間的矛盾。
유우소수측량적광보범위교관(276~700 nm ),이CCD탐측기적접수면척촌교소(14.3 mm ×10.5 mm),근거소선용적평면광책원건삼수,채용전통적차이니-특납형결구시무법만족적。기우해결구,이용광선상대광책적입사각화연사각여광책전각적관계,제출료사용량괴반사식평면광책진행광보분리적방법。통과이론계산,학정료량단광보범위화량광책적선전급부앙각도,채용ZEMAX연건건립다중결구,분별설치량괴광책적위치화파장삼수,대광학계통진행료모의분석화우화。결과표명,재상면상득도료량조보면선전관위14 mm,중심간거8 mm적광보대,광보분변솔우우1 nm,각상차득도료충분교정,만족설계지표요구,흔호지해결료관광보화탐측기접수면척촌지간적모순。
Due to the onconflict between the wide spectral range of measuring (276-700 nm) and the limited imaging area of CCD detector (14.3 mm ×10.5 mm), classical Czerny-Turner structure was not able to meet the requirements of design. Based on it, an innovative method applying two uniform plane diffraction gratings to separate the whole spectral range into two different sections was presented. The two separate spectral range, rotation and tilt angles of two gratings were obtained through theoretical computation. The optical software ZEMAX was used to simulate and optimize the optical system by multiple configuring parameters. The simulation results show that two spectral bands are detected on the imaging plane. Their spectrum width is 14 mm respectively, and the center distance between them is 8 mm. The spectral resolution is less than 1 nm and the aberration is substantially corrected. It indicates that the method is a good solution for the situation of wide spectral measurement range and limited imaging dimension of CCD detector in the meanwhile.