红外与激光工程
紅外與激光工程
홍외여격광공정
INFRARED AND LASER ENGINEERING
2013年
3期
805-809
,共5页
马晶%王健%谭立英%于思源%姜义君
馬晶%王健%譚立英%于思源%薑義君
마정%왕건%담립영%우사원%강의군
卫星光通信%最优超声功率%空间傅里叶变换%声光偏转器%超声吸收
衛星光通信%最優超聲功率%空間傅裏葉變換%聲光偏轉器%超聲吸收
위성광통신%최우초성공솔%공간부리협변환%성광편전기%초성흡수
inter-satellite optical communications%optimal ultrasonic power%spatial Fourier transform approach%acousto-optic deflector%ultrasonic attenuation
分别在不考虑晶体超声吸收及考虑超声吸收和超声功率角分布的情况下,建立了声光互作用方程.运用空间傅里变换方法推导出衍射光场与入射光场在空频下的传递函数.仿真结果表明,超声吸收使得衍射光光强峰值位置偏离光束中心,光强不再呈高斯分布,会引起卫星光通信发射端的指向偏差.通过研究超声功率和频率与衍射光光强分布的关系发现,超声功率选取某一数值时可以消除峰值位置偏差,将此功率值定义为最优超声功率Popt.求出声光偏转器整个工作频带内的Popt并进行多项式拟合,得到了最优超声功率与超声频率的关系.按照该多项式关系同步调节超声频率与功率可以补偿超声吸收引起的指向偏差.
分彆在不攷慮晶體超聲吸收及攷慮超聲吸收和超聲功率角分佈的情況下,建立瞭聲光互作用方程.運用空間傅裏變換方法推導齣衍射光場與入射光場在空頻下的傳遞函數.倣真結果錶明,超聲吸收使得衍射光光彊峰值位置偏離光束中心,光彊不再呈高斯分佈,會引起衛星光通信髮射耑的指嚮偏差.通過研究超聲功率和頻率與衍射光光彊分佈的關繫髮現,超聲功率選取某一數值時可以消除峰值位置偏差,將此功率值定義為最優超聲功率Popt.求齣聲光偏轉器整箇工作頻帶內的Popt併進行多項式擬閤,得到瞭最優超聲功率與超聲頻率的關繫.按照該多項式關繫同步調節超聲頻率與功率可以補償超聲吸收引起的指嚮偏差.
분별재불고필정체초성흡수급고필초성흡수화초성공솔각분포적정황하,건립료성광호작용방정.운용공간부리변환방법추도출연사광장여입사광장재공빈하적전체함수.방진결과표명,초성흡수사득연사광광강봉치위치편리광속중심,광강불재정고사분포,회인기위성광통신발사단적지향편차.통과연구초성공솔화빈솔여연사광광강분포적관계발현,초성공솔선취모일수치시가이소제봉치위치편차,장차공솔치정의위최우초성공솔Popt.구출성광편전기정개공작빈대내적Popt병진행다항식의합,득도료최우초성공솔여초성빈솔적관계.안조해다항식관계동보조절초성빈솔여공솔가이보상초성흡수인기적지향편차.
Acousto-optic interaction equations were established separately under two situations of without or with the consideration of ultrasonic attention and the angular distribution of ultrasonic power. The transfer function in spatial-frequency domain between the diffracted light and incident light was derived by employing spatial Fourier transform approach. Numerical simulation was performed. The results indicate that due to ultrasonic attenuation, the peak intensity of diffracted light deviates from the center of the beam and the distribution of diffracted light intensity is not Gaussian type any more, which leads to the pointing deviation of transmitting terminal in inter-satellite optical communications. The study of the dependence of the distribution of diffracted light intensity on ultrasonic power and ultrasonic frequency shows that the peak intensity deviation of the diffracted light can be eliminated when a certain value is chosen for the ultrasonic power. This certain value was defined as the optimal ultrasonic power Popt. The relation between optimal ultrasonic power and ultrasonic frequency was given by applying a polynomial fitting to various Popt in the whole bandwidth of acousto-optic deflector. The pointing deviation due to ultrasonic attenuation can be compensated by adjusting the ultrasonic frequency and ultrasonic power synchronously according to the expression of polynomial fitting.