强激光与粒子束
彊激光與粒子束
강격광여입자속
HIGH POWER LASER AND PARTICLEBEAMS
2010年
1期
176-180
,共5页
李超龙%石海泉%艾剑峰%陈爱喜%黄克林%刘志荣%刘正方%刘志敏%李金海
李超龍%石海泉%艾劍峰%陳愛喜%黃剋林%劉誌榮%劉正方%劉誌敏%李金海
리초룡%석해천%애검봉%진애희%황극림%류지영%류정방%류지민%리금해
强流束%螺旋管透镜%束流光学%非线性传输%迭代计算
彊流束%螺鏇管透鏡%束流光學%非線性傳輸%迭代計算
강류속%라선관투경%속류광학%비선성전수%질대계산
intense beams%solenoid lenses%beam optics%nonlinear transport%iterative calculation
为计算强流脉冲束在螺旋管透镜6维相空间中的非线性传输,用Visual Fortran 6.5语言设计了一个计算程序,计算由漂浮空间、螺旋管透镜等元件组成的束流光学系统.程序在计算非强流脉冲束流的线性传输时,粒子的轨迹通过矩阵的直接相乘计算得出;程序在计算强流脉冲束流的非线性传输时,需要考虑束流中的空间电荷效应对束流传输的影响,在束流运动过程中,空间电荷场也在不断地变化,而且粒子运动的轨迹与空间电荷势又是相互依赖的,因此需要求得一个自洽的解,先把元件分成若干均等的区间,把电流分成若干等份,后采用束流电流迭代与元件区间迭代的计算方法.程序运行结束时,横向和纵向相图以及束流光学系统的束流包络线可以在微机屏幕上直观地显示出来.
為計算彊流脈遲束在螺鏇管透鏡6維相空間中的非線性傳輸,用Visual Fortran 6.5語言設計瞭一箇計算程序,計算由漂浮空間、螺鏇管透鏡等元件組成的束流光學繫統.程序在計算非彊流脈遲束流的線性傳輸時,粒子的軌跡通過矩陣的直接相乘計算得齣;程序在計算彊流脈遲束流的非線性傳輸時,需要攷慮束流中的空間電荷效應對束流傳輸的影響,在束流運動過程中,空間電荷場也在不斷地變化,而且粒子運動的軌跡與空間電荷勢又是相互依賴的,因此需要求得一箇自洽的解,先把元件分成若榦均等的區間,把電流分成若榦等份,後採用束流電流迭代與元件區間迭代的計算方法.程序運行結束時,橫嚮和縱嚮相圖以及束流光學繫統的束流包絡線可以在微機屏幕上直觀地顯示齣來.
위계산강류맥충속재라선관투경6유상공간중적비선성전수,용Visual Fortran 6.5어언설계료일개계산정서,계산유표부공간、라선관투경등원건조성적속류광학계통.정서재계산비강류맥충속류적선성전수시,입자적궤적통과구진적직접상승계산득출;정서재계산강류맥충속류적비선성전수시,수요고필속류중적공간전하효응대속류전수적영향,재속류운동과정중,공간전하장야재불단지변화,이차입자운동적궤적여공간전하세우시상호의뢰적,인차수요구득일개자흡적해,선파원건분성약간균등적구간,파전류분성약간등빈,후채용속류전류질대여원건구간질대적계산방법.정서운행결속시,횡향화종향상도이급속류광학계통적속류포락선가이재미궤병막상직관지현시출래.
To calculate nonlinear transport of pulsed beams in the six-dimensional phase space of solenoid lens accurately, a beam dynamics program has been designed using Visual Fortran 6.5 to calculate the beam optical system consisting of drift spaces and solenoid lenses. For non-intense beams, particle trajectory can be obtained by multiplying linear transport matrices. For nonlinear transport of intense beams, the influence of space-charge effect on beam transport needs to be taken into account, and self-consistent solution should be derived because of the interaction between charged particle distribution and space charge field. In the program, components and currents are divided into equal intervals, respectively, and each interval is treated as a uniform solenoid field. Then beam current iteration and component interval iteration are conducted to get self-consistent solutions. When program running is finished, horizontal and vertical phase diagrams of the system, as well as beam envelopes can be visually displayed on the computer screen.