中国光学
中國光學
중국광학
CHINESE JOURNAL OF OPTICS
2011年
1期
53-59
,共7页
李仁先%韩香娥%帕尔哈提江·吐尔孙
李仁先%韓香娥%帕爾哈提江·吐爾孫
리인선%한향아%파이합제강·토이손
辐射扭矩%德拜级数%高斯光束%光钳%角矩
輻射扭矩%德拜級數%高斯光束%光鉗%角矩
복사뉴구%덕배급수%고사광속%광겸%각구
radiation torque%Debye series%Gaussian beam%optical tweezer%angular momentum
基于会聚光束所产生的扭矩来实现对小粒子的操纵已在物理学、生物学等领域得到了广泛的应用,为了分离出单个散射过程对扭矩的贡献,给出扭矩物理机理的解释,本文引入德拜级数分析了高斯波束对均匀球粒子所产生的扭矩.计算表明,当德拜项p从1取到一个足够大的值后,德拜级数计算结果与广义米氏理论结果吻合.文中重点分析了单阶p散射过程对横向扭矩的贡献,结果表明:当线极化光束入射时,p=1-5散射过程都可以产生横向扭矩,但扭矩的方向不同;当圆极化光束入射时,p=-1和0对应的扭矩远大于P=1-4对应的扭矩,且P=0过程产生与其他p过程相反方向的扭矩.
基于會聚光束所產生的扭矩來實現對小粒子的操縱已在物理學、生物學等領域得到瞭廣汎的應用,為瞭分離齣單箇散射過程對扭矩的貢獻,給齣扭矩物理機理的解釋,本文引入德拜級數分析瞭高斯波束對均勻毬粒子所產生的扭矩.計算錶明,噹德拜項p從1取到一箇足夠大的值後,德拜級數計算結果與廣義米氏理論結果吻閤.文中重點分析瞭單階p散射過程對橫嚮扭矩的貢獻,結果錶明:噹線極化光束入射時,p=1-5散射過程都可以產生橫嚮扭矩,但扭矩的方嚮不同;噹圓極化光束入射時,p=-1和0對應的扭矩遠大于P=1-4對應的扭矩,且P=0過程產生與其他p過程相反方嚮的扭矩.
기우회취광속소산생적뉴구래실현대소입자적조종이재물이학、생물학등영역득도료엄범적응용,위료분리출단개산사과정대뉴구적공헌,급출뉴구물리궤리적해석,본문인입덕배급수분석료고사파속대균균구입자소산생적뉴구.계산표명,당덕배항p종1취도일개족구대적치후,덕배급수계산결과여엄의미씨이론결과문합.문중중점분석료단계p산사과정대횡향뉴구적공헌,결과표명:당선겁화광속입사시,p=1-5산사과정도가이산생횡향뉴구,단뉴구적방향불동;당원겁화광속입사시,p=-1화0대응적뉴구원대우P=1-4대응적뉴구,차P=0과정산생여기타p과정상반방향적뉴구.
The radiation torque induced by a focused laser beam has been widely utilized for the optical manipulation of small particles in various fields such as physics, biology, and optofluidics. To isolate the contribution of each scattering process to the radiation torque and to clarify the physical mechanism of radiation torque, the Debye Series Expand(DSE) is introduced to analysis of the radiation torque exerted on a homogeneous sphere by Gaussian beam. When Debye mode p ranges from 1 to a value Pmax large enough, the result obtained by DSE is identical to that by Generalized Lorenz-Mie Theory (GLMT).Furthermore, the radiation torque corresponding to each Debye mode p is mainly analyzed. Results show that when incident beam is linearly polarized, all scattering processes for p in 1-5 can produce a transverse torque while the directions of torque are different. When the beam is circularly polarized, the torques for p in 1 and 0 are much larger than that for p in 1-4,and the direction of torque for p in 0 is opposite with that for other mode p.