原子与分子物理学报
原子與分子物理學報
원자여분자물이학보
CHINESE JOURNAL OF ATOMIC AND MOLECULAR PHYSICS
2015年
2期
275-280
,共6页
李鹏茂%萨楚尔夫%苏少龙
李鵬茂%薩楚爾伕%囌少龍
리붕무%살초이부%소소룡
薛定谔猫态%非旋波近似%布局数反转%反聚束效应
薛定諤貓態%非鏇波近似%佈跼數反轉%反聚束效應
설정악묘태%비선파근사%포국수반전%반취속효응
Schr?dinger cat state%Without RWA%Atomic population%The antibunching effect
在非旋波近似下,通过采用相干态正交化展开的方法,研究了薛定谔猫态光场与二能级原子相互作用系统中,原子的布局数和光场的反聚束效应,并与旋波近似下的结果进行了对比。在旋波近似与非旋波近似下,讨论了初始光场强度、相干态间的相位角以及失谐量对原子布局数和光场反聚束效应的影响;在非旋波近似下,讨论了强弱耦合情况下光场的反聚束效应。研究结果表明:旋波近似与非旋波近似下,原子的布局数随着初始光场强度的不同,表现出不同的特性;当初始光场强度较小时,旋波近似与非旋波近似下,原子的布局数表现出相同的特性;随着初始光场强度的增大,旋波近似下,原子的布局数将表现出坍塌现象。耦合强度较大时,光场的聚束与反聚束效应在非旋波近似与旋波近似下有较大的区别;非旋波近似下,随着初始光场强度的增大,光场一直处于聚束效应状态;而旋波近似下,光场的聚束效应与反聚束效应交替出现。
在非鏇波近似下,通過採用相榦態正交化展開的方法,研究瞭薛定諤貓態光場與二能級原子相互作用繫統中,原子的佈跼數和光場的反聚束效應,併與鏇波近似下的結果進行瞭對比。在鏇波近似與非鏇波近似下,討論瞭初始光場彊度、相榦態間的相位角以及失諧量對原子佈跼數和光場反聚束效應的影響;在非鏇波近似下,討論瞭彊弱耦閤情況下光場的反聚束效應。研究結果錶明:鏇波近似與非鏇波近似下,原子的佈跼數隨著初始光場彊度的不同,錶現齣不同的特性;噹初始光場彊度較小時,鏇波近似與非鏇波近似下,原子的佈跼數錶現齣相同的特性;隨著初始光場彊度的增大,鏇波近似下,原子的佈跼數將錶現齣坍塌現象。耦閤彊度較大時,光場的聚束與反聚束效應在非鏇波近似與鏇波近似下有較大的區彆;非鏇波近似下,隨著初始光場彊度的增大,光場一直處于聚束效應狀態;而鏇波近似下,光場的聚束效應與反聚束效應交替齣現。
재비선파근사하,통과채용상간태정교화전개적방법,연구료설정악묘태광장여이능급원자상호작용계통중,원자적포국수화광장적반취속효응,병여선파근사하적결과진행료대비。재선파근사여비선파근사하,토론료초시광장강도、상간태간적상위각이급실해량대원자포국수화광장반취속효응적영향;재비선파근사하,토론료강약우합정황하광장적반취속효응。연구결과표명:선파근사여비선파근사하,원자적포국수수착초시광장강도적불동,표현출불동적특성;당초시광장강도교소시,선파근사여비선파근사하,원자적포국수표현출상동적특성;수착초시광장강도적증대,선파근사하,원자적포국수장표현출담탑현상。우합강도교대시,광장적취속여반취속효응재비선파근사여선파근사하유교대적구별;비선파근사하,수착초시광장강도적증대,광장일직처우취속효응상태;이선파근사하,광장적취속효응여반취속효응교체출현。
Applying the method of coherent states orthogonalization expansion , the atomic population and the anti-bunching effect of the light field are studied in the system of interaction between a two -level atom and the Schr?dinger cat state without rotating wave approximation ( RWA) .The results are compared with those in RWA . The influences of the original strength of the light field and two coherent phase angles on the atomic population and antibunching effect with RWA and without RWA are discussed respectively , and the antibunching effect in the weak coupling condition is also discussed without RWA .The results show that the atomic populations with RWA and without RWA have different properties with the different original strengths of the light field .As the original strength of the light field is smaller , the atomic populations with RWA and without RWA show the same properties , but with the increase of the original strength of the light field the population with RWA will show the collapse phe -nomenon .When the coupling strength is larger , the antibunching effects with RWA and without RWA have bigger difference .Without RWA the light field will appear bunching effect , whereas with RWA it will appear alternately the bunching effect and the antibunching effect with the increase of the original strength of light field .