中国传媒大学学报(自然科学版)
中國傳媒大學學報(自然科學版)
중국전매대학학보(자연과학판)
JOURNAL OF COMMUNICATION UNIVERSITY OF CHINA(SCIENCE AND TECHNOLOGY)
2014年
1期
1-15
,共15页
表面波%大GH位移%负GH位移%Kretschmann结构%纳米金属薄膜
錶麵波%大GH位移%負GH位移%Kretschmann結構%納米金屬薄膜
표면파%대GH위이%부GH위이%Kretschmann결구%납미금속박막
surface waves%giant GHS%negative GHS%Kretschmann’ s structure%nano metal-films
1947年Goos和H?nchen发现,当电磁波束在玻璃/空气界面全反射时,在返回玻璃内部时有一项发生在入射面内的纵向位移;我们称之为正位移。实际上,稳态相位法的计算表明,位移可以为正、为零,甚至为负。由于界面上的表面波可以是前向型的和后向型的,携带的功率向着不同方向;故当激发起后向型表面波时就可获得入射波束的负位移。在多层结构中,当入射波束波矢的切向分量与表面波传播常数一致时,会发生类谐振现象并导致位移增大。<br> 在一般情况下,当光束入射到金属表面,TM极化时GHS为负,并且绝对值比TE极化时大得多。但我们在微波的实验研究表明,在使用金属时可以在TE极化时发生负位移。实验时在全反射界面处为纳米级金属膜,是厚度30nm和60nm的铝膜,它蒸镀在厚18μm聚乙烯膜上。实验还发现,当改变入射角θ1并使之达到约qθ1c(θ1c为全反射临界角,q>1)出现类谐振现象,GHS的绝对值可达(5~7)cm。目前尚缺少对这些结果的理论解释。
1947年Goos和H?nchen髮現,噹電磁波束在玻璃/空氣界麵全反射時,在返迴玻璃內部時有一項髮生在入射麵內的縱嚮位移;我們稱之為正位移。實際上,穩態相位法的計算錶明,位移可以為正、為零,甚至為負。由于界麵上的錶麵波可以是前嚮型的和後嚮型的,攜帶的功率嚮著不同方嚮;故噹激髮起後嚮型錶麵波時就可穫得入射波束的負位移。在多層結構中,噹入射波束波矢的切嚮分量與錶麵波傳播常數一緻時,會髮生類諧振現象併導緻位移增大。<br> 在一般情況下,噹光束入射到金屬錶麵,TM極化時GHS為負,併且絕對值比TE極化時大得多。但我們在微波的實驗研究錶明,在使用金屬時可以在TE極化時髮生負位移。實驗時在全反射界麵處為納米級金屬膜,是厚度30nm和60nm的鋁膜,它蒸鍍在厚18μm聚乙烯膜上。實驗還髮現,噹改變入射角θ1併使之達到約qθ1c(θ1c為全反射臨界角,q>1)齣現類諧振現象,GHS的絕對值可達(5~7)cm。目前尚缺少對這些結果的理論解釋。
1947년Goos화H?nchen발현,당전자파속재파리/공기계면전반사시,재반회파리내부시유일항발생재입사면내적종향위이;아문칭지위정위이。실제상,은태상위법적계산표명,위이가이위정、위령,심지위부。유우계면상적표면파가이시전향형적화후향형적,휴대적공솔향착불동방향;고당격발기후향형표면파시취가획득입사파속적부위이。재다층결구중,당입사파속파시적절향분량여표면파전파상수일치시,회발생류해진현상병도치위이증대。<br> 재일반정황하,당광속입사도금속표면,TM겁화시GHS위부,병차절대치비TE겁화시대득다。단아문재미파적실험연구표명,재사용금속시가이재TE겁화시발생부위이。실험시재전반사계면처위납미급금속막,시후도30nm화60nm적려막,타증도재후18μm취을희막상。실험환발현,당개변입사각θ1병사지체도약qθ1c(θ1c위전반사림계각,q>1)출현류해진현상,GHS적절대치가체(5~7)cm。목전상결소대저사결과적이론해석。
It has been shown by Goos and H?nchen in 1947 that electro-magnetic wave beam totally re-flected from a glass-air interface suffers a longitudinal displacement in the plane of incidence before re-entry into the glass,we say this situation to be positive GH shifts. In fact,the longitudinal displacement as computed by the application of the stationary phase method can be positive,zero or negative. The sur-face waves may be of the forward or the backward type and they carry power in opposite directions in the interface. And then,a negative shift of the incident beam is obtained when the backward surface waves are excited. In a layered structure,when the tangential component of the wave vector of incident beam co-incides with the propagation constant of the surface wave,the resonance-like phenomenon leading to a large enhancement of the beam shift. <br> In common cases when a light beam incident on a metal surface,the GHS for TM polarized light in metals is negative and much bigger than the positive shift for TE polarized light. But a experimental re-search of the GHS was performed by our team with microwaves,the result was that the shifts for TE polar-ized wave in metals is negative---dataes of the total reflection influenced by nano metal-films deposite on the total reflecting surface,and the Al-films were 30nm and 60nm thick and were vapor deposited on polyethylene films of 18μm thickness. When the incidence angleθ1 near the value of qθ1c (θ1c is the critical angle of total reflection,q>1),it show a resonance-like behavior,the GHS has a strong maximum of (5~7)cm absolute-ly. There is no exact theory for explain these effects,now.