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Volumn 76, Issue 6, 2007, Pages

Axial optical trapping efficiency through a dielectric interface

Author keywords

[No Author keywords available]

Indexed keywords

ELECTRON TRAPS; LIGHT EMISSION; MICROSPHERES; OPTICAL TWEEZERS;

EID: 37749044476     PISSN: 15393755     EISSN: 15502376     Source Type: Journal    
DOI: 10.1103/PhysRevE.76.061917     Document Type: Article
Times cited : (38)

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    • Here, following a change of integration variable x=cos α1, fn TM,TE (x) represents the amplitude that does not depend on either beam position zo or displacement from cover slip d. The phase function, g (x), is (1- zo d) (n2 n1) 2 - (1- x2) -x, and γ= k1 d. Note that some restrictions apply, so as to have a real critical point. We need 1> (1- zo d) >0 and 1> (n2 n1) >0; this consequently restricts the interval of the beam displacement variable (zo) to the region of the observed oscillations.
    • Here, following a change of integration variable x=cos α1, fn TM,TE (x) represents the amplitude that does not depend on either beam position zo or displacement from cover slip d. The phase function, g (x), is (1- zo d) (n2 n1) 2 - (1- x2) -x, and γ= k1 d. Note that some restrictions apply, so as to have a real critical point. We need 1> (1- zo d) >0 and 1> (n2 n1) >0; this consequently restricts the interval of the beam displacement variable (zo) to the region of the observed oscillations.


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