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在电介质-电介质界面处全内反射时伴随的相移。

Phase shifts that accompany total internal reflection at a dielectric-dielectric interface.

作者信息

Azzam R M A

机构信息

Department of Electrical Engineering, University of New Orleans, New Orleans, Louisiana 70148, USA.

出版信息

J Opt Soc Am A Opt Image Sci Vis. 2004 Aug;21(8):1559-63. doi: 10.1364/josaa.21.001559.

Abstract

The absolute, average, and differential phase shifts that p- and s-polarized light experience in total internal reflection (TIR) at the planar interface between two transparent media are considered as functions of the angle of incidence phi. Special angles at which quarter-wave phase shifts are achieved are determined as functions of the relative refractive index N. When the average phase shift equals pi/2, the differential reflection phase shift delta is maximum, and the reflection Jones matrix assumes a simple form. For N > square root 3, the average and differential phase shifts are equal (hence deltap = 3 deltas) at a certain angle phi that is determined as a function of N. All phase shifts rise with infinite slope at the critical angle. The limiting slope of the delta-versus-phi curve at grazing incidence (partial partial differential delta/partial partial differential phi)phi=90 degrees = -(2/N)(N2 - 1)1/2 = -2 cos phic, where phic is the critical angle and (partial partial differential2 delta/partial partial differential phi 2)phi=90 degrees = 0. Therefore delta is proportional to the grazing incidence angle theta = 90 degrees - phi (for small theta) with a slope that depends on N. The largest separation between the angle of maximum delta and the critical angle is 9.88 degrees and occurs when N = 1.55377. Finally, several techniques are presented for determining the relative refractive index N by using TIR ellipsometry.

摘要

p偏振光和s偏振光在两种透明介质的平面界面上发生全内反射(TIR)时所经历的绝对相移、平均相移和微分相移被视为入射角φ的函数。实现四分之一波相移的特殊角度被确定为相对折射率N的函数。当平均相移等于π/2时,微分反射相移δ最大,并且反射琼斯矩阵具有简单形式。对于N>√3,在某个由N确定的角度φ处,平均相移和微分相移相等(因此δp = 3δs)。所有相移在临界角处都以无限斜率上升。掠入射角(∂δ/∂φ)φ = 90°时δ-φ曲线的极限斜率为-(2/N)(N² - 1)½ = -2cosφc,其中φc是临界角,且(∂²δ/∂φ²)φ = 90° = 0。因此,对于小θ,δ与掠入射角θ = 90° - φ成正比,其斜率取决于N。最大δ角与临界角之间的最大间距为9.88°,且在N = 1.55377时出现。最后,介绍了几种使用TIR椭圆偏振法确定相对折射率N的技术。

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