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Fresnel coefficient for reflection

This problem was treated in section 1.6 of Chapter 1, where the Fresnel coefficients for reflected and refracted light were calculated and presented in equations (1.74) to (1.77). The problem being treated is pictured in Figure 1.4, and it is convenient to represent the electric vector as a Jones vector having orthogonal components that are either parallel... [Pg.45]

If a mirror is to be an effective optical element then the reflectivity must be as close to 100% as possible. Parratt (1954) gives an expression, derived from the Fresnel coefficient for reflection (Compton and Allison 1935), for the reflectivity, R, for an incidence angle, 6, and critical angle, 0C, for a perfectly smooth homogeneous mirror surface... [Pg.165]

The refractive index depends on the propagation of light as well as the reflected and transmitted fractions of incident waves on an interface. The Fresnel coefficients for reflection and transmission are given by the refractive indices of the two adjacent materials. For many applications of porous silicon in optics or optoelectronics, it is necessary to know the exact refractive index (see, e.g., chapters Porous Silicon Photonic Crystals, Porous Silicon Optical Waveguides, Porous... [Pg.796]

Here r is the Fresnel coefficient for reflection, fraction of the amplitude that is refleaed back to medium ),... [Pg.435]

Ellipsometry. Determination of h(u>) by KK analysis and coupled measurements of 1Z and T are affected, respectively, by the problem of the tails added to the experimental R(u>) spectra and by the need to perform 7Z and T measurements separately These problems, which introduce some uncertainty, can be solved by spectroscopic ellipsometry. The technique involves analyzing the polarization of a light beam reflected by a surface. The incident beam must be linearly polarized and its polarization should be allowed to rotate. A second linear polarizer then analyzes the reflected beam. The roles of polarizer and analyzer can be exchanged. The amplitudes of the s and p components of the reflected radiation are affected in a different way by reflection at the surface. The important function describing the process is the ellipsometric ratio p, which is defined as the polarization of the reflected wave with respect to the incident wave, expressed as the ratio between the Fresnel coefficients for p and s polarizations ... [Pg.64]

For perpendicular polarized radiation, the reflection (Fresnel) coefficients are given by the expressions ... [Pg.250]

A simple and practical way to achieve the field enhancement is to use backside illumination of a dielectric plate, for instance a cover glass, in a standard DLW geometry with an oil-immersion focusing lens. According to the Fresnel formulas for the right angle incidence (0, = 0°), the coefficients of the in-plane ( ) polarized amphtudes of transmitted and reflected electric fields are, respectively ... [Pg.176]

Ie is the true scattered intensity I e is the measured scattered intensity at angle 6, and Z i8o-e is at the supplementary angle. fa and fi are the Fresnel s coefficients for the fractions of light reflected at perpendicular incidence at the glass-air and glass-liquid interfaces, respectively ta and tx are the corresponding transmission coefficients. They are defined by the following equations ... [Pg.101]

For n layers, the matrices for each layer are multiplied together, [C] = [Ci][C2]. .. [C + i], to give the resultant reflectivity from the elements of the final 2x2 matrix such that, R = cc jaa. In practice, recurrence relationships between the Fresnel coefficients in the successive layers can be used to provide an efficient calculation. Furthermore, following the approach of Nevot and Croce [20], a Gaussian roughness or diffuse profile can be included at each interface in the stack, such that... [Pg.92]

In addition to the tensor element dependence of the sum-frequency intensity, there is also a dependence on the geometry of the experiment that manifests itself in the linear and non-linear Fresnel factors that describe the behaviour of the three light beams at the interface. Fresnel factors are the reflection and transmission coefficients for electromagnetic radiation at a boundary and depend on the frequency, polarization and incident angle of the electromagnetic waves and the indices of refraction for the media at the boundary [16,21]. [Pg.32]

For the case of non-normal illumination incidence at some angle 0, the Fresnel transmission and reflection coefficients are now functions of the angle of incidence as well as the polarization of the incident light they are given hy ... [Pg.568]

Fresnel equations relate the electric field strength amphtudes of the incident, reflected, and transmitted waves. They are solutions of Maxwells equations by applying the above-mentioned boundary conditions. It can be shown that for a plane boundary between two non-magnetic isotropic phases of infinite thickness, schematically depicted in Fig. 9.1, the Fresnel reflection (r) and transmission (t) coefficients for s- and p-polarized light are given by the following equations ... [Pg.319]

The Fresnel equations for the reflectance coefficients roi and for the ambient-film and the film-substrate interface are given by... [Pg.86]

This equation is the so-called basic ellipsometric equation. It contains R and R which depend on the optical properties of the reflecting system, the wavelength of the light X the angle of incidence cp and the experimentally measurable parameters Pand A. For the reflection at a clean interface, the Rp and R are the Fresnel coefficients (246) of the single uncovered interface. They depend only on the refractive indices of the two adjacent phases and the angle of incidence. For systems that do not absorb light the optical constants of the two bulk phases (ambient and substrate media) are usually obtained from the experimental values of P and A for the clean interface (denoted by subscript 0 via Eq. (111). For a layer-covered interface, multiple reflections and refractions take place within the layer (Fig. 24). [Pg.33]

After reflection at the interface, the reflected wave is in general elliptically polarized. The shape and orientation of the ellipse depend on the incident polarization, incident angle and reflection properties of the interface, and can be described with the ratio p of the complex Fresnel s reflection coefficients for the p and s polarizations ... [Pg.204]

The samples were freestanding films with thickness 40-100 p,m. This thickness is greater than the electromagnetic penetration depth [5 = c/ 2tt xwo-(w), where c is the speed of light and 10 S/cm. Samples with or cTdc < 10 S/cm were first checked to determine whether they had transmitted far-IR radiation. Therefore, the reflectance can be analyzed using the Fresnel reflection coefficients for semi-infinite media [103]. [Pg.618]

For nonabsorbing materials, the boundary conditions (1.4.7°) lead to the Fresnel formulas for the amplitude of reflection and transmission coefficients (1.4.5°) ... [Pg.26]

If an isotropic layer with a thickness d.2 is located at the planar interface of two semi-infinite media (Fig. 1.12), the incident wave gives rise to reflected and refracted waves in all the media except for the ontput halfspace, where only the refracted wave exists. For such an optical configuration, the Fresnel coefficients (1.4.5°) can be rewritten in the Drude (exact) form [9] as... [Pg.32]


See other pages where Fresnel coefficient for reflection is mentioned: [Pg.243]    [Pg.216]    [Pg.247]    [Pg.68]    [Pg.243]    [Pg.216]    [Pg.247]    [Pg.68]    [Pg.250]    [Pg.71]    [Pg.306]    [Pg.250]    [Pg.46]    [Pg.215]    [Pg.301]    [Pg.40]    [Pg.292]    [Pg.235]    [Pg.66]    [Pg.94]    [Pg.47]    [Pg.287]    [Pg.227]    [Pg.306]    [Pg.451]    [Pg.499]    [Pg.258]    [Pg.202]    [Pg.2607]    [Pg.32]    [Pg.40]    [Pg.44]    [Pg.383]    [Pg.383]   


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