By Hermann Wollnik
Educational Press, 1987. Paperback. e-book situation no longer Used
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Extra info for Optics of Charged Particles
Determine the minimal thickness d of the plate for which the ordinary and extraordinary light beams output from the plate would not overlap. 8 If in the previous problem the beams of the ordinary and extraordinary waves overlap, what is the state of polarization of light oscillations in the domain where the beams superimpose? 9 Determine the intensity I2 of a light beam passed through two linear polarizers whose axes of transmission form angle α = 60 deg. org/terms 24 Chapter 3 is linearly polarized, and the direction of oscillations (polarization azimuth) of the incident light forms the angle θ = 30 deg with the transmission axis of the first linear polarizer.
Determine frequency fS of the periodical variation of the light intensity I(t) in the interference pattern at the output of the interferometer if the wavelength of the light is λ0 = 633 nm. 5 µm and frequency f = 102 Hz. 5 mW/mm2 . The initial phase difference between the waves is ∆φ0 = 0, π/2, or π rad. For plotting, take the time interval [0, t] equal to two periods of the mirror oscillation. 35 A mirror in a Michelson interferometer harmonically oscillates with frequency f0 and amplitude l0 along the optical axis, ∆z = l0 sin(2π f0 t + φ0 ).
The major semiaxis of the ellipse is parallel to the incidence plane, and the ratio of the semiaxes of the polarization ellipse is equal to the ratio of the amplitude reflection coefficients for the waves polarized parallel and perpendicular to the incidence plane. 3; the major semiaxis is perpendicular to the incident plane. 9 R p = (ρ p )2 , T p = (τ p )2 nn21 cos cos α0 ; R = (ρ ) , T = (τ ) n1 cos α0 ; p p ρ and τ are amplitude reflection and transmission coefficients, α2 is refraction angle.
Optics of Charged Particles by Hermann Wollnik