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2c). 30) which describes a left circularly polarized (usually abbreviated as LCP) wave. At any particular value of x, the tip of the E-vector, with increasing time t, can easily be shown to rotate on the circumference of a circle like a left-handed screw. 31) thus the tip of the electric vector rotates on a circle in the anti-clockwise direction (see Fig. 3) and therefore it is said to represent an LCP beam. When propagating in air or in any isotropic medium, the state of polarization (SOP) is maintained, 16 2 Basic Optics Fig.
51) one can readily show that +∞ +∞ I(x, y, z) dxdy = −∞ −∞ π w20 I0 2 which is independent of z. This is to be expected, as the total energy crossing the entire x–y plane will not change with z. 59) On the plane z= R (see Fig. 60) x2 + y2 2R where we have assumed |x| , |y| << R. 62) 22 2 Basic Optics Fig. 5 Diffraction divergence of a Gaussian beam whose phase front is plane at z= 0. The dashed curves represent the phase fronts (on the x–y plane) represents a diverging spherical wave of radius R.
It is not possible to derive it from anything you know. It came out of the mind of Schrödinger. Although we have obtained Eq. 16) starting from an expression for a plane wave, the Schrödinger equation as described by Eq. 16) is more general in the sense that ψ (r, t) called the wave function contains all information that is knowable about the system. 4, ψ ∗ (r, t)ψ(r, t)dτ represents the probability of finding the particle in a volume element dτ . Note also that observables such as momentum energy are represented by operators [see Eq.