Use of a laser beam is an obvious choice in many metrological applications. When the laser is oscillating in TEM00 mode, the beam has a Gaussian profile, and its spatial extent is very small. It is important to understand its propagation and manipulation by the lens or any other image-forming component. Since light is characterized by wave motion as well, we begin with the three-dimensional wave equation and search for a solution, which would resemble a laser beam. The wave equation is given by
|
(2.1) |
where:
u is the wave amplitude
∇2 = (∂2/∂x2) + (∂2/∂y2) + (∂2/∂z2) is the Laplacian
We will consider a monochromatic wave traveling along the +z-direction and express the solution as ...
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