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Lasers

A laser is a monochromatic coherent beam of light.

Glossary​

  • Monochromatic: a single wavelength
  • Coherent: All the light waves move precisely together in the same phase, which gives the beam intense power.
  • Beam Waist: The narrowest point of a laser beam. This isn't necessarily the emitter, the beam might be focused on a far away point.

Damage Types​

  • Dazzling: Temporarily blinding sensors
  • Blinding: Permanently damaging optical sensors
  • Heating: Damaging surface electronics (e.g. radar panel) and mechanics (e.g. gun mounts).
  • Fracturing: Thermal stresses can cause cracks, or delamination of layers
  • Weakening: Hot structural elements are not as strong and may buckle under load
  • Melting: Melting away surface material
  • Vaporising: Evaporating surface material
  • Plasma Erosion: Plasma plume can physically erode material around it as it exits the hole

Physics​

Irradiance​

Measure of radiant power incident on a surface per unit area:

I=PAI = \frac{P}{A}

  • I: W/m2W/m^2
  • P: W, power
  • A: m^2, spot size

Gaussian Beam Spot Size​

The size of the laser beam, usually calculated at a given distance. The equation normally depends on the refractive index of the medium, in vacuum that's exactly 1 which slightly simplifies the equation.

w(z)=w0⋅1+(zλπw02)2w(z) = w_0\cdot\sqrt{1+\left(\frac{z\lambda}{\pi w_0^2}\right)^2}

Rayleigh Range is the distance to where the area of the spot size has doubled (i.e. irradiance has halved).

zR=πwo2λz_R = \frac{\pi w_o^2}{\lambda}

Beam divergence is a simplification of the gaussian spot size which assumes the laser is a cone with a constant divergence angle. This provides a simpler equation for spot size.

w(z)=w0+zθw(z) = w_0 + z\theta

  • w(z)w(z): mm, spot size radius (w) at range (z)
  • w0w_0: mm, beam waist radius
  • zz: mm, range (from beam waist to target, not emitter to target)
  • λ\lambda: mm, wavelength
  • θ\theta: radians, beam divergence angle

Diffraction Limit​

This sets the physical lower limit on beam divergence.

θ=1.27λDaperture\theta = 1.27\frac{\lambda}{D_{aperture}}

  • θ\theta: radians, beam divergence angle
  • λ\lambda: mm, wavelength
  • D_{aperture}: m, aperture diameter

Beam Quality Factor​

Diffraction limited is the best you can do, but beam quality measures how much worse it is in reality. This is a factor of the quality of your optics etc. This is measured as M2M^2, for a perfect system M2=1M^2 = 1.

θactual=M2⋅θdiffraction\theta_{actual} = M^2 \cdot \theta_{diffraction}

Minimum Spot Size​

The smallest spot size a laser can be focused to. Airy disc formula.

Rspot=1.22⋅λ⋅LDaperture⋅M2R_{spot} = \frac{1.22 \cdot \lambda \cdot L}{D_{aperture}} \cdot M^2

  • RspotR_{spot} is the spot diameter
  • λ\lambda is the wavelength of the laser
  • LL is the distance to the target
  • DapertureD_{aperture} is the diameter of the aperture
  • M2M^2 is the beam quality factor

Jittered Spot Size​

Assuming the emitter is vibrating, we can account for that by rolling it into spot size.

Reffective=Rspot2+(L⋅tan(θjitter))2R_{effective} = \sqrt{R_{spot}^2 + (L \cdot tan(\theta_{jitter}))^2}

  • θjitter\theta_{jitter} RMS of jitter angle

Note that the small angle approximation says tan(θ)≈θtan(\theta) \approx \theta, for laser pointing errors the jitter angle is always going to be tiny, so the tan function can be ignored.

References​