Equations
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1
Common DOE surfaces
1.1
Sinusoidal, triangle
1.2
Square, rectangle
1.3
Blazed, sawtooth
2
Holographic Deflectors (hologons)
Common DOE surfaces
Sinusoidal, triangle
Max D.E. ~ 30% ± 1 order
Power distribution follows Bessel function in the scaler region.
T ≈ λ for transmission.
T ≈ λ/4 for reflection.
Easily replicated or deep etch can yield higher efficiency.
Square, rectangle
Max D.E. ~ 40% ± 1 order.
Power distributions favors odd orders.
Pi phase shift typical.
Classic binary grating.
T ≈ λ for transmission.
T ≈ λ/4 for reflection.
Blazed, sawtooth
Max D.E ~ 98%
Reflection Case:
λ = 2 d sin a
T = λ/2 ± 10%
Transmission Case:
λ = d sin b
a ≈ 2b
T = λ/(n-1) ± 10%
Surface shadows reduce D.E. by
λ
2
n
d
2
{\displaystyle \textstyle {\frac {\lambda ^{2}}{nd^{2}}}}
Wavelength changes reduce D.E. by
(
π
Δ
λ
b
λ
)
2
{\displaystyle \textstyle \left({\frac {\pi \Delta \lambda }{b\lambda }}\right)^{2}}
Holographic Deflectors (hologons)
N = θD/(1.4λ)
N = number of resolvable spots
θ = full scan angle in radians
D = beam diameter in microns
λ = wavelength
Φ = wedge angle of glass
Special case of linear scan and near wobble invariance a ~ b ~ 45° max straight scan angle ~ 36°
Dynamic wobble
≃
Δ
Ω
/
128
{\displaystyle \scriptstyle \simeq \Delta \Omega /128}
Wedge wobble = (n-1)Φ
Scan angle multiplier = 1.4 @ 90° cross scan angle
Last modified on 9/29/97
Category
:
Rallison
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