2011
DOI: 10.1081/e-eoe
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Encyclopedia of Optical Engineering

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Cited by 16 publications
(4 citation statements)
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“…435 where w 0 is the original waist of the beam, x is the distance along the optical path, λ is the wavelength of light, and n is the index of refraction [41]. Calculation considers G = 100, R = 100 Ω, κ = 0.119 A/W, P = 133 mW, d = 6 mm, t = 0.25 440 mm, w 0 = 0.5 mm, λ= 6.8 mm, δ= 1 nm.…”
Section: Resultsmentioning
confidence: 99%
“…435 where w 0 is the original waist of the beam, x is the distance along the optical path, λ is the wavelength of light, and n is the index of refraction [41]. Calculation considers G = 100, R = 100 Ω, κ = 0.119 A/W, P = 133 mW, d = 6 mm, t = 0.25 440 mm, w 0 = 0.5 mm, λ= 6.8 mm, δ= 1 nm.…”
Section: Resultsmentioning
confidence: 99%
“…A major advantage in using these LCs is that, despite their high rotational viscosity, they exhibit a fast response time to an applied electric field. The threshold voltage, V th at which the LC starts to respond to the external applied voltage is directly related to the dielectric anisotropy and can be described as (Spring, 2011):…”
Section: B Electric Tunabilitymentioning
confidence: 99%
“…Therefore, as the dielectric anisotropy, ∆ε increases, the LC responds to lower applied voltages. It should be emphasized that other factors such as the rise and decay times, elastic constants, Frederick's transition of the LCs also play a role in the final performance of the LC-based devices (Onuki, 2004;Spring, 2011).…”
Section: B Electric Tunabilitymentioning
confidence: 99%
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