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Internal Structure of LCD LCD stands for Liquid Crystal Display. LCD is finding wide spread use replacing LEDs (seven segment LEDs or other multi segment LEDs) because of the following reasons:

Internal Structure of LCD LCD stands for Liquid Crystal Display. LCD is finding wide spread use replacing LEDs (seven segment LEDs or other multi segment LEDs) because of the following reasons:

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Basic peculiarities of the laser-induced optical breakdown of matter are discussed. Main experimental data for various materials and regimes of laser irradiation are represented and analyzed. Role of Nonlinear and Relaxed Optical processes are observed. Three types of optical breakdown are selected^ thermal, plasma and direct. It was shown that the...

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... used for harvesting solar energy directly for electricity production. Photovoltaic cells are made of a semi conductive material that is specially treated wafer of silicon, sandwiched between two thin contact plates where the top contact plate is positively charged and the back contact plate is negatively charged making it a semiconductor device (Fig. 3). The n-type semiconductor is negatively charged due to the abundance of electrons, while the p-type semiconductor is positively charged. Electron movement at p-n junction produces an electric field that allows flow of electrons from the p-type layer to the n-type semiconductor layer. As soon as the Sun rays of suitable wavelength hits ...
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... pulse duration of laser irradiation is re[presented in Fig. 2b) [3] . For stable dimensions of irradiation region and pulse duration a breakdown is realized with some probability and probability of breakdown is increased for increasing of power density of irradiation. Analogous results were received for the increasing the surface of irradiation (Fig. 3 a)) [3] . [3] , b) Dependence of threshold power P of destruction the Ruby crystals from pulse duration of laser irradiation [3] A dependence of probability the optical breakdown from quantity q/q(r 0 ), where q(r 0 )-a power density, for which in the irradiation region with radius r 0 probability of breakdown is near to one [3] . Fig 3: ...
Context 3
... , b) Dependence of threshold power P of destruction the Ruby crystals from pulse duration of laser irradiation [3] A dependence of probability the optical breakdown from quantity q/q(r 0 ), where q(r 0 )-a power density, for which in the irradiation region with radius r 0 probability of breakdown is near to one [3] . Fig 3: a) Dimensional dependence of threshold the surface destruction (optical breakdown) of glass K-8 [3] ; b) Dependence of probability the optical breakdown from quantity q/q(r0), where q(r0)-a power density, for which in the irradiation region with radius r0 probability of breakdown is near to one [3] The time-resolved refractive index and absorption mapping of lightplasma filaments in water were observed in [19] . ...
Context 4
... used for harvesting solar energy directly for electricity production. Photovoltaic cells are made of a semi conductive material that is specially treated wafer of silicon, sandwiched between two thin contact plates where the top contact plate is positively charged and the back contact plate is negatively charged making it a semiconductor device (Fig. 3). The n-type semiconductor is negatively charged due to the abundance of electrons, while the p-type semiconductor is positively charged. Electron movement at p-n junction produces an electric field that allows flow of electrons from the p-type layer to the n-type semiconductor layer. As soon as the Sun rays of suitable wavelength hits ...
Context 5
... pulse duration of laser irradiation is re[presented in Fig. 2b) [3] . For stable dimensions of irradiation region and pulse duration a breakdown is realized with some probability and probability of breakdown is increased for increasing of power density of irradiation. Analogous results were received for the increasing the surface of irradiation (Fig. 3 a)) [3] . [3] , b) Dependence of threshold power P of destruction the Ruby crystals from pulse duration of laser irradiation [3] A dependence of probability the optical breakdown from quantity q/q(r 0 ), where q(r 0 )-a power density, for which in the irradiation region with radius r 0 probability of breakdown is near to one [3] . Fig 3: ...
Context 6
... , b) Dependence of threshold power P of destruction the Ruby crystals from pulse duration of laser irradiation [3] A dependence of probability the optical breakdown from quantity q/q(r 0 ), where q(r 0 )-a power density, for which in the irradiation region with radius r 0 probability of breakdown is near to one [3] . Fig 3: a) Dimensional dependence of threshold the surface destruction (optical breakdown) of glass K-8 [3] ; b) Dependence of probability the optical breakdown from quantity q/q(r0), where q(r0)-a power density, for which in the irradiation region with radius r0 probability of breakdown is near to one [3] The time-resolved refractive index and absorption mapping of lightplasma filaments in water were observed in [19] . ...

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