嫌恶
发表于 2025-3-28 15:02:27
Rethinking Peace and Conflict Studiesrmal behaviour which can be used for chromatic or thermal aberration correction in hybrid elements. For broad band or white light applications, their strong chromatic dispersion is usually not wanted, but in many applications, using monochromatic laser light, it is of no importance.
Flustered
发表于 2025-3-28 21:20:05
Design and Fabrication Aspects of Continuous-Relief Diffractive Optical Elementsrmal behaviour which can be used for chromatic or thermal aberration correction in hybrid elements. For broad band or white light applications, their strong chromatic dispersion is usually not wanted, but in many applications, using monochromatic laser light, it is of no importance.
易于
发表于 2025-3-29 00:58:17
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财产
发表于 2025-3-29 06:20:15
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DAFT
发表于 2025-3-29 10:39:08
GRIN Planar Structures for Focusing, Collimation and Beam Size Controle index varies from point to point within it..In a GRIN medium, the optical rays follow curved trajectories, instead of straight lines as in a homogeneous medium. By an appropriate choice of the refractive index profile, a GRIN medium can have the same effect on light rays as conventional optical co
ATOPY
发表于 2025-3-29 12:56:59
Numerical Analysis of Surface Relief Gratingsng the methods introduced for the analysis of diffraction gratings one may recall the integral method,.the coupled wave method,.and the differential method..In this paper we will discuss a modal method for the analysis of lamellar surface relief diffraction gratings.
OUTRE
发表于 2025-3-29 18:03:26
Diffraction with Second-Harmonic Generation for the Formation of Self-Guided or “Solitary” Wavesracteristic length exceeds the propagation distance, will weaken its intensity and ability to spatially resolve a given area or spot. Propagation in optical waveguides is generally considered as the most effective approach for counterbalancing diffraction over finite propagation distances, utilizing
是限制
发表于 2025-3-29 22:14:25
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meretricious
发表于 2025-3-30 01:34:43
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CAMP
发表于 2025-3-30 07:58:00
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