Lab 2: Abbe Theory of Imaging
... The set-up is now ready for the examination of slides. The image will be observed on an index card in another modified target assembly. The location of the observation plane will be about 450mm after the last lens and will give an image about twice the size as the object slide when the card at the b ...
... The set-up is now ready for the examination of slides. The image will be observed on an index card in another modified target assembly. The location of the observation plane will be about 450mm after the last lens and will give an image about twice the size as the object slide when the card at the b ...
Conference title, upper and lower case, bolded, 18 point type
... schematic cross-section of such an axicon with angle . ...
... schematic cross-section of such an axicon with angle . ...
Fiber Optic
... conversion efficiency of a photodetector. ii ) Dark current: Dark current is the leakage current that flows through a photodiode with no light input. iii ) Transit time: Transit time is the time it takes a light-induced carrier to travel across the depletion region. iv ) Spectral response: Spectral ...
... conversion efficiency of a photodetector. ii ) Dark current: Dark current is the leakage current that flows through a photodiode with no light input. iii ) Transit time: Transit time is the time it takes a light-induced carrier to travel across the depletion region. iv ) Spectral response: Spectral ...
Fourier Spectra for Non-Homogeneous Patterns
... waves, then one may proceed to optimize the spatial analysis of the pattern using the method employed by Polis (1974). Namely, one estimates the rms variation in the wave number ak of a given component caused by the nonhomogeneity over a variable distance, I. This variation will usually increase mon ...
... waves, then one may proceed to optimize the spatial analysis of the pattern using the method employed by Polis (1974). Namely, one estimates the rms variation in the wave number ak of a given component caused by the nonhomogeneity over a variable distance, I. This variation will usually increase mon ...
Chapter 8a Wave Optics
... 3. The wave theory of light (Huygens (1629-95)) 4. Interference effects of light were first observed by Thomas Yong in 1800. ...
... 3. The wave theory of light (Huygens (1629-95)) 4. Interference effects of light were first observed by Thomas Yong in 1800. ...
Chapter 23
... • If a wave hits a barrier, at least part of it will bounce back. This is reflection. • The law of reflection states that the angle of incidence (i) is equal to the angle of reflection (r). • Looking in the mirror is an example of light waves reflecting back with your image. ...
... • If a wave hits a barrier, at least part of it will bounce back. This is reflection. • The law of reflection states that the angle of incidence (i) is equal to the angle of reflection (r). • Looking in the mirror is an example of light waves reflecting back with your image. ...
PDF
... normal optical fibers in that they consist of a core surrounded by cladding, such that light is guided within the core of the fiber. The primary difference between PCF and standard optical fibers is that PCFs feature an air-silica cross-section, whereas standard optical fibers have an all-glass cros ...
... normal optical fibers in that they consist of a core surrounded by cladding, such that light is guided within the core of the fiber. The primary difference between PCF and standard optical fibers is that PCFs feature an air-silica cross-section, whereas standard optical fibers have an all-glass cros ...
Basics in Confocal Microscopy Handouts
... Imaging e.g. CFP and YFP simultaneous is important for some biological applications. ...
... Imaging e.g. CFP and YFP simultaneous is important for some biological applications. ...
Do Solitonlike Self-Similar Waves Exist in Nonlinear Optical Media?
... fundamental bright (or dark) spatial soliton using an appropriate phase mask placed at the entrance to the gradedindex waveguide. If the amplifier gain g satisfies the condition given in Eq. (11), the entering phase-chirped spatial soliton propagates inside the amplifier as a self-similar wave found ...
... fundamental bright (or dark) spatial soliton using an appropriate phase mask placed at the entrance to the gradedindex waveguide. If the amplifier gain g satisfies the condition given in Eq. (11), the entering phase-chirped spatial soliton propagates inside the amplifier as a self-similar wave found ...
