
1 CHAPTER 4 OPTICAL ABERRATIONS 4.1 Introduction We have
... focal length in one plane than in the other. This may be the easiest way for an introductory explanation of the aberration. However, in practice it is unlikely that a lens has different focal lengths in two orthogonal planes; indeed it would be quite difficult to make such a lens. In most cases asti ...
... focal length in one plane than in the other. This may be the easiest way for an introductory explanation of the aberration. However, in practice it is unlikely that a lens has different focal lengths in two orthogonal planes; indeed it would be quite difficult to make such a lens. In most cases asti ...
TAPERED OPTICAL FIBER PLATFORM FOR HIGH SENSITIVITY
... correction algorithm. The anamorphic pupil relay causes two closely spaced sub-apertures in the entrance pupil to appear to be shifted further apart in the exit pupil. Analytic and numerical wave optics models demonstrate the effectiveness of this relay system, matching with experimental results. An ...
... correction algorithm. The anamorphic pupil relay causes two closely spaced sub-apertures in the entrance pupil to appear to be shifted further apart in the exit pupil. Analytic and numerical wave optics models demonstrate the effectiveness of this relay system, matching with experimental results. An ...
Chapter 23
... A goldfish is swimming inside a spherical bowl of water having an index of refraction n = 1.333. Suppose the goldfish is p = 10.0 cm from the wall of a bowl of radius |R| = 15.0 cm, as in the figure. Neglecting the refraction of light caused by the wall of the bowl, determine the apparent distance o ...
... A goldfish is swimming inside a spherical bowl of water having an index of refraction n = 1.333. Suppose the goldfish is p = 10.0 cm from the wall of a bowl of radius |R| = 15.0 cm, as in the figure. Neglecting the refraction of light caused by the wall of the bowl, determine the apparent distance o ...
F - mjburns.net
... light moving from air into glass will move toward the normal light moving from glass back into air will move away from the normal virtual focus ...
... light moving from air into glass will move toward the normal light moving from glass back into air will move away from the normal virtual focus ...
Training modules for an advanced interactive course on
... magnification factor. A sequence of images was produced with great ease using the OSLO® program simply as a compiler platform for the C-like macro language CCL. This was undertaken by placing the Hopkins formulae into the kernel of the sample code in the command fill_contour_sample, provided with th ...
... magnification factor. A sequence of images was produced with great ease using the OSLO® program simply as a compiler platform for the C-like macro language CCL. This was undertaken by placing the Hopkins formulae into the kernel of the sample code in the command fill_contour_sample, provided with th ...
optics(conceptuals)
... Q.46 Draw ray diagrams to show how a right angled isosceles prism can be used to (i) deviate the ray through 180 (ii) deviate the ray through 90 (iii) invert the rays. Q.47 What is the nature and size of the image formed by a concave mirror when the object is placed between its pole and focus? Dra ...
... Q.46 Draw ray diagrams to show how a right angled isosceles prism can be used to (i) deviate the ray through 180 (ii) deviate the ray through 90 (iii) invert the rays. Q.47 What is the nature and size of the image formed by a concave mirror when the object is placed between its pole and focus? Dra ...
Lecture 12: Fraunhofer diffraction by a single slit
... Problem: A propagating wave encounters an obstacle (i.e. a distortion of the wave-front occurs). How will the distortion influence the propagation of the wave? Fraunhofer diffraction: the resultant wave is measured very far away from the place where the wave-front was distorted (R>>size of the obsta ...
... Problem: A propagating wave encounters an obstacle (i.e. a distortion of the wave-front occurs). How will the distortion influence the propagation of the wave? Fraunhofer diffraction: the resultant wave is measured very far away from the place where the wave-front was distorted (R>>size of the obsta ...
ABCD law for Gaussian laser beams
... through a distance d and transmission through a thin lens with focal length f (or a concave mirror with focal length f ). From these elements we can derive more complicated systems. The ABCD matrix for a thick lens cannot be constructed from just these two elements. However, we can construct the mat ...
... through a distance d and transmission through a thin lens with focal length f (or a concave mirror with focal length f ). From these elements we can derive more complicated systems. The ABCD matrix for a thick lens cannot be constructed from just these two elements. However, we can construct the mat ...
A method for characterizing longitudinal chromatic aberration of
... 1·4, and a second when stopped down to 0·7NA, where the performance is seen to be slightly improved. It should be noted that this objective is of a much more recent design than the semi-apochromat 100× 1·36NA objective (C), results of which are also presented in Fig. 3. Figure 4(a) shows the variati ...
... 1·4, and a second when stopped down to 0·7NA, where the performance is seen to be slightly improved. It should be noted that this objective is of a much more recent design than the semi-apochromat 100× 1·36NA objective (C), results of which are also presented in Fig. 3. Figure 4(a) shows the variati ...
Light microscopy
... 5. By noting the length of an unknown structure in graticule divisions you can then convert this into absolute units of length, e.g. µm. 6. Each objective lens needs to be calibrated in the same way. Once calibrated objects can be measured in EPUs. EPUs are converted into absolute measurement using ...
... 5. By noting the length of an unknown structure in graticule divisions you can then convert this into absolute units of length, e.g. µm. 6. Each objective lens needs to be calibrated in the same way. Once calibrated objects can be measured in EPUs. EPUs are converted into absolute measurement using ...
The Absolute Sensitivity of Lens and Compound Eyes
... pupil of the dark adapted human eye, however, can be as large as 7 mm, which makes its area larger by a factor of approxim ately 105 times. Due to this fact, it is generally accepted that the num ber of light quanta available to the photoreceptors in insects is small compared to that available to an ...
... pupil of the dark adapted human eye, however, can be as large as 7 mm, which makes its area larger by a factor of approxim ately 105 times. Due to this fact, it is generally accepted that the num ber of light quanta available to the photoreceptors in insects is small compared to that available to an ...
High refractive index Fresnel lens on a fiber fabricated by
... increase by a factor of three (from Δn=0.12 to Δn=0.36). This leads to better light control in general, in particular in a tighter focal spot, which is advantageous for many applications. For example, in the case of optical trapping, a tighter focal spot allows trapping of smaller nanoparticles and ...
... increase by a factor of three (from Δn=0.12 to Δn=0.36). This leads to better light control in general, in particular in a tighter focal spot, which is advantageous for many applications. For example, in the case of optical trapping, a tighter focal spot allows trapping of smaller nanoparticles and ...
Is the Magnetosphere a Lens to MHD Waves?
... field lines in the upper half of the noon-midnightmeridian plane from the combineddipole/solenoid systemfor the case a = 10, Xo= 3 and v = 2 corresponding to an axial lengthL = 20. The value of a = 10 corresponds to the averagelocation of the magnetopause[Fairfield, 1991]. This field resembles close ...
... field lines in the upper half of the noon-midnightmeridian plane from the combineddipole/solenoid systemfor the case a = 10, Xo= 3 and v = 2 corresponding to an axial lengthL = 20. The value of a = 10 corresponds to the averagelocation of the magnetopause[Fairfield, 1991]. This field resembles close ...
F-number
In optics, the f-number (sometimes called focal ratio, f-ratio, f-stop, or relative aperture) of an optical system is the ratio of the lens's focal length to the diameter of the entrance pupil. It is a dimensionless number that is a quantitative measure of lens speed, and an important concept in photography. The number is commonly notated using a hooked f, i.e. f/N, where N is the f-number.