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This reflector bends the light, keeping the Light guide straight and the beam profile uniform. It also keeps the working distance as short as possible. An ...

Courant and Snyder found that the net effect of alternating the field gradient was that both the vertical and horizontal focusing of protons could be made strong at the same time, allowing tight control of proton paths in the machine. This increased beam intensity while reducing the overall construction cost of a more powerful accelerator. The theory revolutionised cyclotron design and permitted very high field strengths to be employed, while massively reducing the size of the magnets needed by minimising the size of the beam. Most particle accelerators today use the strong-focusing principle.

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Earnshaw's theorem shows that simultaneous focusing in two directions transverse to the beam axis at once by a single magnet is impossible - a magnet which focuses in one direction will defocus in the perpendicular direction. However, iron "poles" of a cyclotron or two or more spaced quadrupole magnets (arranged in quadrature) can alternately focus horizontally and vertically, and the net overall effect of a combination of these can be adjusted to focus the beam in both directions.[1][2]

Oct 10, 2024 — The meaning of F-NUMBER is the ratio of the focal length to the aperture in an optical system.

Jun 20, 2023 — One large segment of experts, for example, defines polarization as a state that can be entered and exited. For another, it is a phenomenon that ...

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Its primary function is to further magnify the image produced by the objective lens. Ocular lenses are often interchangeable, allowing users to customize ...

In accelerator physics strong focusing or alternating-gradient focusing is the principle that, using sets of multiple electromagnets, it is possible to make a particle beam simultaneously converge in both directions perpendicular to the direction of travel. By contrast, weak focusing is the principle that nearby circles, described by charged particles moving in a uniform magnetic field, only intersect once per revolution.

The action upon a set of charged particles by a set of linear magnets (i.e. only dipoles, quadrupoles and the field-free drift regions between them) can be expressed as matrices which can be multiplied together to give their net effect, using ray transfer matrix analysis.[7] Higher-order terms such as sextupoles, octupoles etc. may be treated by a variety of methods, depending on the phenomena of interest.

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The FT/IR-4X is a powerful Mid-IR FTIR spectrometer with many features that you find in a research grade instrument, such as non-hygroscopic KRS-5 windows to ...

One of the characteristics of a microscope eyepiece is the microscopic Field of View commonly abbreviated FOV. The size of the FOV is ...

Modern systems often use multipole magnets, such as quadrupole and sextupole magnets, to focus the beam down, as magnets give a more powerful deflection effect than earlier electrostatic systems at high beam kinetic energies. The multipole magnets refocus the beam after each deflection section, as deflection sections have a defocusing effect that can be countered with a convergent magnet 'lens'.

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A circular polarizing filter absorbs rays of sunlight, by rotating the ring you control the effect. A Circular Polarizer is used on cameras with beam ...

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Vision Forward stand magnifiers are placed directly on the reading surface, a good option for people with limited hand strength. 3X-14X available.

Strong focusing was first conceived by Nicholas Christofilos in 1949 but not published (Christofilos opted instead to patent his idea).[3] In 1952, the strong focusing principle was independently developed by Ernest Courant, M. Stanley Livingston, Hartland Snyder and J. Blewett at Brookhaven National Laboratory,[4][5] who later acknowledged the priority of Christofilos' idea.[6] The advantages of strong focusing were then quickly realised, and deployed on the Alternating Gradient Synchrotron.

So a 10x objective plus a 10x eyepiece = 100x magnification. And a 100x objective lens with 20x eyepieces = 2,000x magnification - right? False! False ...

This can be shown schematically as a sequence of divergent and convergent lenses. The quadrupoles are often laid out in what are called FODO patterns (where F focusses vertically and defocusses horizontally, and D focusses horizontally and defocusses vertically and O is a space or deflection magnet). Following the beam particles in their trajectories through the focusing arrangement, an oscillating pattern would be seen.