232_1.PDF
... rebunching with good linearity using a modest rf system. However, it is much too far upstream to permit the sharp focus (small longitudinal beta function) required to match to the Afterburner. This design includes a new buncher structure located about 25 m upstream of the Afterburner. To reduce the ...
... rebunching with good linearity using a modest rf system. However, it is much too far upstream to permit the sharp focus (small longitudinal beta function) required to match to the Afterburner. This design includes a new buncher structure located about 25 m upstream of the Afterburner. To reduce the ...
Standing-wave transform spectrometer based on integrated MEMS
... cessing [7] that has enabled the real-time discrimination of different spectra. This simple processing also means that the operation of the spectrometer need not correspond exactly to the standard Fourier transform response, as long as the response of the spectrometer is linear in the signal; other ...
... cessing [7] that has enabled the real-time discrimination of different spectra. This simple processing also means that the operation of the spectrometer need not correspond exactly to the standard Fourier transform response, as long as the response of the spectrometer is linear in the signal; other ...
LINEAR AND NONLINEAR LIGHT BULLETS: RECENT
... Figures 7 and 8 illustrate the typical soliton norm-nonlinear wave numberHamiltonian diagram for stable three-dimensional continuous discrete light bullets confined by two-dimensional optical lattices for the value p = 20 of the lattice strength, and for unstable three-dimensional NLS solitons (p = ...
... Figures 7 and 8 illustrate the typical soliton norm-nonlinear wave numberHamiltonian diagram for stable three-dimensional continuous discrete light bullets confined by two-dimensional optical lattices for the value p = 20 of the lattice strength, and for unstable three-dimensional NLS solitons (p = ...
Post compression of high-energy femto
... It is very important that the pulse is broadened in such a way, that it is recompressible in order to create a pulse with a good temporal shape. Avoiding nonlinear effects as well as selecting the central part of the beam with a pinhole (because that is where the spectral broadening is the biggest) ...
... It is very important that the pulse is broadened in such a way, that it is recompressible in order to create a pulse with a good temporal shape. Avoiding nonlinear effects as well as selecting the central part of the beam with a pinhole (because that is where the spectral broadening is the biggest) ...
A Low Cost Optical Coherence Tomography Machine
... Time domain OCT was the format first used in early OCT machines. The concepts behind the technology are relatively straightforward and it is an easy technology to fabricate. As described above, the most basic component of time domain OCT is the interferometer. This device splits the light and sends ...
... Time domain OCT was the format first used in early OCT machines. The concepts behind the technology are relatively straightforward and it is an easy technology to fabricate. As described above, the most basic component of time domain OCT is the interferometer. This device splits the light and sends ...
Galileoscope Optics Guide - Teaching with Telescopes
... the Astronomical Society of the Pacific. A kit of materials was developed to go with these activities which included all the equipment needed to do these activities. Both the Hands-On Optics and Astronomy from the Ground Up projects were aimed at informal science educators such as museum educators a ...
... the Astronomical Society of the Pacific. A kit of materials was developed to go with these activities which included all the equipment needed to do these activities. Both the Hands-On Optics and Astronomy from the Ground Up projects were aimed at informal science educators such as museum educators a ...
Two-point microrheology and the electrostatic analogy
... 关5,6兴 and have found that in many experimental systems there is a significant frequency range over which Eq. 共1兲 is a good approximation to the single-sphere response function. At frequencies where the single-particle response function deviates significantly from Eq. 共1兲, the breakdown of the GSER c ...
... 关5,6兴 and have found that in many experimental systems there is a significant frequency range over which Eq. 共1兲 is a good approximation to the single-sphere response function. At frequencies where the single-particle response function deviates significantly from Eq. 共1兲, the breakdown of the GSER c ...
On the Prospect of Resonance Energy Transfer for Hybrid
... • where any part of this thesis has previously been submitted for a degree or any ...
... • where any part of this thesis has previously been submitted for a degree or any ...
Resonant nonlinear magneto-optical effects in atoms
... Magneto-optics plays an important role in the study of resonant light scattering in the direction of the incident light (forward scattering, FS) whose detection is normally hindered experimentally by the presence of a strong incident light beam that has identical properties (frequency, polarization, ...
... Magneto-optics plays an important role in the study of resonant light scattering in the direction of the incident light (forward scattering, FS) whose detection is normally hindered experimentally by the presence of a strong incident light beam that has identical properties (frequency, polarization, ...
Microscopic Light Field Particle Image Velocimetry
... Comparison of theoretical and computational velocity profiles in the narrow channel section, S3 . The channel dimensions for the CFD simulation are shown in row 1 of Table 2.3. (a) Profile comparison of v across x at z = 0 µm and y = 3500 µm. The red line represents the theoretical profile and the s ...
... Comparison of theoretical and computational velocity profiles in the narrow channel section, S3 . The channel dimensions for the CFD simulation are shown in row 1 of Table 2.3. (a) Profile comparison of v across x at z = 0 µm and y = 3500 µm. The red line represents the theoretical profile and the s ...
Exp. 71 - Caltech
... will look just like that shown in Figure 2, except the mode spacing will be ∆ν conf ocal = c/4L. The width of the transmission peaks ∆ν f whm stays roughly the same in principle, but in practice ∆ν f whm depends on how well the cavity is aligned, and how precisely we have L = Rmirror . Another nice ...
... will look just like that shown in Figure 2, except the mode spacing will be ∆ν conf ocal = c/4L. The width of the transmission peaks ∆ν f whm stays roughly the same in principle, but in practice ∆ν f whm depends on how well the cavity is aligned, and how precisely we have L = Rmirror . Another nice ...
Thomas Young (scientist)
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Thomas Young (13 June 1773 – 10 May 1829) was an English polymath and physician. Young made notable scientific contributions to the fields of vision, light, solid mechanics, energy, physiology, language, musical harmony, and Egyptology. He ""made a number of original and insightful innovations""in the decipherment of Egyptian hieroglyphs (specifically the Rosetta Stone) before Jean-François Champollion eventually expanded on his work. He was mentioned by, among others, William Herschel, Hermann von Helmholtz, James Clerk Maxwell, and Albert Einstein. Young has been described as ""The Last Man Who Knew Everything"".