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MEMS-based handheld confocal microscope for in
MEMS-based handheld confocal microscope for in

Optical Properties of Aluminum Oxide
Optical Properties of Aluminum Oxide

... of the image before, during, and after data acquisition showed no sign of electron-beam irradiation damage of the specimen. The energy dispersion was 0.1 eV, which corresponded to 100 eV width of the spectrum. For each measurement, two spectra (for 10 s each) were acquired, one covering the energy r ...
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... overall thickness is sufficiently large for the problem on hand [16]. In the fifties and early sixties work was started in different laboratories on more powerful thin film design methods that did not require starting designs. Such computer programs are commonly called synthesis methods. In Russia, ...
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... Microscopy is a field of investigation which is used to study objects which are too small to be easily viewed by the human eye. Viewing and studying objects that range in size from millimeters (1 mm = 10-3 meter) to nanometers (1 nm = 10-9 meter) intrigues everyone and is currently applied to every ...
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... that SPPs can be molded more effectively and efficiently than ever, with only isotropic, nonmagnetic, and nondispersive dielectric materials introduced by the transformation. SPPs are bound surface waves at metal-dielectric interfaces, which implies that both the metal and dielectric materials need ...
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... stage. Here the output signal from the first link was used to drive the second link directly, and there was no signal processing or logic circuit in between. From both the simulation and the experimental results above, we know that the signal from one link has a rise–fall time of more than 2 ns. The ...
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... The trap itself is usually formed using a high numerical aperture (NA) microscope objective and the setup is usually built around an inverted microscope [33, 34]. This makes imaging of the sample easy since all optics is already there. In addition, it also makes it very straight forward to include m ...
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... typically uses a series of cylindrical atomic lenses formed by an optical standing wave (SW) to focus or manipulate atoms and deposit an atomic beam onto a substrate [1]. The collimation of the atomic beams plays an important role in atom lithography technology for two main reasons: the structure wi ...
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... are amplified rather than absorbed, and thus they always increase in amplitude with distance away from the interface for both below-critical and above-critical angles of incidence. These solutions are therefore the opposite of evanescent. Since there is no antonym to the term evanescent other than th ...
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Retroreflector



A retroreflector (sometimes called a retroflector or cataphote) is a device or surface that reflects light back to its source with a minimum of scattering. In a retroreflector an electromagnetic wavefront is reflected back along a vector that is parallel to but opposite in direction from the wave's source. The angle of incidence at which the device or surface reflects light in this way is greater than zero, unlike a planar mirror, which does this only if the mirror is exactly perpendicular to the wave front, having a zero angle of incidence.
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