Birefringence in Optical Fibers: Applications
... categories: (i) high-birefringence (Hi-Bi) fibers and (ii) single-polarization single-mode (SPSM) fibers. 9.2.1 High-birefringence (Hi-Bi) fibers In the case of highly birefringent fibers, the propagation constants of the two orthogonally polarized modes are made quite different from each other so t ...
... categories: (i) high-birefringence (Hi-Bi) fibers and (ii) single-polarization single-mode (SPSM) fibers. 9.2.1 High-birefringence (Hi-Bi) fibers In the case of highly birefringent fibers, the propagation constants of the two orthogonally polarized modes are made quite different from each other so t ...
Discovery of the Classical Bose–Einstein Condensation of Magnons
... ciently low, so that they can form the BEC before their relaxation occurs in the case of pulsed NMR. In the case of continuous NMR, magnons should be gener ated more rapidly than they decay at relatively small pumping amplitudes. The magnetic subsystem should not be overheated. Second, in order to ...
... ciently low, so that they can form the BEC before their relaxation occurs in the case of pulsed NMR. In the case of continuous NMR, magnons should be gener ated more rapidly than they decay at relatively small pumping amplitudes. The magnetic subsystem should not be overheated. Second, in order to ...
PPTX
... Dots are small so that the spectra do not fall on top of each other, allowing the input image to be sampled contiguously. The disadvantage is that the length of spectrum that can be produced without overlapping is very small and the packing of the CCD is not efficient. Examples: VLT FLAMES(GIR ...
... Dots are small so that the spectra do not fall on top of each other, allowing the input image to be sampled contiguously. The disadvantage is that the length of spectrum that can be produced without overlapping is very small and the packing of the CCD is not efficient. Examples: VLT FLAMES(GIR ...
ComplexLightBookChapterEG
... which for the photon of our example is 3.3 pN. This force is greater than the weight of a 5-µm plastic sphere: 0.67 pN. The realization of these magnitudes and the wide-spread use of lasers has led to the development of optical tweezers, which can trap and move micron-sized objects in a small sample ...
... which for the photon of our example is 3.3 pN. This force is greater than the weight of a 5-µm plastic sphere: 0.67 pN. The realization of these magnitudes and the wide-spread use of lasers has led to the development of optical tweezers, which can trap and move micron-sized objects in a small sample ...
Comparison of two-color methods based on wavelength and
... the refraction index can be corrected by a proposed method [2] for measuring the distance with two wavelengths (two colors) by utilizing the wavelength dependence of the refractive index of air. Several researchers [3]–[15] have studied this twocolor method. For example, the correction of the phase ...
... the refraction index can be corrected by a proposed method [2] for measuring the distance with two wavelengths (two colors) by utilizing the wavelength dependence of the refractive index of air. Several researchers [3]–[15] have studied this twocolor method. For example, the correction of the phase ...
IX71/IX81 - Olympus Microscopy Resource Center
... open a new world of live cell imaging. As new fluorochromes are developed and new methods of light excitation and manipulation become more popular for live cell experiments, more and more researchers will require the use of low phototoxicity near-IR wavelengths in addition to the conventional visibl ...
... open a new world of live cell imaging. As new fluorochromes are developed and new methods of light excitation and manipulation become more popular for live cell experiments, more and more researchers will require the use of low phototoxicity near-IR wavelengths in addition to the conventional visibl ...
Flatland Electrons in High Magnetic Fields
... turns out this is crucial for much of the phenomena observed in these systems: by reducing the disorder and the electron-impurity interaction, electrons are allowed to interact with each other, and the result is a host of new many-body ground and excited states. Another ...
... turns out this is crucial for much of the phenomena observed in these systems: by reducing the disorder and the electron-impurity interaction, electrons are allowed to interact with each other, and the result is a host of new many-body ground and excited states. Another ...
Nonlinear effects in Silicon Waveguides
... spectrally resolved FROG trace of input pulses at 1500 nm. ...
... spectrally resolved FROG trace of input pulses at 1500 nm. ...
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... (i) The presence of the P1–P6 components is a common signature of all the low-temperature -PL spectra recorded in the thin InSe flakes, which supports the physical origin of each one of the P1–P6 components discussed in the main text. (ii) The -PL spectra obtained in terraces with similar thicknes ...
... (i) The presence of the P1–P6 components is a common signature of all the low-temperature -PL spectra recorded in the thin InSe flakes, which supports the physical origin of each one of the P1–P6 components discussed in the main text. (ii) The -PL spectra obtained in terraces with similar thicknes ...
RAJ EAP talk - Rob Jackson`s Website
... materials and suggest ones. – e.g. by calculating transitions with different dopants before the sample preparation is carried out. ...
... materials and suggest ones. – e.g. by calculating transitions with different dopants before the sample preparation is carried out. ...
The LISA Optimal Sensitivity
... transmission from spacecraft 2 共along L 3 ). Similarly, y 21 is the corresponding time series derived from reception at spacecraft 1 with transmission from spacecraft 3. The other four one-way relative frequency time series from signals exchanged between the spacecraft are obtained by cyclic permuta ...
... transmission from spacecraft 2 共along L 3 ). Similarly, y 21 is the corresponding time series derived from reception at spacecraft 1 with transmission from spacecraft 3. The other four one-way relative frequency time series from signals exchanged between the spacecraft are obtained by cyclic permuta ...
Sample pages 1 PDF
... any rays that are not normal (perpendicular) to the prism when they enter or exit it will be dispersed more by BaK4 glass than by BK7 glass. At the magnification in most binoculars, you are unlikely to be able to detect this in use, but it is one of the reasons that BK7 prisms may be a preferable pr ...
... any rays that are not normal (perpendicular) to the prism when they enter or exit it will be dispersed more by BaK4 glass than by BK7 glass. At the magnification in most binoculars, you are unlikely to be able to detect this in use, but it is one of the reasons that BK7 prisms may be a preferable pr ...
Investigation of positive and negative modes of nanosecond pulsed
... In this paper we analyze the development of nanosecond pulsed plasma in water for negative and positive polarity, on the basis of this electrostriction mechanism as a possible initiation phase. High voltage pulses with nanosecond rise times are used to ignite discharges in pure water using both posi ...
... In this paper we analyze the development of nanosecond pulsed plasma in water for negative and positive polarity, on the basis of this electrostriction mechanism as a possible initiation phase. High voltage pulses with nanosecond rise times are used to ignite discharges in pure water using both posi ...
Beam Diagnostics 2 - ab-abp-frankz
... no information on x-y coupling with 1 wire (need 3 wires at common location) dynamic range: saturation of detectors (PMTs) single-pulse beam heating wire thickness (adds in quadrature with beam size) ...
... no information on x-y coupling with 1 wire (need 3 wires at common location) dynamic range: saturation of detectors (PMTs) single-pulse beam heating wire thickness (adds in quadrature with beam size) ...
Observation of a Localization Transition in
... replaced with Wn , where Wn are random numbers drawn from a flat distribution ranging from 1 to 1. In this case there is no sharp localization transition at nonzero , instead there is a smooth decrease of the localization length as the strength of the disorder is increased. For infinite one-dim ...
... replaced with Wn , where Wn are random numbers drawn from a flat distribution ranging from 1 to 1. In this case there is no sharp localization transition at nonzero , instead there is a smooth decrease of the localization length as the strength of the disorder is increased. For infinite one-dim ...
Negative refraction, subwavelength focusing and beam formation by
... does not suffer from Bragg reflections inside the PC and a well-defined single beam propagation is guaranteed within the PC. The scaled frequency range that gives negative refraction extends from ω̃ == 0.2093 to ω̃ = 0.2467 By using the setup depicted in figure 4(a), the negative refraction in this ...
... does not suffer from Bragg reflections inside the PC and a well-defined single beam propagation is guaranteed within the PC. The scaled frequency range that gives negative refraction extends from ω̃ == 0.2093 to ω̃ = 0.2467 By using the setup depicted in figure 4(a), the negative refraction in this ...
Dual-color total internal reflection fluorescence cross
... excitation and single-photon detection. Nonetheless, for several applications, TIR illumination can provide further benefits, for instance when ligands interacting with receptors immobilized onto a surface are to be studied.9–12 First, in TIRFCCS the molecules are only excited near the glass-sample ...
... excitation and single-photon detection. Nonetheless, for several applications, TIR illumination can provide further benefits, for instance when ligands interacting with receptors immobilized onto a surface are to be studied.9–12 First, in TIRFCCS the molecules are only excited near the glass-sample ...