optics. Develop multiplex assays with the ability to detect fluorescent signal in four distinct channels.
optics. Fibers per node -4 dedicated Forward TX: 2:1 split ratio Reverse TX: RPTV 1 - FP laser Redundancy: RF bypass where applicable (architecture dependent) Dual receives with hot optics input to both RXs when available from GI
optics. The term "Optics" shall mean the 6x Basic starter monocular optics components used in connection with PPS which is manufactured by or for Perisphere.
optics. EMC may source optics for use with the VDX Products from Brocade or direct from suppliers consistent with those used in EMC’s own Storage Products. Use of optics as described above will not void the warranty on the VDX Products, and, Brocade will continue to support the VDX Products. The optic quality and part numbers will be reviewed on a quarterly basis.
optics. The model of the reflectometer SONATA is shown in Fig. 1. The concept of the SONATA neutron reflectometer contains a number of innovations that define unique experimental possibilities: - variation of operating wavelengths and time-of-flight resolution in fairly wide ranges, as well as complete elimination of parasitic slow neutrons (making the main contribution to the background) using a chopper with a limited passband; - a combination of vertical and horizontal focusing onto the sample to achieve maximum possible fluxes with the option of reflectometry with a fan-shaped beam; - polarization analysis in a wide range of angles using a fan-shaped analyzer; - measurements with vector analysis of the polarization of the reflected beam; - fast switching between survey modes: slit / quasi-point geometry; time-of-flight / constant wavelength technique; standard / fan beam option; unpolarized / polarized beam mode.
optics. Firstly, exponential sensitivity of the evolution of the intra-cavity ray to the initial conditions is required, and, secondly, the ray has to remain confined inside the resonator for a sufficient time to produce mixing. We have designed a bifocal mirror that, in combination with a conventional concave mirror, forms a resonator with an unstable inner and a stable outer part (“inner” and “outer” refer here to the transverse coordinate). The unstable part provides for the exponential sensitivity, whereas the stable part provides for the mixing. We note that although the resonator comprises an unstable part, the resonator is stable in an overall sense. In order to achieve chaos in this overall stable cavity, we need, as mentioned above, a long residence time of the light in the cavity. This implies that the finesse must be as large as possible and thus requires a solid understanding of the imperfections of a Xxxxx- Xxxxx. In fact, this has become the main theme of this thesis. Another motivation for a thorough understanding of imperfections is that the unstable part of the bifocal resonator acts as a sort of “macro”-imperfection and produces, in combination with the stable part, a challenging and complex physical system. For full appreciation and understanding of this system, it is necessary to be able to distinguish phenomena unique for this configuration from effects also present in conventional resonators, comprising two
optics. Advanced, free-form, optics designed with unique "multi-scale lenses" to create uniform light distribution and glare-reduction. SOLID STATE DESIGN Unique “SSD” design, simple, and advanced. Ensures durability of LED chip. All parts are individual, rugged, and strong. ENERGY EFFICIENCY Our photoelectric conversion is the most efficient method to save energy and produce more light. C CtlTC SCRlCS INNOvATION LIGHTS UP THE FUTURE THERMAL MANAGEMENT Seamless link between aerometal materia and numerous heat sink vents to improve heat management and ensure stability of lighting system.
optics. Additionally, a fifth set of deflector plates could be pulsed to act as a mass gate to only allow the anion of interest to enter the detachment region. One plate of each pair was grounded while the opposite plate was connected to a dual polarity voltage source. Once inside the VMI optics, the mass selected anions were intercepted by the polarized, focused output of a Nd:YAG pumped dye laser or an excimer pump dye laser operating at a photon energy above the detachment threshold of the species of interest. Typical detachment laser pulse energies were in the range of 0.5 – 1.0 mJ, with a beam diameter of < 2 mm. The dye laser linewidths were approximately 0.3 cm-1 (FWHM). Wavelength calibrations of the lasers were established using the gas phase absorption spectrum of the B – X transition of room temperature I2. The absolute energies of the I2 lines were taken from the PGOPHER software package.53 The velocity map imaging electrodes were replicated from the original Eppink and Xxxxxx design49 using 1/16 in thick 304 stainless steel. The photoelectrons produced within the VMI lens were accelerated down a 66 xx xxxx drift region, shielded from external electric and magnetic fields by layers of mu-metal, to the detector (Photonis USA, Inc. 75 mm Chevron stacked microchannel plates (MCP) with a fiberoptic P47 phosphor screen). Images from the detector screen were recorded by a CCD camera (Physimetrics UI-2230SE-M-GL, 1024x768). The photodetached electrons were discriminated from all other charged particles by pulsing the voltage (gain) on the MCPs at the appropriate arrival time. Individual cycles of the experiment were recorded and summed over several hundred thousand laser pulses to produce an image. The final image was saved using the imaging collection software developed by Li et al.54. Transformation of the image from velocity space to energy was done using the Maximum Entropy Velocity Xxxxxxxx Reconstruction (MEVELER) technique55. The total emission of the screen from electron or anion impacts could also be monitored with a photomultiplier tube positioned off axis from the camera (not shown in Figure 1). This mode of detection produced a TOF-MS spectrum, and was extremely useful in the optimization of anion and photoelectron production. The repetition rate of the experiment was 10 Hz. All images were calibrated using the known transitions from detachment of the sulfur anion, S-.56-58
optics. 1. Optics shall be beads or elements incorporated into pavement markings so as to produce reflectorized pavement markings. Optics shall be one of the products listed on the Agency’s Approved Product List for the respective material specification and shall meet the following requirements.
