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Velocity distributions, focusing

In TOF-SARS [9], a low-keV, monoenergetic, mass-selected, pulsed noble gas ion beam is focused onto a sample surface. The velocity distributions of scattered and recoiled particles are measured by standard TOF methods. A chaimel electron multiplier is used to detect fast (>800 eV) neutrals and ions. This type of detector has a small acceptance solid angle. A fixed angle is used between the pulsed ion beam and detector directions with respect to the sample as shown in figure Bl.23.4. The sample has to be rotated to measure ion scattering... [Pg.1805]

Time Focusing Devices. The resolution of the TOF analyzer is limited by the initial velocity spread of the ions. However, there are powerful devices that can compensate for this velocity distribution, and the most widespread techniques at present are the electrostatic ion reflector (electrostatic mirror) and time-lag focusing (delayed extraction). [Pg.41]

Abstract We briefly review selected results in astrophysics of neutron stars (NSs) obtained during the last two years, focusing on isolated radioquiet objects. We discuss in some detail the population synthesis of close-by isolated NSs (INSs), the spectra of INSs, the detection of spectral features in these sources (including cyclotron features), and the recent results on velocity distribution of NSs and accretion onto INSs from the interstellar medium. [Pg.53]

Let us focus our attention on a region of space containing molecules of N different chemical species. The viewpoint is versatile, in that molecules of the same kind in different energy levels may be considered to be different species. In definining the velocity distribution function for molecules of species i,... [Pg.618]

We focus our attention on the DIPR (direct interaction with product repulsion) model and its variant, the DIPR-DIP model, mainly because it can be used to predict an entire range of dynamic observables in chemical reactions angular and recoil velocity distributions, rotational energy and orientation and vibrational energy of the reaction products. It is also able to account for the switch from the rebound to the stripping reaction mechanism for a given system when the collision energy is increased. The beauty of the model is its ability to include semiempirical parameters, each of which is related to a different physical phenomenon. [Pg.3012]

Various approximate formulas for the velocity distribution in the buffer layer can be found, for example, in [138, 276, 398]. Choosing not to focus on these formulas (since these do not have sufficient theoretical justification), we only indicate a simple interpolation formula with a wider scope ... [Pg.34]

Today, the modern version of time-lag focusing, or delayed extraction,14 16 is used in almost all MALDI-TOF mass spectrometers. It is in fact a special case of the Wiley and McLaren method, in which the initial spatial distribution (usually a very thin sample and matrix mixture dried on a stainless steel plate) is assumed to be zero. Therefore, after the delay time the velocity and spatial distributions are correlated, i.e. ions of highest velocity have moved the greatest distance. This space velocity correlated focusing has been described by Colby and Riley,17 and provides considerably better focusing than can be obtained from two independent and uncorrelated initial distributions in space and velocity/energy that comprise the general Wiley-McLaren case. [Pg.295]

Another velocity distribution occurs when the hydrodynamic flow is caused by capillary forces in a stabilizing flat bed sorbent, when evaporation of the electrolyte from the surface can occur. If this evaporation is not too intensive, it is equal over the whole surface of the sorbent. Concomitantly, with the buffer evaporation from the surface, the buffer solution is supplied from both electrode vessels due to surface forces. Thus, a longitudinal flow originates the velocity of which is a function of the distance. This flow can be made use of in focusing methods [1,9,12,13]. [Pg.37]

Abstract Prediction of droplet size and velocity distribution produced by splash plate requires information on the liquid sheet characteristics and its breakup process. This chapter focuses on the sheet produced by splash plate nozzles and their characteristics such as sheet breakup length and produced droplet size. It explains different flow regimes occurring in splash plate nozzles as well as various breakup lengths provided by different researchers. Sheet formation phenomenon is explained theoretically and at the end correlations for droplet size prediction are provided. [Pg.709]

IV. Spatially dependent velocity distributions. When the spectrum is independent of position, the central problem is the determination of the energy-transfer cross sections. The calculation of the spectrum once these cross sections are known is a straightforward procedure. The cross-section aspect of the problem is both more difficult from a physics point of view, and more time consuming from the point of view of machine computation. This situation is reversed when we come to consider the spatial dependence of the slow neutron spectrum. The cross sections needed are the same ones that already have been computed for the infinite medium spectrum problem. The transport equation must now be solved in at least two variables, and in a form for which the existing approximate techniques are not very well adapted. The focus of the problem therefore shifts to the development of appropriate techniques for solution of the transport equation when the energy and position variables are coupled in such a way that neutrons can both gain and lose energy in a collision. [Pg.39]

Further publications have presented microscopic methods for the 3D determination of the velocity distribution in microchaimels by means of the 3D point spread function (PSF). With defocus, the spot diameter of a nanoparticle first increases, and then for larger displacements from the focus complex ring intensity patterns are developed. The full 3D pattern represents the PSF of the optical system and is determined mainly by the objective lens of the microscope system. The intensity pattern, i.e. the number and diameter of rings and the relative intensity of rings, gives information about the distance of the object from the imaging focal plane. Speidel... [Pg.108]


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