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Cheju Island, Korea, using low-Z electron probe X-ray microanalysis: a direct proof of nitrate formation from seasalts. Environ. Sci. Technol., 35, 4487 4494 (2001c). Roth, B. and Okada, K. On the modi cation of sea-salt particles in the coastal atmosphere. Atmos. Environ., 32, 1555 1569 (1998) Scott, V. D. and Love, G. EPMA using low-energy (0.1 1.0 keV) X-rays an historical perspective. J. Anal. At. Spectrom., 14, 367 376 (1999). Small, J. A. The detection of low-intensity peaks in energydispersive X-ray spectra from particles. Scanning, 20, 92 98 (1998). Sorbier, L., Rosenberg, E., Merlet, C. and Llovet, X. EPMA of porous media: a Monte Carlo approach. Mikrochim. Acta, 132, 189 199 (2000). Staub, P. F. IntriX: a numerical model for electron probe analysis at high depth resolution. Part I. Theoretical description. X-ray Spectrom., 27, 43 57 (1998). Szal ki, I., Somogyi, A., Braun, M. and T th, A. Investigao o tion of geochemical composition of lake sediments using ED-XRF and ICP-AES techniques. X-Ray Spectrom., 28, 399 405 (1999). Szal ki, I., Os n, J., Ro, C.-U., Van Grieken, R. Quantio a tative characterisation of individual aerosol particles by thin-window electron probe microanalysis combined with iterative simulation. Spectrochim. Acta B, 55, 1015 1028 (2000). Szal ki, I., Os n, J., Worobiec, A., de Hoog, J. and Van o a Grieken, R. Optimization of experimental conditions of thinwindow EPMA for light element analysis of individual environmental particles. X-Ray Spectrom., 30, 143 155 (2001a). Szal ki, I., Szegedi, S., Varga, K., Braun, M., Os n, J. and o a Van Grieken, R. Ef ciency calibration of energy dispersive detectors for application in quantitative X- and -ray spectrometry. X-Ray Spectrom., 30, 49 55 (2001b). Trincavelli, J. and Castellano, G. MULTI: an interactive program for quanti cation in EPMA. X-ray Spectrom., 28, 194 197 (1999). Trincavelli, J., Castellano, G. and Riveros, J. A. Model for the Bremsstrahlung spectrum in EPMA application to standardless quanti cation. X-Ray Spectrom., 27, 27 86 (1998). Tsuji, K., Spolnik, Z., Wagatsuma, K., Zhang, J. and Van Grieken, R. E. Enhancement of electron-induced X-ray intensity for single particles under grazing-exit conditions. Spectrochim. Acta, B54, 1243 1251 (1999a). Tsuji, K., Wagatsuma, K., Nullens, R. and Van Grieken, R. Grazing exit electron probe microanalysis for surface and particle analysis. Anal. Chem., 71, 2497 2501 (1999b). Tsuji, K., Nullens, R., Wagatsuma, K. and Van Grieken, R. Elemental X-ray images obtained by grazing-exit electron probe microanalysis (GE-EPMA). J. Anal. At. Spectrom., 14, 1711 1713 (1999c).
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Windows 7. That said, for the best results, anyone utilizing Virtual PC to run an older operating system such as Windows XP along with whatever set of Windows 7 incompatible applications is well served to pack the host PC with as much RAM as physically possible. For typical PCs today, that means loading up with 4GB. Remember: you re running two operating systems and any number of applications simultaneously. That old Pentium 3 with 256MB of RAM just isn t going to cut it.
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In Program Auto mode, the camera sets both the shutter speed and the aperture in the same way as it does in Auto mode. The big difference is that you can override the shutter speed choice or the aperture choice, but not both at the same time. Set the Mode dial to P and look through the view nder and compose your photo. Pressing the Shutter button halfway down causes the camera to set the exposure and display the shutter speed and aperture in the view nder. Rotating the Front control dial changes the shutter speed and the camera then sets a new aperture to achieve proper exposure. This is great for when you
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The drift speed for practical drift elds varies between 1 m/ns and 10 m/ns. The maximum drift length realized up to now is about 4 cm.23
Yds = -9d - g,, Ybg = -jO)Cbg Ybd = -jo)Cbd Ybs = -jioCbs Ybb = jo)Cbb
THE IMAGE-ORTHICON* The image-orthicon was developed during World War II for military purposes. It was based on the design of a new, two-sided, conductive thin glass target that Albert Rose had proposed earlier and had already tested. It offered a way of correcting the instability of the orthicon as well as the possibility of higher sensitivity. In the final form of the image-orthicon, electrons from the photosensitive cathode on the inside face of the tube were accelerated along axial magnetic lines (produced by a DC solenoid electromagnet enveloping the tube, see Figures 10.2 and 10.3)* to strike the glass target structure. The complete target structure in*This section was written by Paul Weimer (2003). *It should be noted that a DC solenoid electromagnet is used to envelope all inline tube constructions, serving as it does to maintain the focus of electron streams moving along the axis of a tube. Both scanning beams as well as photoelectron images formed at a photosensor are served. Since this mechanism was first required to create the image-dissector-type tube, Philo Farnsworth obtained an early patent on the effect. RCA and other manufacturers were, therefore, obliged to obtain a license under his patent in order to produce the later sensitive types of camera tubes described here, which Farnsworth himself had no part in developing.
Schematic diagram of a portion of a T-cell EPROM array.
DNS is the locator service for Kerberos. The governing Request For Comment (RFC) 1510 speci es how DNS should resolve KDC hosts to IP addresses. Client computers need to send their messages to the IP address. If the IP address of the KDC cannot be resolved, it generates an error message to the client indicating that the domain cannot be located.
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