By James A. Samson, David L. Ederer
This quantity is for practitioners, experimentalists, and graduate scholars in utilized physics, really within the fields of atomic and molecular physics, who paintings with vacuum ultraviolet functions and are wanting deciding upon the simplest form of glossy instrumentation. It presents first-hand wisdom of the cutting-edge gear resources and provides technical info on tips on how to use it, besides a extensive reference bibliography. Key good points * geared toward experimentalists who're short of selecting the simplest kind of sleek instrumentation during this utilized box * incorporates a unique bankruptcy on laboratory resources * presents an up to date description of state of the art apparatus and methods * encompasses a vast reference bibliography
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Example text
Sci. hTstrum. 63, 392 (1992). Dejus, R. , and Luccio, A. Nucl. Instrum. Methods' A347, 61 (1994). Howells, M. , and Kincaid, B. M. Lawrence Berkeley Laboratory Report 34751 (1993). Kim, K. J. Nucl. Inso'um. Methods A246, 67 (1986). Kitamura, H. Japan. J. Appl. Phys. 19, L 185 (1980). Kim, K. J. Nucl. Instrum. Methods A246, 71 (1986). Green, G. K. Brookhaven National Laboratory 50522 (1976); G. K. Green, Brookhaven National Laboratory 50595 (1977). , and Snyder, H. S. Ann. Phys. 3, 1 (1958). , and Kaminaga, U.
Plane of the monochromator, where it can be seen that the vertical image size is close to the one calculated, defining the source size limited resolution. Because dispersion across the exit plane is continuous, an exit slit has to be placed there to select the wavelength required. 03 mm (FWHM) in this case. Fig. 4a shows the image size in the middle of the ANCILLARY COMPONENTS 35 ion-beam interaction region, I in Fig. 2, and Fig. 03 mm. For these ray traces a polychromatic source was used, and the large number of rays lost is due to the fact that the slit selects only a small fraction of these corresponding to the bandwidth for which it has been set.
Because dispersion across the exit plane is continuous, an exit slit has to be placed there to select the wavelength required. 03 mm (FWHM) in this case. Fig. 4a shows the image size in the middle of the ANCILLARY COMPONENTS 35 ion-beam interaction region, I in Fig. 2, and Fig. 03 mm. For these ray traces a polychromatic source was used, and the large number of rays lost is due to the fact that the slit selects only a small fraction of these corresponding to the bandwidth for which it has been set.