Atom, Molecule, and Cluster Beams I: Basic Theory, - download pdf or read online

By Hans Pauly

ISBN-10: 3642086233

ISBN-13: 9783642086236

ISBN-10: 3662042134

ISBN-13: 9783662042137

This ebook offers a constant, updated description of the super manifold and sundry experimental recommendations which these days permit paintings with impartial debris. It lays the actual foundations of a few of the experimental options, which make the most of equipment from such a lot fields in physics. for that reason this booklet is meant not just as a reference average for researchers, but additionally as a textbook to let scholars to achieve a superior heritage and creation to the sphere and its concepts.

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Additional resources for Atom, Molecule, and Cluster Beams I: Basic Theory, Production and Detection of Thermal Energy Beams

Sample text

5 GHz prevents recognition of any spectral details. The lower half (b) shows the same segment employing a collimated beam with the Doppler spread reduced to 15 MHz [Demtröder (1996)]. g. measurements of the angle and energy distribution of photoelectrons [Baum et al. (1970), Luhmann et al. (1998)], some on polarized target beams, as weIl as photofragmentation studies [Hepbum (1992)]. Continuous light sources (synchrotron radiation) facilitate studies of a large variety of ionization processes of molecules as a function of the wave1ength [Yencha et al.

3). Simultaneous measurement of the time-of-flight through a flight seetion of about I m allows the determination of the energy transfer between helium atoms and the crystal. The flight section consists of four differentially pumped stages (evacuated I. The Role of Molecular Beams in the 20th Century 33 by 150 Vs oil diffusion pumps), separated from each other by small apertures. The large number of differentially pumped stages is necessary to achieve the largest possible gradient in helium partial pressure between the target chamber (helium partial pressure around 5x 10-9 mbar during measurements) and the detector charnber proper (evacuated by a 450 Vs turbo-molecular pump) which should operate with helium partial pressures below 10- 14 mbar.

The various differential pumping stages are designated as PI to P9 . (KI) source chamber, (K2) target chamber, (K3) detector chamber. (I) helium beam source, (2) skimmer, (3) chopper, (4) manipulator, (5) mass spectrometer for residual gas analysis, (6) electron diffraction device for structure analysis of surface, (7) ion source for surface cleaning, (8) Auger spectrometer for determination of purity of SUfface, (9) surface under study, (10) spring bellows, (\ I) ion source and lens system, (12) 90° deflection by a magnetic sector field, (\3) electron multiplier 34 l.

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Atom, Molecule, and Cluster Beams I: Basic Theory, Production and Detection of Thermal Energy Beams by Hans Pauly

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