Download Atom, Molecule, and Cluster Beams I: Basic Theory, by Hans Pauly PDF

By Hans Pauly

This e-book offers a constant, updated description of the tremendous manifold and sundry experimental ideas which these days let paintings with impartial debris. It lays the actual foundations of a number of the experimental thoughts, which make the most of tools from such a lot fields in physics. accordingly this booklet is meant not just as a reference average for researchers, but additionally as a textbook to allow scholars to realize a high-quality historical past 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

Example text

1), the energy ei of the i-th state is well approximated to be additive and consisting of three contributions, the internal energy and the specific heat also constitute sums of three contributions. 6) Correspondingly, the total distribution function becomes a product of three distribution functions. These functions and the partial partition functions are discussed in the following sections. 1 The Maxwellian Velocity Distribution First we treat the distribution of translational energy. 7) 2. /h3, the number of quantum states in the volume element d.

Inside one fmds the electron impact ionization source and a photoionization region, cooled with liquid helium (25 K). 5xl0-1J torr. I. The Role of Molecular Beams in the 20th Century 29 The quadrupole mass filter (see Sect. 3) and the scintillation detector (see Sect. 4) are housed inside the pumping stage designated by (6). This stage too is pumped by a turbo-molecular pump (300 1/s). A B p P Fig. 7. Schematic of a universal scattering apparatus for the investigation of inelastic and reactive collision processes employing crossed molecular beams [Yang et al.

The Role of Molecular Beams in the 20th Century As an example for the manipulability of atoms Fig. 4 shows the reflection of Cs atoms by an atomic concave mirror. 25 mm) from a magnetooptical trap falls onto an atomic mirror, is reflected there, reaches its tuming point in the gravitational field, and falls back again onto the mirror. This process repeats itself several times ("atomic trampoline"), while the atoms cross a laser beam each time, making their temporal motion visible by fluorescence [Aminoff et al.

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