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Rainbow scattering oscillations

Fig. 3. Part of the deflection function which is responsible for rainbow scattering. The shaded area determines the positions of the rainbow oscillations which are caused by the interference of trajectories around b2 and b3. Fig. 3. Part of the deflection function which is responsible for rainbow scattering. The shaded area determines the positions of the rainbow oscillations which are caused by the interference of trajectories around b2 and b3.
Upper and lower bounds for Dq AtH ) are reasonably well established from photo-ionization and flowing-afterglow measurements " 4.2 eV > Dq(AtV ) > 3.4 eV. Several groups have scattered protons oif argon. Wherever the analysis has depended exclusively on the location of the supernumerary rainbows, the derived values for Do(ArH ) are all < 3.4 eV. In one study, " superior resolution has revealed the rapid oscillations in the differential cross section and an analysis based on their location gives Do(ArH ) = 3.85 eV, agreeing with a theoretical calculated value of 3.9 Zero-point-energy... [Pg.207]

See other pages where Rainbow scattering oscillations is mentioned: [Pg.2055]    [Pg.233]    [Pg.372]    [Pg.2055]    [Pg.495]    [Pg.50]    [Pg.234]    [Pg.238]    [Pg.342]    [Pg.349]    [Pg.357]    [Pg.476]    [Pg.501]    [Pg.140]    [Pg.100]    [Pg.405]    [Pg.461]    [Pg.962]   
See also in sourсe #XX -- [ Pg.127 ]



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