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Barkas-Andersen effect

The theoretical literature on the Barkas-Andersen effect is extensive. The present discussion focuses on the role of quantal V5. classical arguments. [Pg.100]

Traditionally the effect is incorporated into stopping theory via expansion in powers of Zj. As pointed out by Lindhard [21], there are two independent dimensionless parameters containing Zj, namely, the Bohr parameter k (equation (17)) and the Barkas parameter [Pg.100]

While the Bloch correction represents a series expansion in powers of k, the leading term in the Barkas-Andersen correction was found [22] to be oc B. [Pg.100]

One must expect the presence of mixed terms of the form k B in the expansion. The term of lowest order a —2, d = l), contributing oczf to the stopping cross section, would indicate a difference between the Barkas-Andersen correction evaluated from the Born series and the Bohr model, respectively. While such a comparison has not been performed in general terms, a numerical evaluation for the specific case of Li in C revealed a negligible difference [24]. [Pg.100]

In practice, series expansions of the stopping cross section in powers of Zi are only useful at high beam velocities where neither the Bloch nor [Pg.100]


Fig. 3. Barkas-Andersen effect predicted by binary stopping theory. Plotted are stopping numbers for singly charged Ar, Li, and H ions and for their anti-ions in Si. Also shown are the respective ion/anti-ion ratios. From Ref. [23]. Fig. 3. Barkas-Andersen effect predicted by binary stopping theory. Plotted are stopping numbers for singly charged Ar, Li, and H ions and for their anti-ions in Si. Also shown are the respective ion/anti-ion ratios. From Ref. [23].
Clever schemes have been developed to treat the Barkas-Andersen effect for light ions in an electron gas ([27,34] and others) in what is called the nonlinear quantum regime. While there is little doubt that there must be a lower velocity limit for the validity of Bohr-like stopping theory, a reliable estimate of this limit does not seem available, nor is there a demonstration of where and in what manner quantum mechanics is an indispensable feature. [Pg.101]

Moreover, estimates for an electron gas can hardly be representative for insulating materials. There have been speculations on the relevance of promotion effects [35], but theoretical estimates of the Barkas-Andersen effect in insulating solid materials have been performed only on the basis of classical theory so far... [Pg.101]


See other pages where Barkas-Andersen effect is mentioned: [Pg.91]    [Pg.100]    [Pg.100]    [Pg.101]    [Pg.107]    [Pg.91]    [Pg.100]    [Pg.100]    [Pg.101]    [Pg.107]    [Pg.123]    [Pg.210]   


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