1965
DOI: 10.1016/0029-5582(65)90478-5
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The energy loss of oxygen and chlorine ions in solids

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Cited by 173 publications
(25 citation statements)
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“…The background has been taken into account. The solid lines result from a least squares fitting inserting f ( T) from equation (12) ((or (13)) into (9) and varying q f s and 8 (or q f s and lk2). The numerical results are listed in Table 2 We have also measured the maximum Mossbauer absorption of the crystalline germanium absorber as a function of the target temperature.…”
Section: Recoilless Fractionsmentioning
confidence: 99%
See 1 more Smart Citation
“…The background has been taken into account. The solid lines result from a least squares fitting inserting f ( T) from equation (12) ((or (13)) into (9) and varying q f s and 8 (or q f s and lk2). The numerical results are listed in Table 2 We have also measured the maximum Mossbauer absorption of the crystalline germanium absorber as a function of the target temperature.…”
Section: Recoilless Fractionsmentioning
confidence: 99%
“…1 shows the y-yield Y as a function of ed for different values of the energy E(0). The integral was evaluated as a function of the bombarding energy using the specific stopping power dE/dex of germanium for lSO ions gained by interpolation of the energy range data for Ni and Ag [9]. …”
Section: Coulomb Excitationmentioning
confidence: 99%
“…Same as Fig. 1 for H and Cl in C. Original data from [5,26,27,[33][34][35][36][37][38][39][40][41][42][43]. Listing of proton in Ref.…”
Section: Comparison With Theorymentioning
confidence: 96%
“…The universal stopping function [23] B(E)/AZzff, where B ( E ) = -(dE/ds) E is given versus the energy per at'omic mass unit ( A is the inass and Zeff the efficient charge of t,he incident particle). The efficient charge of 4He+ ions is t'aken from [21]. The figure presents t>he dat'a of experiment's on the prot'on stopping obtained by Appleton et'al.…”
Section: M2(q)mentioning
confidence: 95%
“…With the inclusion of (20) and (21) formula (18) for high velocities of t'he incident particle u > t i F can be written as Here e ( r ) = 1 + C elGT f ( G ) is the normalized density of valence electrons in a given Formulae (21) and (23) are obtained without the additional assumption that the generalized oscillator strengths of atomic electrons are analogous to the harnionic oscillator (such approximation is used in [6]). As a basic parameter of stopping we involve the plasma frequency cop, rather than the mean ionization potential.…”
Section: Stopping Formula In the Non-uniform Eleetron Gasmentioning
confidence: 99%