Abstract:Projectile (Zl) and target (Z2) K-vacancy production cross sections induced by 3.6-, 4.75-, and 5.9-MeV/amu 2asU ions in selected targets between C and U are reported. The cross sections are discussed within the context of the molecular model of inner-shell vacancy production in heavy-ion-atom collisions. The measured l sa and 2pa excitation cross sections are compared with semiempirical formulas, and with the perturbed-stationarystates calculations of Betz et al. The dependence of these cross sections on Z, =… Show more
“…to [18]. Since both systems are measured at four different projectile velocities, one gets for (20) agree fairly well with those from theory. Certainly, the variation of the theoretical energies within the whole covered Ro-range amounts only to ~40 keV and is even smaller than the statistical errors of the "measured" binding energies.…”
Section: St-binding Energies Extracted From 1 S~r Excitation Datasupporting
confidence: 67%
“…Some methods based on the encouraging agreement with experimental results are proposed in order to extract from measured P~(b)-data or mean impact parameters <b> the binding energy of the quasimolecular lso-state as function of R o ( (20,22,27)). Looking to the assumptions made when deriving these analytical expressions one finds that the basic physical quantity entering into these formulae is the energy transferred to the ls a electron in the collision.…”
Section: Discussionmentioning
confidence: 96%
“…3 we show the values for Elso(Ro) extracted from the experiments acc. to (20), whereas the full curve gives the calculated values acc. to [18].…”
Section: St-binding Energies Extracted From 1 S~r Excitation Datamentioning
confidence: 99%
“…Concerning the total lsa excitation cross section for ctZ > 130, a lot of experimental data are available [19,20]. From the measured lso-cross sections, D(Z) can be determined in the following way: Starting with an arbitrary value for <Ro> one calculates acc.…”
Section: Total 1so Cross Section Data For C~z> Imentioning
An analytical formula for the excitation probability of the quasimolecular l sa orbital as a function of the impact parameter b is derived for collision systems with e(Z 1 +Z2)> 1. This formula describes well all existing experimental data for those collision systems except for the heaviest system Pb + Cm (Z 1 + Z 2 = 178) at impact parameters b <40 fm. It is discussed in which way energies of the quasimolecular l so-orbital can be extracted from experimental lso-vacancy production data.
“…to [18]. Since both systems are measured at four different projectile velocities, one gets for (20) agree fairly well with those from theory. Certainly, the variation of the theoretical energies within the whole covered Ro-range amounts only to ~40 keV and is even smaller than the statistical errors of the "measured" binding energies.…”
Section: St-binding Energies Extracted From 1 S~r Excitation Datasupporting
confidence: 67%
“…Some methods based on the encouraging agreement with experimental results are proposed in order to extract from measured P~(b)-data or mean impact parameters <b> the binding energy of the quasimolecular lso-state as function of R o ( (20,22,27)). Looking to the assumptions made when deriving these analytical expressions one finds that the basic physical quantity entering into these formulae is the energy transferred to the ls a electron in the collision.…”
Section: Discussionmentioning
confidence: 96%
“…3 we show the values for Elso(Ro) extracted from the experiments acc. to (20), whereas the full curve gives the calculated values acc. to [18].…”
Section: St-binding Energies Extracted From 1 S~r Excitation Datamentioning
confidence: 99%
“…Concerning the total lsa excitation cross section for ctZ > 130, a lot of experimental data are available [19,20]. From the measured lso-cross sections, D(Z) can be determined in the following way: Starting with an arbitrary value for <Ro> one calculates acc.…”
Section: Total 1so Cross Section Data For C~z> Imentioning
An analytical formula for the excitation probability of the quasimolecular l sa orbital as a function of the impact parameter b is derived for collision systems with e(Z 1 +Z2)> 1. This formula describes well all existing experimental data for those collision systems except for the heaviest system Pb + Cm (Z 1 + Z 2 = 178) at impact parameters b <40 fm. It is discussed in which way energies of the quasimolecular l so-orbital can be extracted from experimental lso-vacancy production data.
“…To determine the intensity of 72, we used the measured intensity of the other 7-ray lines in the spectra to normalize theoretical calculations [10] of nuclear Coulomb excitation [11]. Figure 4 shows the number of 7-rays from both contributing center-of-mass angles compared with theoretical predictions.…”
Projectile and target K-vacancy production probabilities in 4.6-, 5.8-and 7.3-MeV/a.m.u. U +U and U + Pb collisions are reported for impact parameters between 10 and 85 fm. These probability measurements are compared with available theory.
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