2012
DOI: 10.1007/s10967-011-1604-y
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Study of the isomeric ratios in photonuclear reactions of natural Selenium induced by bremsstrahlungs with end-point energies in the giant dipole resonance region

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Cited by 8 publications
(4 citation statements)
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“…A higher enhancement can be obtained by taking into account the aberration of light, even from a collimated laser. 31−33 Indeed, for a cross-sectional beam area D 2 = (0.5mm) 2 we get an intensity I = P/D 2 = 4 × 10 17 w/cm 2 and an electric field E ≃ 5 × 10 7 statvolt/cm (all the other parameters being the same). In the rest frame of the ion the power increases by a factor (1−β) −1 , as before, but the cross-sectional area D ′ 2 of the beam, decreases by a factor (1−β)/(1+β) (≃ 1/4γ 2 ), as a consequence of the "forward beaming" (aberration of light); 28 we have D ′ 2 = D 2 (1 − β)/(1 + β), which leads to an enhancement factor (1+β)/(1−β) 2 for intensity and a factor (1+β…”
Section: Introduction Accelerated Ionsmentioning
confidence: 89%
“…A higher enhancement can be obtained by taking into account the aberration of light, even from a collimated laser. 31−33 Indeed, for a cross-sectional beam area D 2 = (0.5mm) 2 we get an intensity I = P/D 2 = 4 × 10 17 w/cm 2 and an electric field E ≃ 5 × 10 7 statvolt/cm (all the other parameters being the same). In the rest frame of the ion the power increases by a factor (1−β) −1 , as before, but the cross-sectional area D ′ 2 of the beam, decreases by a factor (1−β)/(1+β) (≃ 1/4γ 2 ), as a consequence of the "forward beaming" (aberration of light); 28 we have D ′ 2 = D 2 (1 − β)/(1 + β), which leads to an enhancement factor (1+β)/(1−β) 2 for intensity and a factor (1+β…”
Section: Introduction Accelerated Ionsmentioning
confidence: 89%
“…The ratio of the probabilities of excitation of states T > and T < is described by the following relation (6):…”
Section: N − Z|mentioning
confidence: 99%
“…In [5], on bremsstrahlung, the cross section for reactions σ(γ, n) on all isotopes of natural selenium were measured up to an energy of 25 MeV. In [6], the same method was used to measure the cross sections for the reactions 78 Se(γ, n) 77m Se, 80 Se(γ, n) 79m Se, and 82 Se(γ, n) 81m Se. In [16−20], on a beam of quasi-monoenergetic photons obtained as a result of Compton backscattering, the cross sections for reactions σ(γ, n) were measured in the energy range from the threshold to 14.6 MeV on 76,77,78,80 Se isotopes.…”
Section: Introductionmentioning
confidence: 99%
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