1986
DOI: 10.1016/0375-9474(86)90526-9
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Proton threshold states in 27Si and their implications on hydrogen burning of 26Al

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Cited by 18 publications
(28 citation statements)
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“…The elements along the approximate 45 degree diagonal represent nuclei that punch through both the β1 and the proton detector. In this case, these nuclei are the beam impurities mentioned earlier, and with the exception of 25 Si and 24 Al, make up only a small fraction of the beam. As they completely pass through the proton detector, they do not interfere with the proton measurement.…”
Section: Fig 2 Top View Of the Implantation-decay Station Placed Atmentioning
confidence: 79%
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“…The elements along the approximate 45 degree diagonal represent nuclei that punch through both the β1 and the proton detector. In this case, these nuclei are the beam impurities mentioned earlier, and with the exception of 25 Si and 24 Al, make up only a small fraction of the beam. As they completely pass through the proton detector, they do not interfere with the proton measurement.…”
Section: Fig 2 Top View Of the Implantation-decay Station Placed Atmentioning
confidence: 79%
“…While this last γ-ray line corresponds energetically to a double escape peak from the 4792.3-keV γ ray, this peak was far more intense than what was expected for an escape peak. These γ rays established an IAS level energy of 6638(1) keV (verses the 6626(3) keV predicted [23,24]). The large difference in IAS energies might be due to the high density of levels and the constant α contamination observed in the previous reaction study using 28 Si( 3 He, α) 27 Si [24].…”
Section: B Gamma Studymentioning
confidence: 82%
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“…They also used the thick-target method to find the strengths of these resonances. Schmalbrock et al (1986) [26] used the 28 Si( 3 He,α) 27 Si reaction to determine the energies of 58 states from Ex = 4.14 -8.37…”
Section: Introductionmentioning
confidence: 99%