2006
DOI: 10.1016/j.nds.2006.07.002
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Nuclear Data Sheets for A = 51

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Cited by 40 publications
(18 citation statements)
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“…The reaction product 51 Cr decays to the first excited state in 51 V by electron capture and subsequent emission of a characteristic E γ = 320 keV photon with a half-life of T 1/2 = 27.7 d and a branching probability of 9.9 % [36]. The activity and therefore the number of produced 51 Cr nuclei was determined by counting the emitted γ-rays using a Pb-Cu shielded counting station at Notre Dame.…”
Section: Bmentioning
confidence: 99%
“…The reaction product 51 Cr decays to the first excited state in 51 V by electron capture and subsequent emission of a characteristic E γ = 320 keV photon with a half-life of T 1/2 = 27.7 d and a branching probability of 9.9 % [36]. The activity and therefore the number of produced 51 Cr nuclei was determined by counting the emitted γ-rays using a Pb-Cu shielded counting station at Notre Dame.…”
Section: Bmentioning
confidence: 99%
“…A 5 cm thick layer of 5% borated polyethylene surrounds the detector to reduce the background count rate due to neutrons coming from the outside. This detector has been used in the measurement of various ða,nÞ reactions (e.g., 17 Oða,nÞ 20 Ne [21] and 25 Mgða,nÞ 28 Si [22]) and background runs without beam were regularly performed over the course of the experiments. Typical background count rates in the shielded detector were measured to be about 20 counts=min.…”
Section: Number and Positioning Of The Countersmentioning
confidence: 99%
“…The targets were produced by evaporating a thin layer (less than 2 keV in terms of energy loss of the proton beam) of vanadium on a 0.3 mm thick tantalum backing. The reaction product, 51 Cr, decays to the first excited state in 51 V by electron capture and subsequent emission of a characteristic E g ¼ 320 keV photon (with branching probability of 9.9% [28]) with a half-life of T 1=2 ¼ 27:7 d. The activity and therefore the number of produced 51 Cr nuclei was determined by counting the g-rays emitted using a Pb-Cu shielded counting station.…”
Section: Experimental Testsmentioning
confidence: 99%
“…The T = 3/2 quartets have shown an interesting, increasing trend in the cubic IMME coefficients * dmitrii.nesterenko@jyu.fi when entering into the f 7/2 shell [9,10]. On the other hand, the quadratic IMME at A = 53 has been recently revalidated with a reduced χ 2 of 1.34, and the cubic coefficient has been found to be rather small, d = 5.4 (46) keV [11] compared to d = 39 (11) keV obtained in Ref. [12].…”
Section: Introductionmentioning
confidence: 99%