2009
DOI: 10.1016/j.nima.2009.02.016
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A transmission time-of-flight system for particle identification at a recoil mass separator at low energies

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Cited by 21 publications
(35 citation statements)
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“…Further evidence that the resonance strength is in the laboratory frame can be found in a contemporary paper by Tanner [10], where he states that 20 Ne (p, γ) 21 Na direct capture yield can be normalized to the yield of the E lab = 1169 keV resonance using the formula Y DC /Y R = 0.29σ ∆/ωγ, where σ is the direct capture cross section in barns. The factor of 0.29 b −1 is reproduced exactly by 2/λ 2 , where λ 2 = 7.0 b is the square of the laboratory de Broglie wavelength for an 1169 keV proton [7].…”
Section: Thomas and Tanner Resultsmentioning
confidence: 99%
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“…Further evidence that the resonance strength is in the laboratory frame can be found in a contemporary paper by Tanner [10], where he states that 20 Ne (p, γ) 21 Na direct capture yield can be normalized to the yield of the E lab = 1169 keV resonance using the formula Y DC /Y R = 0.29σ ∆/ωγ, where σ is the direct capture cross section in barns. The factor of 0.29 b −1 is reproduced exactly by 2/λ 2 , where λ 2 = 7.0 b is the square of the laboratory de Broglie wavelength for an 1169 keV proton [7].…”
Section: Thomas and Tanner Resultsmentioning
confidence: 99%
“…The strength of the E cm = 1113 keV resonance in 20 Ne (p, γ) 21 Na was recently measured using the DRAGON recoil mass spectrometer [6], part of the ISAC facility at TRI-UMF [15]. This experiment also served as commissioning of a new timestamp-based data acquisition system that will be detailed in an upcoming technical paper.…”
Section: Dragon Measurementmentioning
confidence: 99%
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