Cross Sections for 4He(α, X)
(Current as of 05/16/2017)

NSR Reaction Eα (MeV) Cross Section File X4 Dataset Date Added
2013DA10 4He(α, γ): deduced σ 19 - 29   X4 01/27/2016
1978HI04 4He(α, α): elastic scattering excitation function 32.6 - 35.4 θ = 30.5°, θ = 53.7°, θ = 54.7°, θ = 71.5°, θ = 90.0°   04/24/2012
1995DE18 4He(α, γ): excitation function for the decay to the 3 MeV level 33 - 34.7 θlab = 90.0°   04/24/2012
1975NA12 4He(α, γ): excitation function 33 - 36 1   07/19/2011
1977PA26 4He(α, γ): γ yeild 33.4 - 35 2+ states at 16.6 and 16.9 MeV   07/19/2011
1982SL01 4He(α, p): reaction σ 37 - 43   X4 04/18/2012
1975KI14 4He(α, p)7Li: σ for the formation of 7Li (sum of g.s. and the first excited state transitions) 38 - 140 < 50 MeV, > 50 MeV   07/19/2011
4He(α, n)7Be: σ for the formation of 7Be (sum of g.s. and the first excited state transitions) < 50 MeV, > 50 MeV
1977KI12 4He(α, p), (α n), (α d): σ 39.0 - 49.5   X4 04/16/2012
1976HI04 4He(α, α): excitation function 54.96 - 55.54 1   04/23/2012
4He(α, d): excitation function d0, d1
4He(α, p): excitation function p0, p2
1982GL01 4He(α, 2p): excitation function 60 - 160 total production of 6He   04/24/2012
4He(α, d)6Li: excitation function total production of 6Li, 6Lig.s.
4He(α, pn)6Li: excitation function 6Li
4He(α, p)7Li(g.s. + 477 keV): excitation function 1
4He(α, p)7Be(g.s. + 429 keV): excitation function 1
1978GL03 4He(α, 2p): excitation function 61.5 - 158.2 1   04/23/2012
4He(α, d)6Li: excitation function 1, total σ
4He(α, pn): excitation function 1
4He(α, p)7Li: excitation function sum of ground and first excited state
4He(α, n)7Be: excitation function sum of ground and first excited state
1981PA15 4He(α, p): excitation function at θlab = 10° 110 - 172 1   04/30/2012
4He(α, p)7Li*(4.63 MeV): excitation function at θlab = 10° 1
4He(α, d): excitation function at θlab = 10° 1
2001ME13 4He(α, p), (α n), (α d), (α np), (α 2p): σ 160, 280, 620   X4 04/18/2012
The following references may be related but not included.
1968BE02, 1978BO30, 1980BE14, 1992WU09

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Last modified: 04 October 2017