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本文在Ed=0.1—2.5MeV能量范围内,研究了Be9(d,p0)Be10(0),Be9(d,p1)Be10(3.368MeV),Be9(d,t0)Be8(0),Be9(d,α0)Li7(0)及Be9(d,α1)Li7(0.478MeV)诸反应。在Ed=0.150,0.220,0.401,0.706,1.005,1.301,1.484,1.750,2.000,2.250和2.500MeV共十一个能量上分别测量了这五群出射粒子在θL=10—155°区间的角分布。在θL=135°,Ed=0.1—2.5MeV,在θL=95°,Ed=0.1—2.2MeV,和在θL=112.5°,Ed=0.5—2.5MeV测量了Be9(d,p0)Be10的激发函数。在θL=135°和112.5°,Ed=1.2MeV,用较厚靶(100—300μg/cm2)测量了Be9(d,p0)Be10(0)反应的截面绝对值,结果为σ(p0)(θL=135°)=1.60mb/sr,σ(p0)(θL=112.5°)=1.55mb/sr。这样就得到了在此能区内,这五群出射粒子的截面情况。对所得结果进行了一些讨论。The reactions of Be9(d, p0)Be10(0), Be9(d, p1)Be10(3.368 MeV), Be9(d, t0)Be8(0), Be9(d, α0)Li7(0) and Be9(d, α1) Li7 (0.478 MeV) have been studied at deuteron bombarding energies from 0.1 to 2.5 MeV. The angular distributions of these five groups of outgoing particles have been measured respectively between θL = 10°and 155°at eleven bombarding energies of 0.150, 0.220, 0.401, 0.706, 1.005, 1.301, 1.484, 1.750, 2.000, 2.250 and 2.500 MeV. The excitation functions of the Be9 (d,p0) Be10 reaction have been measured at θL = 135° from Ed = 0.1 to 2.5 MeV, at θL = 95° from Ed = 0.1 to 2.2 MeV and at θL = 112.5° from Ed, = 0.5 to 2.5 MeV, respectively. By use of thicker targets (100-300μg/cm2) and at Ed = 1.2 MeV, the absolute cross sections of the Be9(d, p0)Be10 reaction were measured at θL = 135°and 112.5°; the results obtained are: σ(p0)(θL = 135°)= 1.60 mb/st and σ(p0)(θL = 112.5°)=1.55 mb/st. Thus, the behaviours of the cross sections of all these five groups of outgoing particles have been obtained in this energy range. These experimental results are discussed to some extent.
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