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π0 production in dC- and dCu-interactions at a momentum of 4.5 GeV/c per nucleon

机译:在dC和dCu相互作用中以每个Gen的动量为4.5 GeV / c产生π0

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We report on measurements of neutral pion production in the inclusive reactions d + C → π0 + x and d + Cu → π0 + x at an incident momentum of 4.5 GeV/c per nucleon. The experiments were performed on the LHE 90-channel lead glass γ-spectrometer. The cross sections were measured over the kinematical region specified by the inequalities θπ ≤ 16° and Eπ ≥ 2 GeV (in the laboratory frame). The cumulative number and transverse momentum dependencies of the exponent n in the invariant cross section parameterization Ed3 σ / d3 p ~ Atn are investigated by comparing of the observed cross sections for π0 production on carbon and copper targets in the intervals 0.6 ≤ X ≤ 1.8 and 0.04 ≤ pT2 ≤ 0.40 (GeV/c)2. The double differential cross section for the reaction d + C → π0 + x is measured using statistics of about 4.5 · 104π0 mesons. On the basis of these data we verified the so-called cluster mechanism of π0 production. We have compared our data for the reaction d + C → π0 + x, extrapolated to θπ = 0°, with the data from another experiments on π? production: d + C → π?(0°) + x (P = 1.75 and 2.88 GeV/c per nucleon) [1]; p + d → π?(180°) + x and p + d → π+(180°) + x (P = 8.9 GeV/c per nucleon) [2]; d + p → π?(0°) + x (P = 8.9 GeV/c per nucleon) [3]. The invariant cross sections were approximated by an exponential function Ed3 σ / d3 p ~ exp(?X / X0). The slope parameter X0 at different kinetic energies of the projectiles in the range of 1.05÷8.0 GeV per nucleon is determined.
机译:我们报告了在包容性反应d + C→π0+ x和d + Cu→π0+ x的包容性反应中,每个核子的入射动量为4.5 GeV / c时测量中性离子的产生。实验在LHE 90通道铅玻璃γ光谱仪上进行。在不等式θπ≤16°和Eπ≥2 GeV指定的运动区域上测量横截面(在实验室框架中)。通过比较在0.6≤X≤1.8的区间内碳和铜靶上π0产生的横截面在不变截面参数化Ed3σ/ d3 p〜Atn中的指数n的累积数和横向动量依赖性。 0.04≤pT2≤0.40(GeV / c)2。反应d + C→π0+ x的双微分截面使用约4.5·104π0介子的统计量度。根据这些数据,我们验证了π0产生的所谓簇机制。我们将外推到θπ= 0°的反应d + C→π0+ x的数据与来自π?的另一个实验的数据进行了比较。生产:d + C→π?(0°)+ x(每个核子P = 1.75和2.88 GeV / c)[1]; p + d→π?(180°)+ x和p + d→π+(180°)+ x(P = 8.9 GeV / c /每个核子)[2]; d + p→π?(0°)+ x(每个核子P = 8.9 GeV / c)[3]。不变横截面由指数函数Ed3σ/ d3 p〜exp(ΔX/ X0)近似。确定在每个核子1.05÷8.0 GeV范围内的弹丸的不同动能下的斜率参数X0。

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