强子物理中动量的(aQ)~νK_ν(aQ)标度分布(英文)

Scaling (aQ⊥)νKν(aQ⊥)Distribution of Momentum atS=2—1800GeV in Multihadron Physics

对固定的Ｎ在紫外固定点（β（ｇ※Ｒ）＝０），γＢ（ｇ※Ｒ）＝－０．０４５±０．０１２（－３γＢ＝αｓ，ＱＣＤ），单个发射源之内，陶标度（ａＱ⊥）νＫν（ａＱ⊥）分布成立（Ｓ＝２～１８００ＧｅＶ），这是强相互作用的非线性关联〈ｐ⊥（Ｎ）〉Ｎ／〈Ｎ〉，〈ｐ⊥（Ｍｉ）〉Ｍｉ／〈Ｍ〉与〈Ｎ（ｐ⊥）〉ｐ⊥／〈ｐ⊥〉存在的缘故．实验上适当迭代地截除动量可得枚举平均标度动量分布．Ｊ源作为整体而运动，质心系中的的罗仑兹因子为γＪ．

In the form of (aQ⊥)νKν(aQ)the mass identified hadrons (pion,kaon,protonantiproton,…)at fixed multiplicity Nch and ultraviolet fixed point (β(g※R)=0),the anomalous dimension of the nonlinear quantum fields,γB(g※R)=-0.045±0.012,-3γB(g※R)=α※s,because of the correlations,〈p⊥(N)〉-N/〈N〉,〈p⊥(Mi)〉-Mi/〈M〉 and the 〈N(p⊥)〉-p⊥/〈p⊥〉 which is the nonlinear effects of strong interactions.Mean scaling of the inclusive momentum distribution can be obtained by using the cuttechnique with iterative procedure for the nonlinear correlations.The Jsource moves as a whole with the Lorentzfactor γJ in the centreof mass system.