Fragmentation Function and Hadronic Production of the Heavy Supersymmetric Hadrons

The light top-squark $\text{sto}$ may be the lightest squark and its lifetime may be long enough' in a kind of SUSY models which have not been ruled out yet experimentally, so colorless supersymmetric hadrons (superhadrons)’ $(\sto \bar{q})$($q$isaquarkexcept$t$-quark) may be formed as long as the light top-squark $\text{sto}$ can be produced. Fragmentation function of $\text{sto}$ to heavy supersymmetric hadrons (superhadrons)' $(\sto \bar{Q})$ ($\bar{Q}=\bar{c}$ or $\bar{b}$) and the hadronic production of the superhadrons are investigated quantitatively. The fragmentation function is calculated precisely. Due to the difference in spin of the SUSY component, the asymptotic behavior of the fragmentation function is different from those of the existent ones. The fragmentation function is also applied to compute the production of heavy superhadrons at hadronic colliders Tevatron and LHC under the so-called fragmentation approach. The resultant cross-section for the heavy superhadrons is too small to observe at Tevatron, but great enough at LHC, even when all the relevant parameters in the SUSY models are taken within the favored region for the heavy superhadrons. The production of light superhadrons’ $(\text{sto}\bar{q})$ ($q=u,d,s$) is also roughly estimated. It is pointed out that the production cross-sections of the light superhadrons $(\text{sto}\bar{q})$ may be much greater than those of the heavy superhadrons, so that even at Tevatron the light superhadrons may be produced in great quantities.