In this paper, we study the sensitivity of the fraction of ttˉ events
arising from gluon-gluon fusion to the chromoelectric and chromomagnetic dipole
moments (CEDM and CMDM) as well as the total and differential ttˉ cross
sections at the LHC and Tevatron. The sensitivity of measured charged asymmetry
at the LHC to CEDM and CMDM is also studied. We find that at the Tevatron and
the LHC, non-zero values of CMDM could suppress the ttˉ production rate.
It is shown that the ratio of σ(gg→ttˉ)/σ(ppˉ​→ttˉ) at the Tevatron is more
sensitive to CEDM and CMDM than the LHC case. The presence of CEDM always
increases the contribution of gluon-gluon fusion process in top pair rate at
the Tevatron and LHC. Except for a small range of CMDM, the presence of CEDM
and CMDM can increase the fraction of gluon-gluon fusion at the Tevatron and
LHC. The measured ratio of σ(gg→ttˉ)/σ(ppˉ​→ttˉ) at the Tevatron is used to
derive bounds on the chromoelectric and chromomagnetic dipole moments as well
as the total and differential (dσ/dmttˉ​) cross sections at the
LHC and Tevatron, and the measured charged asymmetry at the LHC. The
combination of dσTeV​/dmttˉ​ and σLHC​ provides
stringent limits on CMDM and CEDM.Comment: 11 pages,6 figures,2 table