Central heavy jet mass

Definition of the observable

Given a central region in rapidity ${\cal C}$, one can construct the normalised invariant masses $\rho_{U,{\cal C}}$ and $\rho_{D,{\cal C}}$ as explained in eq. (14), and then consider the maximum of the the two normalised masses:

$$\rho_{H,{\cal C}} \equiv \max\{\rho_{U,{\cal C}},\rho_{D,{\cal C}}\}\,.$$ (18)

Born event used for the analysis

The hard scale (Q) is taken to be the Born partonic center-of-mass energy.
Rapidity of the center of mass of the outgoing pair: 0.000
Cosine of the angle between outgoing jet and beam (in the partonic CM frame): 0.200

Elementary tests on the observable

Test	result
check number of jets	T
all legs positive	T
globalness	F

Since this observable is non-global, the analysis has not been continued. Since this observable is discontinuosly global, multiple emission effects have not been computed.

Collection of automatically generated results

mh_HH_cut.tar.gz collects all files produced automatically by Caesar.