computed according to a new clustering algorithm. The jet multiplicity n is defined in such a
way that jets i and j with energies Ei and Ej at relative angle angle θij are resolved if y ij= 2
(1− cos θ ij) min (E i2, E j2) s> y cut, where s is the centre-of-mass energy squared. Using
this algorithm, large higher-order corrections at small values of ycut can easily be evaluated.
Our calculations include resummation of leading and next-to-leading logarithms of ycut to all …