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## VI. CONCLUSIONS 

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In this paper we have presented phenomenological predictions for the production of a Higgs boson and two jets through gluon fusion. These predictions have been made possible through the implementation of recent compact analytic results for the relevant 1-loop am- plitudes [18–24]. The speed with which these amplitudes can be evaluated has enabled us to improve upon an existing semi-numerical implementation of the same process [12], with various decays of the Higgs boson now included. 

We have investigated the behaviour of the NLO cross section at the Tevatron, where contributions from this channel form part of the event sample for the latest Higgs searches [1]. 

We find that corrections to the event rate in the Higgs + ≥ 2 jet bin are modest and that the estimate of the theoretical error is reduced by approximately a factor of two compared to a LO calculation. The resulting error is still rather large, corresponding to approximately +40% and − 30% across the region of Higgs masses, 150 GeV < m$_{H}$ < 180 GeV. 

For the LHC we have provided a brief study of the behaviour of our predictions for collisions at √$_{s}$ = 10 TeV. We have also performed an analysis of this channel in the 

