English (United Kingdom)

https://curated-unify.zendy.io/wp-json/zendy-region/v1/featured_content/oa?rat=en

https://curated-unify.zendy.io/wp-json/zendy-region/v1/highlighted_journal/

Global: Zendy Tools annual

Presents the keyphrase highlighting as premium feature

Keyphrase Highlighting

Presents the summarisation as premium feature

Summarisation

Insights

Presents the pdf analysis as premium feature

PDF Analysis

Presents the zaia usage as premium feature

ZAIA

Global: Zendy Tools monthly

Global: Zendy Plus monthly

Presents the access of premium content as premium feature

Premium Content

Global: Zendy Plus annual

Global: Zendy Free Plan

We present the calculation of the most important electroweak corrections todijet production at the LHC and the Tevatron, comprising tree-level effects ofO(\alpha_s\alpha,\alpha^2) and weak loop corrections of O(\alpha_s^2\alpha).Although negligible for integrated cross sections, these corrections can reach10-20% in the TeV range for transverse jet momenta k_T. Our detailed discussionof numerical results comprises distributions in the dijet invariant mass and inthe transverse momenta of the leading and subleading jets. We find that theweak loop corrections amount to about -12% and -10% for leading jets withk_T~3TeV at the 14TeV LHC and k_T~800GeV at the Tevatron, respectively. Theelectroweak tree-level contributions are of the same generic size and typicallypositive at the LHC and negative at the Tevatron at high energy scales.Generally the corrections to the dijet invariant mass distributions are smallerby at least a factor of two as compared to the corresponding reach in the k_Tdistributions, because unlike the k_T spectra the invariant-mass distributionsare not dominated by the Sudakov regime at high energy scales.

Weak radiative corrections to dijet production at hadron colliders