Hard color-singlet exchange in dijet events in proton-proton collisions at 13 TeV
arXiv:2102.06945 · doi:10.1103/PhysRevD.104.032009
Abstract
Events where the two leading jets are separated by a pseudorapidity interval devoid of particle activity, known as jet-gap-jet events, are studied in proton-proton collisions at 13 TeV. The signature is expected from hard color-singlet exchange. Each of the highest transverse momentum () jets must have 40 GeV and pseudorapidity 1.4 4.7, with 0, where and are the leading and subleading jets in , respectively. The analysis is based on data collected by the CMS and TOTEM experiments during a low luminosity, high- run at the CERN LHC in 2015, with an integrated luminosity of 0.66 pb. Events with a low number of charged particles with 0.2 GeV in the interval 1 between the jets are observed in excess of calculations that assume only color-exchange. The fraction of events produced via color-singlet exchange, , is measured as a function of , the pseudorapidity difference between the two leading jets, and the azimuthal angular separation between the two leading jets. The fraction has values of 0.4-1.0%. The results are compared with previous measurements and with predictions from perturbative quantum chromodynamics. In addition, the first study of jet-gap-jet events detected in association with an intact proton using a subsample of events with an integrated luminosity of 0.40 pb is presented. The intact protons are detected with the Roman pot detectors of the TOTEM experiment. The in this sample is 2.91 0.70 (stat) (syst) times larger than that for inclusive dijet production in dijets with similar kinematics.
Corrected the URL for the public results site. All the figures and tables can be found at http://cms-results.web.cern.ch/cms-results/public-results/publications/SMP-19-006 (CMS Public Pages)
References in corpus (19)
- An Introduction to PYTHIA 8.2
- Particle-flow reconstruction and global event description with the CMS detector
- The CMS trigger system
- Description and performance of track and primary-vertex reconstruction with the CMS tracker
- Jet energy scale and resolution in the CMS experiment in pp collisions at 8 TeV
- Exclusive J/ photoproduction off protons in ultra-peripheral p-Pb collisions at TeV
- BFKL evolution and the growth with energy of exclusive J/Psi and Upsilon photo-production cross-sections
- Measurements of jet vetoes and azimuthal decorrelations in dijet events produced in collisions at = 7 TeV using the ATLAS detector
- Measurement of the inclusive jet cross-sections in proton--proton collisions at 8 TeV with the ATLAS detector
- Ratios of dijet production cross sections as a function of the absolute difference in rapidity between jets in proton-proton collisions at sqrt(s) = 7 TeV
- Gaps between jets in hadronic collisions
- The next-to-leading order vertex for a forward jet plus a rapidity gap at high energies
- The quark induced Mueller-Tang jet impact factor at next-to-leading order
- The Gluon-Induced Mueller-Tang Jet Impact Factor at Next-to-Leading Order
- Diffractive Dijet Production in Antiproton-Proton Collisions at =1.96 TeV
- Gaps between jets at hadron colliders in the next-to-leading BFKL framework
- LHC Optics Measurement with Proton Tracks Detected by the Roman Pots of the TOTEM Experiment
- Hard color singlet BFKL exchange and gaps between jets at the LHC
- Measurement of single-diffractive dijet production in proton-proton collisions at 8 TeV with the CMS and TOTEM experiments
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- Physics perspectives of a CMS near-beam proton spectrometer at the HL-LHC
- Dijets with a large rapidity separation in the next-to-leading order BFKL formalism for searches of large extra dimensions at colliders