| Study
of Exclusive Dijet Production in Double Pomeron Exchange in Run II Last Update: May 19th, 2003 |
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We present results from studies of dijet events produced in Double Pomeron Exchange (DPE) in Run II. We use about 26 pb-1 of data collected with diffractive triggers during the period of September-December 2002. Results on exclusively produced dijet events in DPE trigger data are emphasized. Single diffraction (SD) in pbar-p collisions is characterized by a leading nucleon, which remains intact, and/or a ``rapidity gap'', defined as a region of pseudo-rapidity devoid of particles. In this process, a colorless object with vacuum quantum numbers, generally referred to as ``Pomeron'' (IP), is emitted by one nucleon and interacts with the other producing a cluster of particles, X: pbar + p ---> [pbar' + IP] + p ---> pbar' + X In Double Pomeron Exchange (DPE), a Pomeron
is emitted from each nucleon and a IP-IP collision
occurs producing a system X in the central rapidity region:
In Run I, we studied dijet production in DPE events using a ``Roman Pot'' (RP) inclusive trigger that tagged events with a leading antiproton in the RP detectors located along the pbar direction about 57 m downstream from the interaction region. We found that the DPE dijets have similar kinematic properties to those of the SD dijets, but the number of observed DPE events (~100) was too small for detailed studies (Run I PRL). In Run II we have obtained so far about two orders of magnitude more data. These data allow us to study DPE dijet events in detail, and in particularly to study ``exclusive dijet production in DPE'', pbar + p ---> [pbar' + IP] + [p' + IP] ---> pbar' + jet + jet + p' which has been a subject of great interest in the diffractive physics community. This interest stems from the desire to use the cross section for exclusive dijet events to calibrate calculations for diffractive Higgs production.
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Top: Bottom: |
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MP hit multiplicity versus BSC hit counter multiplicity on the pbar (p) side in the RP+Jet5 data sample is shown on the left (right). Events in the SD (ND) dominated region 0.01<xi_pbar^X<0.1
(0.3<xi_pbar^X<3.2) are shown on the top (bottom). |
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Left: Right: E_T of second to leading jet is required to be >10 GeV in all plots. |
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Invariant mass of the two leading jets with
jet energy corrections in DPE, SD and ND events. E_T of second leading jet is required to be
>10 GeV. |
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Number of events as a function of dijet mass fraction in DPE (open circle: 5.5<eta_gap<7.5, filled circle: 3.6<eta_gap<7.5) and SD (triangle) events. Dijet mass fraction is defined as dijet mass
measured in the cones of R=0.7 divided by the system mass. Error bars on the points are statistical.
Systematic uncertainty shown on the distribution
of DPE events with a gap of 3.6<eta_gap<7.5 is due to calorimeteter energy scale. E_T of second leading jet is required to be
>10 GeV. |
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Number of events as a function of dijet mass fraction in DPE events with a gap of 3.6<eta_gap<7.5. The filled (open) points show the distribution for events with leading jet E_T greater than 10 (25) GeV. E_T cut of second to leading jet is not used. |
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Calorimeter-Tower E_T in eta-phi space (LEGO) and COT-Track with calorimeter hit information. Top: Bottom: |
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Please send comments to terashi@fnal.gov |
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