Home > Publications database > Exclusive Central Meson Production in Proton Antiproton Collisions at the Tevatron at √s = 1960 GeV and 900 GeV > print |
001 | 187946 | ||
005 | 20210129215113.0 | ||
024 | 7 | _ | |2 Handle |a 2128/8434 |
037 | _ | _ | |a FZJ-2015-01453 |
100 | 1 | _ | |0 P:(DE-Juel1)159209 |a Zurek, Maria |b 0 |e Corresponding Author |u fzj |
111 | 2 | _ | |a International Workshop on Diffraction in High-Energy Physics |c Primosten |d 2014-09-10 - 2014-09-17 |g DIFFRACTION 2014 |w Croatia |
245 | _ | _ | |a Exclusive Central Meson Production in Proton Antiproton Collisions at the Tevatron at √s = 1960 GeV and 900 GeV |
260 | _ | _ | |c 2014 |
336 | 7 | _ | |0 PUB:(DE-HGF)6 |2 PUB:(DE-HGF) |a Conference Presentation |b conf |m conf |s 1425044481_25104 |x Invited |
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520 | _ | _ | |a We have measured exclusive $\pi^{+}\pi^{-}$ production in proton-antiproton collisions at $\sqrt{s}=$0.9 and1.96 TeV in the Collider Detector at Fermilab. We selected events with exactly two oppositely chargedparticles in $|\eta|<1.3$, with no other particles detected in $|\eta|<5.9$. The central $\pi^{+}\pi^{-}$ wasrequired to have rapidity $|y|<1$. By requiring no other charged particles, these events are dominated bydouble pomeron exchange, which constrains the quantum numbers of the central state. The data showresonance structures attributed to the $f_0$ and $f_2$ mesons. We place upper limits on exclusive$\chi_{c0}\rightarrow\pi^{+}\pi^{-}$ and $\chi_{c0}\rightarrow K^{+}K^{-}$. |
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773 | _ | _ | |y 2014 |
856 | 4 | _ | |u https://juser.fz-juelich.de/record/187946/files/FZJ-2015-01453.pdf |y OpenAccess |
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