000187946 001__ 187946
000187946 005__ 20210129215113.0
000187946 0247_ $$2Handle$$a2128/8434
000187946 037__ $$aFZJ-2015-01453
000187946 1001_ $$0P:(DE-Juel1)159209$$aZurek, Maria$$b0$$eCorresponding Author$$ufzj
000187946 1112_ $$aInternational Workshop on Diffraction in High-Energy Physics$$cPrimosten$$d2014-09-10 - 2014-09-17$$gDIFFRACTION 2014$$wCroatia
000187946 245__ $$aExclusive Central Meson Production in Proton Antiproton Collisions at the Tevatron at √s = 1960 GeV and 900 GeV
000187946 260__ $$c2014
000187946 3367_ $$0PUB:(DE-HGF)6$$2PUB:(DE-HGF)$$aConference Presentation$$bconf$$mconf$$s1425044481_25104$$xInvited
000187946 3367_ $$033$$2EndNote$$aConference Paper
000187946 3367_ $$2DataCite$$aOther
000187946 3367_ $$2ORCID$$aLECTURE_SPEECH
000187946 3367_ $$2DRIVER$$aconferenceObject
000187946 3367_ $$2BibTeX$$aINPROCEEDINGS
000187946 520__ $$aWe 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 $\chi_{c0}\rightarrow K^{+}K^{-}$.
000187946 536__ $$0G:(DE-HGF)POF2-899$$a899 - ohne Topic (POF2-899)$$cPOF2-899$$fPOF I$$x0
000187946 773__ $$y2014
000187946 8564_ $$uhttps://juser.fz-juelich.de/record/187946/files/FZJ-2015-01453.pdf$$yOpenAccess
000187946 8564_ $$uhttps://juser.fz-juelich.de/record/187946/files/FZJ-2015-01453.jpg?subformat=icon-144$$xicon-144$$yOpenAccess
000187946 8564_ $$uhttps://juser.fz-juelich.de/record/187946/files/FZJ-2015-01453.jpg?subformat=icon-180$$xicon-180$$yOpenAccess
000187946 8564_ $$uhttps://juser.fz-juelich.de/record/187946/files/FZJ-2015-01453.jpg?subformat=icon-640$$xicon-640$$yOpenAccess
000187946 909CO $$ooai:juser.fz-juelich.de:187946$$pVDB$$popen_access$$popenaire$$pdriver
000187946 9101_ $$0I:(DE-588b)5008462-8$$6P:(DE-Juel1)159209$$aForschungszentrum Jülich GmbH$$b0$$kFZJ
000187946 9141_ $$y2014
000187946 915__ $$0StatID:(DE-HGF)0510$$2StatID$$aOpenAccess
000187946 9132_ $$0G:(DE-HGF)POF3-899$$1G:(DE-HGF)POF3-890$$2G:(DE-HGF)POF3-800$$aDE-HGF$$bForschungsbereich Materie$$lForschungsbereich Materie$$vohne Topic$$x0
000187946 9131_ $$0G:(DE-HGF)POF2-899$$1G:(DE-HGF)POF2-890$$2G:(DE-HGF)POF2-800$$3G:(DE-HGF)POF2$$4G:(DE-HGF)POF$$aDE-HGF$$bProgrammungebundene Forschung$$lohne Programm$$vohne Topic$$x0
000187946 9201_ $$0I:(DE-Juel1)IKP-2-20111104$$kIKP-2$$lExperimentelle Hadrondynamik$$x0
000187946 980__ $$aconf
000187946 980__ $$aVDB
000187946 980__ $$aUNRESTRICTED
000187946 980__ $$aFullTexts
000187946 980__ $$aI:(DE-Juel1)IKP-2-20111104
000187946 9801_ $$aFullTexts