002834120 001__ 2834120
002834120 003__ SzGeCERN
002834120 005__ 20220922201954.0
002834120 0247_ $$2DOI$$9Springer$$a10.1007/s10751-019-1565-z
002834120 0248_ $$aoai:cds.cern.ch:2834120$$pcerncds:CERN
002834120 035__ $$9https://inspirehep.net/api/oai2d$$aoai:inspirehep.net:1725605$$d2022-09-21T14:27:07Z$$h2022-09-22T04:00:07Z$$mmarcxml
002834120 035__ $$9Inspire$$a1725605
002834120 041__ $$aeng
002834120 084__ $$2PACS$$a24.70.+s
002834120 100__ $$aGrzonka, D$$jORCID:0000-0001-6172-3841$$tGRID:grid.8385.6$$uJulich, Forschungszentrum
002834120 245__ $$9Springer$$aSearch for polarized antiproton production
002834120 260__ $$c2019
002834120 300__ $$a8 p
002834120 520__ $$9Springer$$aThe production of antiprotons is studied in view of possible polarization effects as basis for a polarized antiproton beam. If antiprotons are produced with some polarization, a quite simple procedure for the generation of a polarized antiproton beam could be worked out. The experiments are performed at the CERN PS test beam T11 where secondary particles with momenta around 3.5 GeV/c are selected. The polarization analysis is performed by measuring the asymmetry of the elastic $\bar {p} p$ -scattering in the Coulomb-nuclear interference region. The detection system includes Cherenkov and tracking detectors for the particle identification and the 3d track reconstruction. Details on the detection system and the status of the analysis are given.
002834120 542__ $$dSpringer Nature Switzerland AG$$g2019
002834120 65017 $$2SzGeCERN$$aNuclear Physics - Experiment
002834120 6531_ $$9author$$aPolarized antiproton
002834120 6531_ $$9author$$aCNI
002834120 6531_ $$9author$$aElastic scattering
002834120 6531_ $$9author$$aDIRC
002834120 6531_ $$9author$$aDrift chamber
002834120 6531_ $$9author$$aTrack reconstruction
002834120 690C_ $$aARTICLE
002834120 690C_ $$aCERN
002834120 700__ $$aAlfs, D$$tGRID:grid.8385.6$$tGRID:grid.5522.0$$uJulich, Forschungszentrum$$uJagiellonian U.$$vM. Smoluchowski Institute of Physics - Jagiellonian U. - Krakow - Poland
002834120 700__ $$aAsaturyan, A$$uNAS Armenia, Yerevan
002834120 700__ $$aCarmignotto, M$$tGRID:grid.39936.36$$uCatholic U.
002834120 700__ $$aDiermaier, M$$tGRID:grid.475784.d$$uStefan Meyer Inst. Subatomare Phys.
002834120 700__ $$aEyrich, W$$tGRID:grid.5330.5$$uErlangen - Nuremberg U.
002834120 700__ $$aGłowacz, B$$tGRID:grid.5522.0$$uJagiellonian U.
002834120 700__ $$aHauenstein, F$$tGRID:grid.261368.8$$uOld Dominion U.
002834120 700__ $$aHorn, T$$tGRID:grid.39936.36$$uCatholic U.
002834120 700__ $$aKilian, K$$tGRID:grid.8385.6$$uJulich, Forschungszentrum
002834120 700__ $$aLersch, D$$tGRID:grid.8385.6$$uJulich, Forschungszentrum
002834120 700__ $$aMalbrunot-Ettenauer, S$$tGRID:grid.9132.9$$uCERN
002834120 700__ $$aMkrtchyan, A$$uNAS Armenia, Yerevan
002834120 700__ $$aMkrtchyan, H$$uNAS Armenia, Yerevan
002834120 700__ $$aMoskal, P$$tGRID:grid.5522.0$$uJagiellonian U.
002834120 700__ $$aNadel-Turonski, P$$tGRID:grid.450315.6$$uJefferson Lab
002834120 700__ $$aOelert, W$$tGRID:grid.5802.f$$uMainz U.
002834120 700__ $$aRitman, J$$tGRID:grid.8385.6$$uJulich, Forschungszentrum
002834120 700__ $$aSefzick, T$$tGRID:grid.8385.6$$uJulich, Forschungszentrum
002834120 700__ $$aTadevosyan, V$$uNAS Armenia, Yerevan
002834120 700__ $$aWidmann, E$$tGRID:grid.475784.d$$uStefan Meyer Inst. Subatomare Phys.
002834120 700__ $$aWolke, M$$tGRID:grid.8993.b$$uUppsala U.
002834120 700__ $$aZhamkochyan, S$$uNAS Armenia, Yerevan
002834120 700__ $$aZieliński, M$$tGRID:grid.5522.0$$uJagiellonian U.
002834120 700__ $$aZink, A$$uErlangen - Nuremberg U., ECAP
002834120 700__ $$aZmeskal, J$$tGRID:grid.475784.d$$uStefan Meyer Inst. Subatomare Phys.
002834120 773__ $$01695299$$c22$$n1$$pHyperfine Interact.$$v240$$wC18-03-12.1$$y2019
002834120 960__ $$a13
002834120 962__ $$b2683660$$k22$$nparis20180312
002834120 980__ $$aARTICLE
002834120 980__ $$aConferencePaper