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Measurement of proton induced pion pair production in nuclei. Tetsuro Itabashi (Osaka University). Introduction. QCD and spontaneous breaking of Chiral Symmetry quarks & qluons ⇒ hadrons at low energy Quark and anti-quark pair condensation <qq>=0 ⇒ <qq>≠0 hadrons have effective mass
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Measurement of proton induced pion pair production in nuclei Tetsuro Itabashi(Osaka University)
Introduction QCD and spontaneous breaking of Chiral Symmetry • quarks & qluons ⇒ hadrons at low energy • Quark and anti-quark pair condensation • <qq>=0 ⇒ <qq>≠0 • hadrons have effective mass • M∝fπ, fπ2mπ2~m<qq> • Generate pion as Nambu-Goldstone boson • Light pion mass
Introduction How to confirm it experimentally • Phase transition at high energy : <qq>0 • New phase of matter – QGP • Heavy ion collider RHIC, LHC • Partial restoration in nuclear medium • Meson mass shift in nuclear medium ρ/ω/φ(KEK E325) σ(CHAOS,TAPS) quark condensate
σmeson ( f0(600) or σ : I,Jp=0,0+ ) • Chiral partner of pion • Change of spectral function at finite nuclear density • Enhancement at just above 2mπthreshold region • Mππdistribution Φ=1-Cρ/ρ0 ω(GeV) T. Hatsuda, T. Kunihiro, H. Shimizu, PRL 82. 2840. (1999)
CHAOS • π+A→π+π-A’ reaction • heavier nuclear target, remarkable enhancement only in sigma channel Crystal ball • π-+A π0+π0+X • No sharp peak
TAPS • γA→π0π0A’ reaction • RPb/C has mass shift to lower Invariant mass region Elementary process seems to be simple Still not conclusive new type of experiments are desirable
Our Experiment p+A→π+ +π- +X reaction • Ring Cyclotron of RCNP @ Osaka university. • Tp~420MeV • Proton beam Elementary process may be simple • Subthreshold beam energy Tthre(pN) = 600MeV for elementary process • influence from secondary process is small • Mass number dependence of Mπ+π- CERSIUS PRL 88 (2002) 192301
Subthreshold 2π production with beam energy Tp=416MeV • invariant mass region : 2mπ to 350 MeV/c2 Enough to see around threshold region ( observed in Mπ+π- <300MeV/c2 ) • cross section ~1nb/nucleon simple calculation using • elementary pp→π+π-pp cross section data • Fermi motion distribution of nuclei • nucleon binding in nuclei
solenoidal magnet (3kG) • opening angle • θ : 15º-105º • φ : 2π • Cylindrical Drift Chamber (CDC) • ⇒ Momentum • Inner Hodoscopes • Outer Hodoscopes • ⇒ Trigger,TOF • acceptance for 2π event ~ 0.6 Experimental set up side view
photo You can see solenoidal magnet and CDC
Trigger system • σππis very small compared to proton scattering • efficient trigger system is needed proton scattering : σ~ a few 10mb pn→ppπ- : σ~ 50μb pN→pNπ+π- : σ~ 1nb negative charge trigger is quite useful for rare π+π- ~10 -3
π- trigger --Design ≧3 Tilted counters with magnetic field distinguish charge by # of hit negative particle : ≧ 3 hits positive particle : ≦ 2 hits Requiring 3 adjacent hits ⇒ π- trigger ≦2 front view
photo Hodoscopes before installing CDC
Efficiency of 3-coin. Efficiency of π- trigger • Determined by geometry • optimized for π- from subthreshold 2π production pT distribution of π
Test experiment • Trigger performance test • Search for π+π- events • Proton beam energy : 392MeV • Beam current : ~0.2nA • Target : Cu 50μm
π‐ trigger performance Inclusive trigger innerOR×outerOR π- trigger innerOR×outer 3 coin. p p π- π- ~2.1%
preliminary result Search for π+ π - like pairs One π- and another h+ 8 hours run(2.7h live time) Sensitivity down to ~0.1nb/nucleon Low statistics
Improvement for π+ detection Additional new counters • To catch some π+ which escapes through gaps of counters • Separate p and π+ well in PID geometry is simple for determining flight length, dE/dx etc.
Test experiment II To check performance of new counters, a part of counters were placed flatly • proton beam energy : 392MeV • Beam current : ~ 0.1 nA • Target : Cu 50μm
Particle ID by flat counter preliminary Protons are dominant but π+locus clearly seen We can distinguish π+events from proton well π+ p p π+
Outlook Further trigger improvement for high statistics • Combination of outer & inner hodoscopes • Combination of outer & CDC wire hit require 2-cluster of them 2-track event/all~1/10 Trigger logic w/ ULM (FPGA base)
4 days experiment with one target is approved • Establish p+p- measurement • Present yield is too few • Discuss p+p- production more clearly • Mpp, ppp and qpp distributions • First step to measure A-dependence • At least 2 more targets
Summary • Medium modification of π+π- pair in sigma channel is still not conclusive • We are preparing another experiment, proton induced subthreshold pion pair production in nuclei • large acceptance detector and effective π- trigger • π+π- like events are seen, but low statistics • With additional detectors and improved trigger system, we will perform 4-day experiment soon.
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