π - p ω n反応を用いた ω 束縛系と質量の 同時測定実験の提案
DESCRIPTION
π - p ω n反応を用いた ω 束縛系と質量の 同時測定実験の提案. 東京大学・理・小沢恭一郎. G.E.Brown and M. Rho, PRL 66 (1991) 2720. T.Hatsuda and S. Lee, PRC 46 (1992) R34. Motivation. hadron can be undestood as excitation of QCD vacuum. Precise measurements of hadron property at nuclear medium can provide QCD information. - PowerPoint PPT PresentationTRANSCRIPT
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ππ-- pp ωω n反応を用いたn反応を用いたωω 束縛系と質量の束縛系と質量の
同時測定実験の提案同時測定実験の提案
東京大学・理・小沢恭一郎東京大学・理・小沢恭一郎
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MotivationMotivationM
ass
[GeV
]
• hadron can be undestood as excitation of QCD vacuum
Precise measurements of hadron property at nuclear medium can provide QCD information
T.Hatsuda and S. Lee,PRC 46 (1992) R34
G.E.Brown and M. Rho,PRL 66 (1991) 2720
0
**
8.0qq
mm
18.0;1mm
0
B
V
*V
Modification of vector meson mass is expected, even at nuclear density.
many experimental and theoritical efforts to search for and study in-medium modifications of hadrons
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Two approaches
– Direct measurements of mass spectra
Emitted Proton Neutronp
Nucleon Hole
Target
Decay
Meson
– Meson spectroscopy
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Mass “spectra”
F. Klingl et al. NPA 624 (1997) 527 NPA 650 (1999) 299
- meson
• Situation is not so simple, several theories and models predict spectral function of vector mesons ().– Lowering of in-medium
mass– Broadening of resonance
R. Rapp and J. Wambach, EPJA 6 (1999) 415
- meson
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Mass spectra (cont’d)
structure in spectral function due to coupling to baryon resonances
M. Lutz et al. , Nucl. Phys. A 706 (2002) 431
structure due to coupling to S11,P13 resonances
P. Muehlich et al. , Nucl. Phys. A 780 (2006) 187
To distinguish several physics processes experimentally, Measurements at exclusive condition are important.
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KEK E325, e+e-
e+e-
Cu the excess over the known hadronic sources on the low mass side of peak has been observed both in Carbon and Cupper target.
m = m0 (1 - /0) for = 0.09
CLAS claims no
The excess for both C and Cu are well reproduced by the model including the 9% mass decrease at 0.
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Positive experimental resultPositive experimental result
disadvantage:
• 0-rescattering
advantage:
• 0 large branching ratio (8 %)
• no -contribution ( 0 : 7 10-4)
p
A + X
0
2ppm
D. Trnka et al., PRL 94 (2005) 192203after background subtraction
%.mm 03
m = m0 (1 - /0) for = 0.13
TAPS, TAPS, 00 with with +A+A
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TAPS, Updated analysisTAPS, Updated analysis
after LH2 backgroundsubtraction refined analysis requiring
recoil proton and p- coplanarity
Strange Peak is seen.It exists on heavier targets.It does NOT exist in higher momentum region.
It’s still preliminary result and under investigation.
It’s gone after further analysis. Information by M. Naruki at workshop
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Missing mass spectroscopyMissing mass spectroscopy
Theoretical prediction for bound states
Energy level of bound state has information about interaction between nucleus and meson.
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Example: bound stateK. Suzuki et al., Phys. Rev. Let., 92(2004) 072302
Y. Umemoto et al., Phys. Rev. C62(2004) 024606
bound state is observed in Sn(d, 3He) pion transfer reaction.
Reduction of the chiral order parameter, f*()2/f2=0.64 at the normalnuclear density, = 0 is indicated.
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– Direct measurements of mass spectra
New experiment @ J-PARCNew experiment @ J-PARC
Simultaneous measurement!
Emitted Neutron
Nucleon Hole
Target
0 decay
Emitted Proton Neutronp
Nucleon Hole
Target
Decay
Meson
– Meson spectroscopy
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Kinematics
“Almost” stopped mesons are created.
Emitted Neutron
0 decay
-50 MeV/c2
= 0 MeV/c2
-100 MeV/c2
0 2 4 6 momentum [GeV/c2]
m
om
entu
m [
GeV
/c2]
0
0.2
0.4
0 2 4 6 momentum [GeV/c2]
0
0.8
0.4 = 0
= 5
= 10
1.2Mass dependence(M = 783 MeV/c2)
Neutron dependence
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0 degree measurement
H. Nagahiro et al, Calculation for 12C(, p)11B
Negative results for Measurements @ 15°
Li
C
O
Al
R.E. Chrien et al., Phys. Rev. Let., 60 (1988) 2595
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no distortion by pion rescattering expected in mass range of interest;
further reduced by requiring T>150 MeV
simulation
Final state interactionFinal state interaction
disadvantage:
• 0-rescattering
J.G.Messchendorp et al., Eur. Phys. J. A 11 (2001) 95
p
A + X
0
2ppm
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Beam lineBeam line
Beam Momentum ≈ 2.0 GeV/cK1.8 or High Momentum Beam line
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Spectrometer
-p n @ 2.0 GeV/c 0
Target: Carbon 1cm
Neutron DetectorFlight length 7m
Gamma DetectorBorrow from T-violation
Charged Track sweepSKS?
Beam Neutron
Gamma Detector
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Neutron DetectorNeutron Detector
Scintillation counter or Resistive Plate To achieve 30 MeV/c2 of missing mass resolution, 80 ps timing resolution is required
7 m flight path 30 MeV/c2
20 m flight path 8.9 MeV/c2
cf :proton & SKS 1.3 GeV/c 100° bending 0.17%2.0 GeV/c 36 ° bending 0.47%
missing mass resolution @ mass ~8 MeV/c2
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Gamma detector
Δ E /E = 1 %/√E
CsI EMCalorimeterBorrow from T-violation experiment
Mass resolution
Δ E /E = 3 %/√E
E/E = 2.8 % @ 200MeV (Δ E /E = 1.7 %/√E ? )( D.V. Dementyev et al., Nucl. Instrum. Meth. A440(2000), 151 )
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Yield Estimation
Summary plot of -p n for backward (G. Penner and U. Mosel, nucl-th/0111024,J. Keyne et al., Phys. Rev. D 14, 28 (1976))
0.14 mb/sr @ s = 1.8 GeV same cross section is assumed.
Beam intensity107 / spill, 3 sec spill length)
Neutron Detector acceptance = 1°(30 cm x 30 cm @ 7m
Gamma Detector acceptance75 % for single, 42% for tripleBranching Ratio: 8.9%
Optimistic obtained yield is 31650
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Summary• New experiment for exploring hadron mass
property in nuclear medium is being proposed.• K1.8 beam line can be used. High momentum
beam line is suitable.• Proposed experiment aims performing two
measurements simultaneously. The experiment seems feasible, at least not impossible.
Next tasks for proposal• Background and trigger should be considered
carefully. – Quasi free reaction– -p 0n– 2 0 4 (1 gamma missing)
• Detector R&D should be done soon.
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ThanksThanks
• R.S. Hayano (University of Tokyo)– Y. Kuroda, A. Ishida, T. Ichikawa
• K. Itahashi, H. Ohnishi, H. Outa, M. Iwasaki, T. Suzuki, F. Sakuma, S. Yokkaichi (RIKEN)
• T. Takahashi (KEK)• H. Nagahiro (RCNP)• S. Hirenzaki (Nara W University)