hadron physics with gev photons at spring-8/leps ii
DESCRIPTION
Contents. Introduction to SPring-8/LEPS I Physics motivation for LEPS II Status of LEPS II project Summary. Hadron physics with GeV photons at SPring-8/LEPS II . M. Niiyama (Kyoto Univ.). Super Photon Ring 8 GeV (SPring-8). Schematic V iew of LEPS I F acility. - PowerPoint PPT PresentationTRANSCRIPT
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Hadron physics with GeV photons at SPring-8/LEPS II
M. Niiyama (Kyoto Univ.)
1. Introduction to SPring-8/LEPS I2. Physics motivation for LEPS II3. Status of LEPS II project4. Summary
Contents
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Super Photon Ring 8 GeV (SPring-8)
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b) Laser hutch
a) SPring-8 SR
c) Experimental hutch
Compton g-ray
Laser light
8 GeV electron Recoil electron
Tagging counter
CollisionBackward-Compton scattering
36m70m
Schematic View of LEPS I Facility
Backward-Compton Scattered Photon 8 GeV electrons in SPring-8
+ 351nm Ar laser (3.5eV ) 8W ~ 2.4 GeV photon + 266nm Solid+BBO (4.6eV ) 1W +3.0 GeV photon
Laser Power ~6 W (351nm) Photon Flux ~1 Mcps (2.4 GeV) E measured by tagging a recoil electron E>1.5 GeV, Eg ~10
MeV Laser linear polarization 95-100% ⇒ Highly polarized g beam
PWO measurement
tagged
Linear Polarization of g beam
photon energy [GeV] photon energy [MeV] 4
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1.5
Setup of LEPS I
Acceptance is limited in forward region
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PRC 79, 025210 (2009)
Q+ LEPS vs CLAS
LEPSforwardangle
CLASlarge angle
Physics motivation for LEPS II
PRL 96, 212001(2006)
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Proton rejection by using dE/dx in Start CounterPid = (Measured energy loss in SC) – (Expectation of KK) – (Half of expectation of proton)
KKp onlyKKn and part of KKp
Proton not tagged(Proton rejected) Proton tagged (e ~60%)
K+
K-
p
n
K+
K-
p
K+
K-
or
Preliminary
Preliminary
Signal enhancement is seen in proton rejected events. should be associated with gn reaction.
p/n ratio:1.6 before proton rejection0.6 after proton rejection
SC SCSC
Peak structure is seen in theM(nK+) for proton rejected events.
(Further more data will be taken at LEPS w/ larger acceptance for proton)
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TOF
Dipole Magnet 0.7 Tesla
TargetStart Counter DC2 DC3
DC1SVTX
AC(n=1.03)
Photons
Strong angular dependence of production rate?
PRC 79, 025210 (2009)
Q+ LEPS vs CLAS
LEPSforwardangle
CLASlarge angle
Physics motivation for LEPS II
PRL 96, 212001(2006)
Angular dependence of production cross section may solve controversial situation. → 4p detector LEPS II.
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L(1405) JP=1/2-Mass spectrum of P-wave baryons
3/2-
1/2-
N(1520)
N(1535)
h+N (1485)
3/2-
1/2-
Λ(1520)
Λ(1405)30 MeV
K+N (1430)
Physics motivation for LEPS II
uud (or udd) uds
mas
s (M
eV)
Meson Baryon molecule picture has been proposed. (ex. Dalitz Phys. Rev.153 1967) 1) 3 quark or meson-baryon molecule? 2) If it is a Kbar N molecule, what is the binding energy?
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Higher mass of Kbar N component of L(1405)
D. Jido, et al. NPA725(2003)
M.Niiyama. PRC78Confirm by photoproduction.
V.K. Magas, E. Oset and A. Ramos, PRL 95
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Hyperon production with K*(892) Parity filter with linearly polarized photon
E g K*K
p
natural parity ex.P=(-1)J
K*(890),κ
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Hyperon production with K*(892) Parity filter with linearly polarized photon
E g K*K
p
unatural parity ex.P= -(-1)J
kaons
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Eg
K*K
p
p L(1405)S(1385)
K-
K*(890) Λ(1405) photoproduction with linearly polarized photon
T.Hyodo et. al, PLB593 High luminosity photon beam with Eg>2.4 GeV. Detect K*+→ K0s p+ → ppp L(1405) → S0p0 → Lg gg S(1385) → Lp0 Large acceptance charged / photon detector
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Physics motivation for LEPS IIh, w, h’ meson in nuclear medium
Detection of scattered and decay particles simaltaneously
M.Kaskulov, H. Nagahiro, S. Hirenzaki, and E. OsetPRC75,064616
Magic momentum~2.7 GeV, 0 degree
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Recoil electron (Tagging)
LEP(GeV g -ray)
Laser roomInside SR bldg
30m long line
8 GeV electron
Laser
Outside SR bldg
Experimental bldg Beam dump
Backward Compton ScatteringSR ring
Schematic view of the LEPS2 facility
10 times high intensity : Multi laser injection &Laser beam shaping
Large 4p spectrometer
Best emittance e beamÞ pencil photon beam
BGO Gamma counterTwo different exp. setup
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prism
UV lasers(355/266 nm)
expander
AR-coated mirrorw/ stepping motor
LEP intensity 107 cps for Eg<2.4 GeV beam (355 nm) 106 cps for Eg<2.9 GeV beam (266 nm) 4-laser injection [x4] Higher power CW lasers. 355 nm (for 2.4 GeV) 8 W16 W, 266 nm (for 2.9 GeV) 1 W2 W
[x2] Laser beam shaping with cylindrical expander
[x2]
10 um
400 umlaser
• Electron beam is horizontally wide. Þ BCS efficiency will be increased by elliptical laser beam.
Need large aperture of the laser injection line construct new BL chambers
High Beam Intensity
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Laser injection system
4 lasers in the laser hatch
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2011.12 SP8New experimental hatch
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2013.1.27 first beam (1.5-2.4 GeV~4Mcps w/ a single 24W laser)
Energy spectra of photon beam
w/ Laser
w/o Laser
mm
mm
Beam size in the experimental hatch
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1320 BGO crystals polar angle 24° ~ 146° ΔE=1.3% @ 1GeV
RPC-TOF wall Δt ~ 50 ps flight length 12m polar angle 0° ~ 5°
LH2, LD2 nuclear target Backward meson production from
this November.
g charged particletracker
targetg
g
BGO EGG+TOF
proton
BGO EGG
RPC-TOF
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Detector performance
π0 reconstructed with BGO-EGG.Further calibration is underway.
Time resolution of RPC-TOFRPC prototype
BGO EGG RPC prototype
1m
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Solenoid spectrometer2.22 m
g
TPC DC
g counter RPC
TOP
Magnet (BNL-E949)B=1 T p/p 〜 1-5% for q >7 degdetectors for
photon, charged particle
3σ K/p/p separation < 2.7 GeV using RPC, TOP, AC
Detector construction isunderwayPhysics run from 2015
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Summary Backward Compton g beam line for hadron physics.
Hadrons with s-quark. Recoilless production of light mesons in nucleus.
Highly polarized photon beam up to 3 GeV. x10 luminosity. ~10Mcps. Two different experimental setups.
BGO EGG + TOF Backward meson production from proton and nuclei
Solenoid spectrometer Θ+, Λ(1405)
First beam in Jan. 2013. BGO EGG experiment from this November!