Lambda hypernuclear spectroscopy up to medium heavy mass number
at JLab Hall-C Graduate school of Science, Tohoku Univ. Toshiyuki
Gogami
Slide 2
Contents Introduction Experimental setup Analyses Missing mass
Summary
Slide 3
Contents Introduction Experimental setup Analyses Missing mass
Summary ee u u d u s s u d p K+K+ ** (e,eK + ) reaction
Slide 4
hypernuclear spectroscopy Updated from: O. Hashimoto and H.
Tamura, Prog. Part. Nucl. Phys. 57 (2006) 564. 52 V
Slide 5
Spectroscopic experiment by the (e,eK + ) reaction p n ** K+K+
e-e- e + p e + K + + target nucleus ~ 1990s The (K -, - ), ( +,K +
) reactions Energy resolution ~ a few MeV n e-Spectrometer K +
-Spectrometer p e p K+ Missing Mass M HY 2000~ The (e,eK + )
reaction Energy resolution ~0.5 MeV p
Slide 6
Experimental motivation JLab E05-115 (2009, Hall-C) Elementary
processes (, 0 ) 7 He [1], 9 Li, 10 Be N charge symmetry breaking
N-N coupling 12 B [2][3][4] Consistency check with the past
experiments Check analysis progress 52 V Single particle energy For
measurements with heavier targets [1] S.N.Nakamura et al., PRL 110,
012502 (2013) [2] T.Miyoshi et al., PRL 90, 232502 (2003) [3]
L.Yuan, PRC 73, 044607 (2006) [4] M.Iodice, PRL 99, 052501
(2007)
Slide 7
Contents Introduction Experimental setup Analyses Missing mass
Summary HES
Slide 8
Experimental setup (E05-115 @ JLab Hall-C)
Slide 9
Contents Introduction Experimental setup Analyses Missing mass
Summary
Slide 10
Analysis
Slide 11
x, x, y, y p, x, y @ Reference plane @ Target Missing Mass
Slide 12
Energy scale calibration e, K + Polyethylene target (0.45 g/cm
2 ) FWHM ~ 1.8 MeV
Slide 13
Contents Introduction Experimental setup Analyses Missing mass
Summary
Slide 14
10 Be, 12 B histograms N s ~190 ss pp FWHM~0.9 MeV N s ~530 ss
Preliminary T.Motoba et al., PTP Supplement 185 ( 2010 ) Analyses
are in progress to achieve better energy resolution with keeping
good linearity. Analyses are in progress to achieve better energy
resolution with keeping good linearity.
Slide 15
Summary and outlook JLab E05-115 (2009) , 0, 7 He, 9 Li, 10 Be,
12 B, 52 V Analyses are in progress Matrix tuning Blind analysis
Efficiencies
Slide 16
E05-115 collaboration
Slide 17
Backup
Slide 18
New challenging experiment , 0 Elementary process Energy scale
calibration 12 B Consistency check 27 Mg, 48 Sc Deformation 208 Tl
Single particle energy 1m p n ** K+K+ e-e- target nucleus
Slide 19
New challenging experiment , 0 Elementary process Energy scale
calibration 12 B Consistency check 27 Mg, 48 Sc Deformation 208 Tl
Single particle energy 4 H Charge symmetry breaking 1m p n --
target nucleus
Slide 20
New challenging experiment , 0 Elementary process Energy scale
calibration 12 B Consistency check 27 Mg, 48 Sc Deformation 208 Tl
Single particle energy Design and setup 3-D magnetic field
calculation Monte Carlo simulation Experimental operation Analyses
Energy scale calibration Tracking 1m 4 H Charge symmetry
breaking
Slide 21
Background events in the HKS z [cm] y [cm] x [cm] KDC1 KDC2
KDC1 KDC2 9 Be, 38.4 [A] REAL DATA SIMULATION e+e+ 52 Cr target
Luminosity ( 1/10 ) Worse S/N Tracking is not easy
Slide 22
Tracking efficiency and residual ~ 160 m Plane efficiency
Tracking residual ~ 350 m
Slide 23
52 Cr(e,eK + ) 52 V Preliminary N bind ~870
Slide 24
Hit wire selection REAL DATA Black : hit wires Blue : selected
wires Red : track 52 Cr Target REAL DATA CH 2 Target Compared to
the conventional code Number of K + +130% Analysis time 30%
CUT
Slide 25
JLab E05-115, Carbon (112mg/cm 2 )
Slide 26
Energy scale calibration e, K + conversion Mx M < 100
keV/c2
Slide 27
REAL DATA Black : hit wires Blue : selected wires Red : track
CH 2 Target H 2 O Target
Slide 28
52LV
Slide 29
Singles rate summary Up to ~30 [MHz] Up to ~15 [MHz] HES HKS
HKS trigger ~ 10[kHz] HES trigger ~ a few[MHz] HKS-HES
Collaboration Meeting, T.Gogami29
Slide 30
B.G. mix rate (real data) a b * hks ntulpe HKS-HES
Collaboration Meeting, T.Gogami30
Slide 31
e + simulation SIMULATION To see 1.Number of event 2.Angle
& momentum of e + generated in target To see 1.Number of event
2.Angle & momentum of e + generated in target HKS-HES
Collaboration Meeting, T.Gogami31
Slide 32
Spectroscopic experiment by the (e,eK + ) reaction p n ** K+K+
e-e- e + p e + K + + ee target nucleus Feynman diagram u u d u s s
u d p K+K+ ** ~ 1990s The (K -, - ), ( +,K + ) reactions Energy
resolution ~ a few MeV n e-Spectrometer K + -Spectrometer p e p K+
Missing Mass H HY 32 2000~ The (e,eK + ) reaction Energy resolution
~0.5 MeV p 2012/9/14JPS meeting in Kyoto, Toshi Gogami
Slide 33
Background events in the HKS z [cm] y [cm] x [cm] KDC1 KDC2
KDC1 KDC2 9 Be, 38.4 [A] REAL DATA SIMULATION ~2.24 ~4.94 e+e+ 52
Cr target Luminosity ( 1/10 ) Worse S/N Tracking is not easy
Slide 34
10 Be, 12 B histograms N s ~190 ss pp FWHM~0.9 MeV N s ~530 ss
Preliminary
Slide 35
Experimental motivation JLab E05-115 (2009, Hall-C) Elementary
processes (, 0 ) 7 He [1], 9 Li, 10 Be N charge symmetry breaking
N-N coupling 12 B Consistency check with the past experiments Check
analysis progress 52 V Single particle energy (systematic study) ls
splitting, core-configuration mixing [1] S.N.Nakamura et al., PRL
110, 012502 (2013)
Slide 36
Detectors & Trigger K + p, + e-e- Drift chambers TOF walls
(Plastic scintillators) Cherenkov detectors Aerogel (n=1.05) Water
(n=1.33) HES HKS HKS trigger (TOF1x2x3) x Chrenkov ~10 kHz HKS
trigger (TOF1x2x3) x Chrenkov ~10 kHz HES trigger (TOF1x2) ~2000
kHz HES trigger (TOF1x2) ~2000 kHz Coincidence trigger HES x HKS
< 2 kHz Coincidence trigger HES x HKS < 2 kHz
2012/10/6Core2Core in Barcelona, Toshi Gogami36
Slide 37
52 Cr(e,eK + ) 52 V Mixed event analysis s p d f
Preliminary
Slide 38
Electro-production of K + JLab E05-115 experiment by the (e,eK
+ ) reaction Small Q 2 ( ~0.01 [GeV/c] 2 ) almost real photon Real
photon 2013/3/27JPS meeting in Hiroshima, Toshi Gogami38
Slide 39
An importance of measurement of K + production at forward
angles At forward angles Data show lack of consistency We can
access K cm ~ 15 deg P.Bydzovsky and T.Mart, Phys. Rev. C 76,
065202 (2007) 2013/3/27JPS meeting in Hiroshima, Toshi Gogami39
Real photon Q 2 = 0 [ GeV/c ] 2
Slide 40
, 0 from polyethylene ( CH 2 )target JPS meeting in Hiroshima,
Toshi Gogami 2013/3/27 Preliminary 40
Cross sections 2013/3/27JPS meeting in Hiroshima, Toshi
Gogami42 SAPHIR : K.H. Glander et al., Eur. Phys. J. A 19, 251-273
(2004) CLAS : R. Bradford et al., Phys. Rev. C 73, 035202 (2006)
(*) + p K + + (*) + p K + + 0 Preliminary 200 16 91 Preliminary 85
13 34
Slide 43
Cross sections 2013/3/27JPS meeting in Hiroshima, Toshi
Gogami43 SAPHIR : K.H. Glander et al., Eur. Phys. J. A 19, 251-273
(2004) CLAS : R. Bradford et al., Phys. Rev. C 73, 035202 (2006)
JLab E94-107 : P. Markoviz et al., Proceedings of SENDAI08 (2009)
JLab E91-016 : F. Dohrmann et al., arXiv 0707.3059v2 (2007) (*) + p
K + + (*) + p K + + 0 Preliminary 200 16 91 Preliminary 85 13
34
Slide 44
Q 2 dependence (JLab E05-115) JLab E05-115, CH 2 target
Preliminary 2013/3/27JPS meeting in Hiroshima, Toshi Gogami44 W =
1.93 GeV CM = 17 degrees W = 1.93 GeV CM = 17 degrees (SAPHIR)
Slide 45
Apply to u,v-layer Applied to uu and vv layers, too. Selective
region determined by 1X and 2X Convert v v-layer x x-layer JPS
meeting in Kyoto, Toshi Gogami452012/9/14
Slide 46
Hit wires event display (2) GREEN region Selective region RED
markers & lines Selected hit wires BLACK markers & lines
Rejected hit wires v v u uu u x x v v u uu u x x KDC1 KDC2 particle
JPS meeting in Kyoto, Toshi Gogami462012/9/14
Slide 47
Detectors & Trigger K + p, + e-e- Drift chambers TOF walls
(Plastic scintillators) Cherenkov detectors Aerogel (n=1.05) Water
(n=1.33) HES HKS 2012/10/6Core2Core in Barcelona, Toshi
Gogami47
Slide 48
Detectors & Trigger K + p, + e-e- Drift chambers TOF walls
(Plastic scintillators) Cherenkov detectors Aerogel (n=1.05) Water
(n=1.33) HES HKS HKS trigger (TOF1x2x3) x Chrenkov ~10 kHz HKS
trigger (TOF1x2x3) x Chrenkov ~10 kHz HES trigger (TOF1x2) ~2000
kHz HES trigger (TOF1x2) ~2000 kHz Coincidence trigger HES x HKS
< 2 kHz Coincidence trigger HES x HKS < 2 kHz
2012/10/6Core2Core in Barcelona, Toshi Gogami48
Slide 49
Coincident K + Identification (OFF-LINE) 2012/10/6Core2Core in
Barcelona, Toshi Gogami49 Cherenkov selection Coincidence time
selection Aerogel (n=1.05) Water (n=1.33) K+K+ ++ p CUT p cut + cut
= HKS T - HES T ( e,ep ) ( e,e + ) CUT ( e,eK + ) Coincidence of
(e,eK + ) selection CUT m K 2 selection Coincident K + : ~90% ( + :
< 1%, p : < 2% )
Slide 50
10 Be, 12 B histograms N s ~190 ss pp FWHM~0.9 MeV N s ~530 ss
Preliminary