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Lambda hypernuclear spectroscopy up to
medium heavy mass number at JLab Hall-C
Graduate school of Science, Tohoku Univ.
Toshiyuki Gogami
Contents
•
•
•
•
•
Introduction
Experimental setup
Analyses
Missing mass
Summary
Contents
• Introduction
(e,e’K+) reaction
e
p
e
u
u
d
γ* u K+
–s
s
u Λ
d
Λ hypernuclear spectroscopy
52
LV
Updated from: O. Hashimoto and H. Tamura, Prog. Part. Nucl. Phys. 57 (2006) 564.
Spectroscopic experiment
by the (e,e’K+) reaction
pe’
e + p ➝ e’ + K+ + Λ
e’-Spectrometer
eγ*
p
n
Λ
target nucleus
Missing Mass MHY
K+
K+-Spectrometer
pK+
~ 1990’s
The (K-,π-) , (π+,K+) reactions
• Energy resolution ~ a few MeV
• n Λ
2000~
The (e,e’K+) reaction
• Energy resolution ~0.5 MeV
• pΛ
Experimental motivation
• JLab E05-115 (2009, Hall-C)
– Elementary processes (Λ,Σ0)
– 7ΛHe[1], 9ΛLi, 10ΛBe
• ΛN charge symmetry breaking
• ΛN-ΣN coupling
–
12 B[2][3][4]
Λ
• Consistency check with the past experiments
• Check analysis progress
–
52 V
Λ
• 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)
Contents
• Experimental setup
HES
Experimental setup
(E05-115 @ JLab Hall-C)
10 msr
∆𝑝
−4
=
2
×
10
𝑝
10 msr
∆𝑝
−4
=
2
×
10
𝑝
Contents
• Analyses
Analysis
Analysis
x, x’, y, y’
x, x’, y, y’
@ Reference plane
@ Reference plane
p, x’, y’
p, x’, y’
@ Target
Missing Mass
Energy scale calibration
e,
K+
Polyethylene target (0.45 g/cm2)
FWHM ~ 1.8 MeV
Contents
• Missing mass
10
ΛBe,
12
ΛB
histograms
FWHM~0.9 MeV
FWHM~0.9 MeV
Analyses
are in progress s
s
p
NsΛto
~190
achieve better energy resolution
NsΛ~530
with keeping good linearity.
Λ
Λ
Λ
T.Motoba et al., PTP Supplement 185 ( 2010 )
Summary and outlook
• JLab E05-115 (2009)
– Λ, Σ0, 7ΛHe, 9ΛLi, 10ΛBe, 12ΛB, 52ΛV
– Analyses are in progress
• Matrix tuning
• Blind analysis
• Efficiencies
E05-115 collaboration
Backup
New challenging experiment
1m
Λ, Σ0
 Elementary process
 Energy scale calibration
12ΛB
 Consistency check
27ΛMg, 48ΛSc
 Deformation
208ΛTl
 Single particle energy
eγ*
p
n
Λ
target nucleus
K+
New challenging experiment
1m
Λ, Σ0
 Elementary process
 Energy scale calibration
12ΛB
 Consistency check
27ΛMg, 48ΛSc
 Deformation
208ΛTl
 Single particle energy
πp
n
Λ
target nucleus
4ΛH
 Charge symmetry breaking
New challenging experiment
1m
Λ, Σ0
Design and setup
 Elementary process
 Energy scale calibration
12ΛB
 Consistency check
27ΛMg, 48ΛSc
 Deformation
208ΛTl
 Single particle energy
• 3-D magnetic field calculation
• Monte Carlo simulation
Experimental operation
Analyses
• Energy scale calibration
• Tracking
4ΛH
 Charge symmetry breaking
Background events in the HKS
REAL DATA
x [cm]
9Be
SIMULATION
, 38.4 [μA]
KDC1
KDC2
y [cm]
KDC1
KDC2
z [cm]
•
52Cr
e+
target
– Luminosity ( 1/10 )
– Worse S/N
– Tracking is not easy
Tracking efficiency and residual
σ ~ 160 μm
σ ~ 350 μm
Plane efficiency
Tracking residual
52Cr(e,e’K+)52
ΛV
Nbind~870
Hit wire selection
52Cr
REAL DATA
Target
Black : hit wires
Blue : selected wires
Red : track
CUT
REAL DATA
CUT
CH2 Target
Compared to the conventional code
 Number of K+ +130%
 Analysis time – 30%
軽い核のミッシングマス
JLab E05-115, Carbon (112mg/cm2)
数、分解能
Energy scale calibration
conversion
e, K+
Mx – MΛ < 100 keV/c2
トラッキング困難
CH2 Target
H2O Target
REAL DATA
Black : hit wires
Blue : selected wires
Red : track
REAL DATA
52LV
Singles rate summary
HKS
Up to ~30 [MHz]
HKS trigger
~ 10[kHz]
HES
Up to ~15 [MHz]
COIN ≤ 2.0 [kHz]
HES trigger
~ a few[MHz]
HKS-HES Collaboration Meeting, T.Gogami
29
B.G. mix rate (real data)
b
a
B.G mix rate =
* hks ntulpe
HKS-HES Collaboration Meeting, T.Gogami
𝑏
𝑎+𝑏
30
e+ simulation
SIMULATION
• To see
1. Number of event
2. Angle & momentum
of e+ generated in target
HKS-HES Collaboration Meeting, T.Gogami
31
Spectroscopic experiment
by the (e,e’K+) reaction
Feynman diagram
e
p
e
u
u
d
γ* u K+
–s
s
u Λ
d
e’-Spectrometer
eγ*
p
n
Λ
target nucleus
~ 1990’s
The (K-,π-) , (π+,K+) reactions
• Energy resolution ~ a few MeV
• n Λ
2012/9/14
pe’
e + p ➝ e’ + K+ + Λ
Missing Mass HHY
K+
K+-Spectrometer
pK+
2000~
The (e,e’K+) reaction
• Energy resolution ~0.5 MeV
• pΛ
JPS meeting in Kyoto , Toshi Gogami
32
Background events in the HKS
REAL DATA
x [cm]
y [cm]
9Be
, 38.4 [μA]
SIMULATION
KDC1
KDC2
KDC1
KDC2
z [cm]
e+
•
~2.24
~4.94
52Cr
target
– Luminosity ( 1/10 )
– Worse S/N
– Tracking is not easy
10
12 B histograms
Be,
Λ
Λ
FWHM~0.9 MeV
sΛ
FWHM~0.9 MeV
sΛ
pΛ
NsΛ~190
NsΛ~530
Experimental motivation
• JLab E05-115 (2009, Hall-C)
– Elementary processes (Λ,Σ0)
– 7ΛHe[1], 9ΛLi, 10ΛBe
• ΛN charge symmetry breaking
• ΛN-ΣN coupling
–
12 B
Λ
• Consistency check with the past experiments
• Check analysis progress
–
52 V
Λ
• Single particle energy (systematic なstudy)
• ls splitting, core-configuration mixing
• 将来重く行くため避けられない道
[1] S.N.Nakamura et al., PRL 110, 012502 (2013)
Detectors & Trigger
HES
K+
e-
HES trigger
(TOF1x2)
~2000 kHz
TOF walls
(Plastic scintillators)
HKS
p, π+
HKS trigger
(TOF1x2x3) x Chrenkov
Cherenkov detectors
~10 kHz
• Aerogel (n=1.05)
• Water (n=1.33)
Coincidence
trigger
Drift chambers
HES x HKS
< 2 kHz
2012/10/6
Core2Core in Barcelona, Toshi Gogami
36
52Cr(e,e’K+)52
ΛV
f
p
数
d
s
Mixed event analysis をやる
Electro-production of K+Λ
JLab E05-115 experiment
by the (e,e’K+) reaction
Small Q2 ( ~0.01 [GeV/c]2 )
 almost real photon
Real photon
2013/3/27
JPS meeting in Hiroshima , Toshi Gogami
38
An importance of measurement of
K+Λ production at forward angles
Real photon
Q2 = 0 [ GeV/c ]2
P.Bydzovsky and T.Mart, Phys. Rev. C 76, 065202 (2007)
At forward angles
2013/3/27
– Data show lack of consistency
– We can access θKcm ~ 15 deg
JPS meeting in Hiroshima , Toshi Gogami
39
Λ, Σ0 from polyethylene ( CH2 )target
2013/3/27
JPS meeting in Hiroshima , Toshi Gogami
40
Λ, Σ0 from CH2 target
JLab E05-115
CH2, ~ 450 [mg/cm2]
~ 2.0 [μA]
~ 38 [hours]
p(e,e’K+)Λ
~1.8MeV (FWHM)
Δm = 19 ± 17 keV/c2
p(e,e’K+)Σ0
~1.8MeV (FWHM)
Δm = 73 ± 47 keV/c2
2013/3/27
JPS meeting in Hiroshima , Toshi Gogami
41
Cross sections
Preliminary
85 ± 13 ±34
Preliminary
200 ± 16 ± 91
γ(*) + p  K+ + Λ
γ(*) + p  K+ + Σ0
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)
2013/3/27
JPS meeting in Hiroshima , Toshi Gogami
42
Cross sections
Preliminary
85 ± 13 ±34
Preliminary
200 ± 16 ± 91
γ(*) + p  K+ + Λ
γ(*) + p  K+ + Σ0
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)
2013/3/27
JPS meeting in Hiroshima , Toshi Gogami
43
Q2 dependence (JLab E05-115)
JLab E05-115, CH2 target
W = 1.93 GeV
θCM = 17 degrees
実光子
(SAPHIR)
2013/3/27
JPS meeting in Hiroshima , Toshi Gogami
44
Apply to u,v-layer
v v’-layer
Selective region determined by
1X and 2X
Convert
x x’-layer
2012/9/14
Applied to uu’ and vv’ layers , too.
JPS meeting in Kyoto , Toshi Gogami
45
Hit wires event display (2)
v v’
u u’
v v’
u u’
particle
particle
x x’
x x’
• GREEN region
Selective region
• RED markers & lines Selected hit wires
• BLACK markers & lines Rejected hit wires
2012/9/14
JPS meeting in Kyoto , Toshi Gogami
46
Detectors & Trigger
HES
K+
eTOF walls
(Plastic scintillators)
HKS
p, π+
Cherenkov detectors
• Aerogel (n=1.05)
• Water (n=1.33)
Drift chambers
2012/10/6
Core2Core in Barcelona, Toshi Gogami
47
Detectors & Trigger
HES
K+
e-
HES trigger
(TOF1x2)
~2000 kHz
TOF walls
(Plastic scintillators)
HKS
p, π+
HKS trigger
(TOF1x2x3) x Chrenkov
Cherenkov detectors
~10 kHz
• Aerogel (n=1.05)
• Water (n=1.33)
Coincidence
trigger
Drift chambers
HES x HKS
< 2 kHz
2012/10/6
Core2Core in Barcelona, Toshi Gogami
48
Coincident K+ Identification (OFF-LINE)
Cherenkov selection
Water (n=1.33)
Coincidence time selection
Aerogel (n=1.05)
( e,e’p )
K+ +
π
CUT
( e,e’K+ )
CUT
CUT
CUT
CUT
CUT
p
( e,e’π+ )
= HKST - HEST
p cut
π+ cut
Coincidence of (e,e’K+) selection
mK2 selection
Coincident K+ : ~90% ( π+ : < 1% , p : < 2% )
2012/10/6
Core2Core in Barcelona, Toshi Gogami
49
10
12 B histograms
Be,
Λ
Λ
FWHM~0.9 MeV
sΛ
FWHM~0.9 MeV
sΛ
pΛ
NsΛ~190
NsΛ~530