HLAB MEETING ~ Status Report

HLAB MEETING
~ Status Report ~
Toshiyuki Gogami
14Jan2014
Contents
• Missing mass status
•
12C, 10B
and 7Li target
• About 7Li target
炭素標的
12C(e,e’K+)12
ΛB
12C
target
Remarks
 Efficiencies are different
between low and high
current data
 Two set of HES collimator
positions are used.
Differential cross section of
12C(γ*,K+)12
ΛB
( FWHM ~ 0.89 MeV )
Peak
-B [MeV]
Number of
event
Cross section
[nb/sr]
1
-11.40 ± 0.03
657±26
83 ±3
3
-8.37 ± 0.10
135±11
17 ±1
4
-5.15 ± 0.18
118±11
15 ±1
5
-1.67 ± 0.23
116±11
14 ±1
2
-0.38 ± 0.04
631±25
82 ±3
6
+0.82 ± 0.09
240±15
31 ±2
Only statistical errors
12
ΛB
comparison
Experiment
-BΛ [MeV]
Cross section [nb/sr]
E05-115
-11.40 ± 0.03
83 ± 3
E01-011
-11.40 ± 0.01 ± 0.04
101 ± 4.2 (+ 38 – 31)
E89-009
-11.52 ± 0.35
140 ± 17 ± 18
Emulsion
-11.37 ± 0.06
N/A
Experiment
-BΛ [MeV]
Cross section [nb/sr]
E05-115
-0.38 ± 0.04
82 ± 3
E01-011
-0.41 ± 0.01 ± 0.13
94 ± 4.0 ±35
E89-009
-0.49 ± 0.16
N/A
ホウ素標的
10B(e,e’K+)10
ΛBe
10B
target
Differential cross section of
10B(γ*,K+)10
ΛBe
( FWHM ~ 0.8 MeV )
Peak
-B [MeV]
Number of
event
Cross section
[nb/sr]
1
-8.66 ± 0.08
141±12
11.6 ±0.9
2
-7.81 ± 0.23
51±7
4.3 ±0.7
3
-6.08 ± 0.09
139±12
11.8 ±1.0
4
-5.03 ± 0.14
78±9
6.5 ±0.7
5
-1.98 ± 0.10
156±13
13.0 ±0.9
6
-0.11 ± 0.16
123±11
10.0 ±0.8
7
2.23 ± 0.07
188±14
15.9 ±1.1
8
11 .14± 0.13
94 ± 10
7.8 ±0.8
Comparison with old data
MeV
リチウム 標的
7Li(e,e’K+)7
ΛHe
7Li
target
Differential cross section of 7Li(γ*,K+)7ΛHe
( FWHM ~ 1.3 MeV )
Peak
-B [MeV]
Number of
event
Cross section
[nb/sr]
1
-5.28 ± 0.14
482±22
12.4 ±0.5
2
-3.50 ± 0.14
271±16
7.0 ±0.4
7Li
target
Remarks
 Target thickness
 ELOG
 Weight and area: 331.2 mg/cm2
 Nitride etc.?
 Thickness and density: 207 mg/cm2
• Nitriding test
• Check Brems. Rate in HES
• Etc.
Need to be done !!!!
7Li
target
Li : 0.534 g/cm3
 Li3N : 1.27 g/cm3
 LiOH : 1.46 g/cm3 (アポロ)
 Li2CO3 : 2.11 g/cm3
何かほかの
3.9 mm
0.4 ~ 0.8 mm
Li
何かほかの
0.4 ~ 0.8 mm
1.3: 0.160235 0.410859
1.4: 0.141732 0.363416
1.5: 0.12706 0.325795
2.0: 0.0837244 0.214678
Backup
52Cr(e,e’K+)52
ΛV
9Be(γ*,K+)9
ΛLi
(only figure)
Differential cross section of
10B(γ*,K+)10
ΛBe
Motoba’s calc.
( FWHM ~ 0.8 MeV )
Hiyama’s calc.
-8.84 without CSB
-8.76 with CSB
Peak
-B [MeV]
Number of
event
Cross section
[nb/sr]
1
-8.66 ± 0.08
141±12
11.6 ±0.9
2
-7.81 ± 0.23
51±7
4.3 ±0.7
3
-6.08 ± 0.09
139±12
11.8 ±1.0
4
-5.03 ± 0.14
78±9
6.5 ±0.7
5
-1.98 ± 0.10
156±13
13.0 ±0.9
6
-0.11 ± 0.16
123±11
10.0 ±0.8
7
2.23 ± 0.07
188±14
15.9 ±1.1
8
11 .14± 0.13
94 ± 10
7.8 ±0.8
7
ΛHe
comparison
( FWHM ~ 1.3 MeV )
(FWHM ~ 1.3 MeV)
Peak
-B [MeV]
Number of
event
Cross section
[nb/sr]
1
-5.28 ± 0.14
482±22
12.4 ±0.5
2
-3.50 ± 0.14
271±16
7.0 ±0.4
Hiyama’s calc.
-5.36 without CSB
-5.16 with CSB
10B
target
制動放射起因電子の計数率
Missing mass estimation
by the full-modeled Monte Carlo simulation
Achievable resolution
( FWHM, Unit: keV )
Hyperon
Target
Hypernucleus [mg/cm2]
Intrinsic Mass offset
due to energy
loss
Matrix zSimulated
dependence (B) total
resolution (A)
Achievable
resolution
(A-B)
Present work
(Toshi’s anlysis)
Λ
CH2 (450)
830
1000
730
2100
1380
1600
7
ΛHe
7Li
(184.0)
440
260
550
1300
750
1300
9
ΛLi
9Be(188.1)
440
260
170
740
560
Not yet
10
ΛBe
10B
(56.1)
430
80
40
590
550
800
12
ΛB
12C
(87.5)
430
130
80
620
540
890
52
ΛV
52Cr
430
160
30
630
600
Not yet
(134.0)
Part of the z-dependence (Λ, Σ0 and 12ΛB) is absorbed by the matrices in a matrix tuning.
 Effects of z-dependence absorption for other hypernuclei are not trivial.
 Blind analysis
Flow chart
Initial matrices
(not distorted)
Λ + B.G.
Σ0 + B.G.
12 B s-shell
Λ
Generated
Λ, Σ0 and hypernucei
Tune
Tuned matrices
Λ, Σ0 and hypernucei
Absorbing effects of
• z-dependence
• Asymmetry shape
• Etc.
Results
+
No matrix distortion
Width
ΔMM [keV]
FWHM [keV]
Mean value displacement
Λ + B.G.
Σ0 + B.G.
12 B s-shell
Λ
ΔMM < 130 keV
Achieved
simultaneously !
500 ~ 700 keV (12ΛB, 10ΛB, 52ΛV)
~ 1000 keV (7ΛHe)
Achievable
~ 1500 keV (Λ, Σ0)
resolutions
Response function