Hlab meeting

22
Hlab meeting 14 Dec 2010 T.Gogami E05-115 experimental setup in JLab Hall C (2009)

description

E05-115 experimental setup in JLab Hall C (2009). Hlab meeting. 14 Dec 2010 T.Gogami. Content. e - , e + background in HKS. Drift chambers in HKS. KDC wire configuration. v ’. 150°. K +. v. x ’. 90 °. x. u’. z. 30°. y. u. x. y. x. M ultiplicity. KDC wire configuration. - PowerPoint PPT Presentation

Transcript of Hlab meeting

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Hlab meeting14 Dec 2010

T.Gogami

E05-115 experimental setup in JLab Hall C (2009)

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Content

• e- , e+ background in HKS

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KDC wire configuration

K+

zy

x

uu’xx’

vv’

30°

150°

90°

y

x

Drift chambers in HKS

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Multiplicity

Multiplicity is higher for heavy target

KDC wire configuration

K+

zy

x

uu’xx’

vv’ CH2 , 2.0 [μA]

52Cr , 7.6 [μA]

Multiplicity distributiony

x

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Number of tracks

Tracking efficiency is lower.Tracking eff. = 80% (Multiplicity = 5 )

TOP view TOP view

KDC1

Black : hit wires Blue : selected wiresRed : track

Black : hit wires Blue : selected wiresRed : track

CH2 52Cr

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Resolution

Need to optimize parameters・・・

CH2 , Ibeam = 2.0 [μA]

σ ≈ 170 [μm]

52Cr, Ibeam = 7.6 [μA]

σ ≈ 350 [μm]

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e, e+ background (Real data )

PortKDC1

KDC2

KDC1

KDC2

Extension chamber76314 , CH2

port , flange

vacuum chamber side

3000 events

20%2%

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e , e+ background in GEANT simulation

• Generated particle : e+

• Distribution : spherical uniform• Momentum : 860 – 1000 [MeV/c]• Angle : 0 – 2 [mrad]• 1000 events

Vacuum chamber(sus304)

NMR port(sus304)

KDC1 KDC2 e- , e+

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e , e+ background

• Number (rate)• Angler distribution• Momentum dist.

ELECTRON2344 [MeV]

Target

SIMULATION

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Angular and momentum distribution of e+

HKS should not accept e+ directory.

HKS detectors

HKS

D-m

agne

t

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Dirty ranking (real data)

Target Run Beam current [μA] B.G. mix rate [%]

CH2 76314 2.0 20.5

H2O 75972 2.7 44.27Li 76220 32.0 10.7

9Be 76607 38.4 14.410B 76184 42.4 9.912C 76077 38.8 19.3

52Cr 77124 7.6 58.7

rank target1 52Cr2 H2O3 CH2

4 12C5 9Be6 7Li7 10B

ab

B.G mix rate =

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Target thickness dependence(Simulation)

H2O52Cr9Be

12C CH2

10B

7Li

rank target

1 52Cr

2 H2O

3 CH2

4 12C

5 9Be

6 7Li

7 10B

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e , e+ background in GEANT simulation

Vacuum chamber(sus304)

NMR port(sus304)

KDC1 KDC2 • Generated particle : e+

• Distribution : spherical uniform• Momentum : 860 – 1000 [MeV/c]• Angle : 0 – 2 [mrad]• 1000 events

e+ make HKS dirty

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Outlook• Tracking for heavy target– Strict cut of TDC in the early stage of analysis.– Parameters for each target• Chambers• TOF counters

– Algorithm• Drift distance (time) calculation• Track fit• Need to introduce new one?

–・・・・ KDC1

KDC2

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Summary

• e- , e+ background make HKS dirty.– High rate– High multiplicity→ Tracking が大変

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END

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Target Hypernucleus Thickness[mg/cm2]

Beam Typical rateHES/HKS/COIN

[kHz]Current [μA] Total charge[C]

7Li 7He 184.0 32.0 4.84 2000 / 7 / 0.9

9Be 9Li 188.1 38.3 5.33 2400 / 9 / 1.6

10B 10Be 56.1 38.7 6.25 1300 / 1 / 0.1

12C 12B 112.5 26.8 5.90 1200 / 5 / 1.0

52Cr 52V 134.0154.0

7.6 0.835.53

2000 / 17 / 1.8

Data summary

22nd Indian-summer school (SNP2010)

Λ

Λ

Λ

Λ

Λ

E05-115 ( 2009 Aug – Nov )

Target Hypernucleus Thickness[mg/cm2]

Beam

Current[μA] Total charge[C]

CH2 Λ , Σ0 450.8 2.0 0.28

H2O Λ , Σ0 ~500.0 2.7 0.20

Physics Data

Calibration Data

(@36μA)

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KDC1 residual for 52Cr

σ ≈ 350 [μm]

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Strangeness 2010 at KEK

Tracking for high multiplicity

CH2 target

particleCH2 target

mean ~ 2 hit

52Cr target

mean ~ 6 hit

52Cr target

particle KDC1 trackingBlue : selected wiresBlack: hit wires

Multiplicity of typical layer

Multiplicity

Trac

king

eff.

52CrCH2

Developing new code

Traditional JLab Hall-C tracking code cannot handle with high multiplicity data.

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HKS detectors

Strangeness 2010 at KEK

K+

p, π+

Drift chambers-KDC1,KDC2-TOF walls -2X,1Y,1X-

(Plastic scintillators)

Cherenkov detectors -AC,WC-• Aerogel (n=1.05)• Water (n=1.33)

1 [m] June 2009 in JLab Hall-C

HKS trigger• CP = 1X ×1Y × 2X • K = WC × AC

CP × K

~18 [kHz](8 [μA] on 52Cr)

−π+

K+

p

σ ≈ 250 [μm]TOF σ ≈ 170 [ps]

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Strangeness 2010 at KEK

HES DetectorsDrift chambers- EDC1 , EDC2 -

TOF walls - EH1 , EH2 - (Plastic scintillators)

HES D magnet

HES triggerEH1 × EH2

~2 [MHz](8 [μA] on 52Cr)e

Time Of Flight

σ ~ 300 [ps]

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Target Hypernucleus Thickness[mg/cm2]

Beam Typical rateHES/HKS/COIN

[kHz]Current [μA] Total charge[C]

7Li 7He 184.0 32.0 4.84 2000 / 7 / 0.9

9Be 9Li 188.1 38.3 5.33 2400 / 9 / 1.6

10B 10Be 56.1 38.7 6.25 1300 / 1 / 0.1

12C 12B 112.5 26.8 5.90 1200 / 5 / 1.0

52Cr 52V 134.0154.0

7.6 0.835.53

2000 / 17 / 1.8

Data summary

22nd Indian-summer school (SNP2010)

Λ

Λ

Λ

Λ

Λ

E05-115 ( 2009 Aug – Nov )

Target Hypernucleus Thickness[mg/cm2]

Beam

Current[μA] Total charge[C]

CH2 Λ , Σ0 450.8 2.0 0.28

H2O Λ , Σ0 ~500.0 2.7 0.20

Physics Data

Calibration Data

(@36μA)