HLab meeting

19
HLab meeting 10/14/08 K. Shirotori

description

HLab meeting. 10/14/08 K. Shirotori. Contents. SksMinus status SKS magnet trouble Magnetic field study. Introduction. Hypernuclear production via the (K - , p - ) and ( p + ,K + ) reaction ⇒Scattered p - and K + are analyzed by the magnetic spectrometer, using SKS. Analysis method - PowerPoint PPT Presentation

Transcript of HLab meeting

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HLab meeting

10/14/08

K. Shirotori

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Contents

• SksMinus status– SKS magnet trouble– Magnetic field study

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IntroductionHypernuclear production via the (K-,-) and (+,K+) reaction

⇒Scattered - and K+ are analyzed by the magnetic spectrometer, using SKS.

Analysis method : Runge-Kutta calculation from the position of drift chambers and the precisely measured magnetic field map

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SKS magnet problem

One of the SKS magnet coil was broken by the high voltage test.

(It cannot be repaired… )

Effects to experiments• Strength of filed : 5/6 (2.7

T 2.5 T @ 395A)⇒⇒Decreasing acceptance and

momentum resolution• Change of filed shape⇒Tracking and absolute

momentum valueThe innermost part of the coil

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StudyCalculated field maps are compared with the measured map.

Simulation• Scattered particles tracks generated with

calculated maps (as a true magnetic filed) are analyzed by the measured map or calculated map.

Real data analysis• Real experimental data (KEK E566 data) are

analyzed by calculated maps.

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Simulation

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Simulated conditions

Particles generation in the simulation• - of 1.4 GeV/c with uniform scattering

angular distribution up to 20 degree • No multiple scattering

Analysis of simulated data• Tracking by using the hit positions of

drift chamber• Drift chamber resolution ~400 m

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Magnetic field map

sksmap395a.dat (measured,) Measured 395A magnetic field map

SksQM4S395AFullC.dat (QM4F) Calculated field map Full coil version

SksQM5S395AFullC.dat (QM5F) Calculated field map Full coil version Different B-H curve from QM4F

QM4 Fis used as generated map in the simulation.

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Field map and particle tracks

Particles pass the incomplete magnetic filed map region, but they are rejected and there are no large effects.

Measured

Calculated(QM4)

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Meaning of observables

P : Momentum U0 : angel (dx/dz) of

production point V0 : angle (dy/dz) of

production point

(x,y,z belong local coordinate)

z

x

● y

Local coordinate (In)zx

y

Local coordinate (Out)

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Calculated(QM4F) measured : U0,V0⇒QM4F→QM4F QM4F→measured

Large difference P vs U0, 2nd polynomial shape P vs V0, tracks near the SKS magnet coil gap

Momentum resolution : 1.7 MeV/c 2.4 MeV/c (to select good region)⇒ Tracking 2~1.6 (1.0 original)

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Calculated(QM4F) calculated(QM5F) : U0,V0⇒QM4F→QM4F QM4F→QM5F

Large difference P vs U0, little 2nd polynomial shape P vs V0, almost flat

Momentum resolution : 1.7 MeV/c 2.3 MeV/c (no correction)⇒ Tracking 2~1.0 (1.0 original)

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QM4F→Measured : P vs U0

Particles passing the circled region have large difference between measured andcalculated map.

Measured

QM4F

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Analysis

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Analysis method

To analyze E566 data : (+,K+) reaction data Correlation by measured map (sksmap272a.d

at) Correlation by calculated map Target thickness : 12C (3.4 g/cm2)(Resolution is determined by the target)

To checkMissing mass (binding energy) vs u0Missing mass (binding energy) vs v0

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Measured map (sksmap272a.dat)Before correction After correction

U0 vs MM : 1st+2nd polynomial correlation V0 vs MM : 2nd polynomial correlation⇒Momentum resolution : 2.8 MeV (After correction)

Correction coefficientsU : -0.012*U-0.01*U2

V : +0.05*V2

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Calculated map (SksQM12S272AFull.dat)

Correction coefficientsU : -0.012*U-0.01*U2

V : +0.05*V2

U0 vs MM : 1st+2nd polynomial correlation V0 vs MM : 2nd polynomial correlation⇒Momentum resolution : 3.1 MeV (After correction)Binding energy offset : -4 MeV

Before correction After correction

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Correlation shape

U0 vs MM : 1st+2nd polynomial correlation

V0 vs MM : 2nd polynomial correlation

Correlation shapes are almost same between all maps. BE vs u0(dx/dz) : strong 1st+2nd polynomial correlation (The

correlation becomes larger to the inner tracks.) BE vs v0(dy/dz) : small 2nd polynomial correlation Offset : less than 10 MeV (Absolute value of magnetic field : ±1%)

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SummaryStudy Simulation

Generated by calculated map Analyzed by measured or ⇒calculated map

Check the correlation between momentum and scattering angle⇒To check the difference of absolute values and angles

Real data analysis @ 272A map E566 thin 12C target data analyzed by measured or calculated map Check the correlation between binding energy and scattering

angle ⇒ Correlation shapes are almost same between all maps. ⇒ The correlation can be corrected.

For the experiments High resolution experiments

To correct the correlation by many binding energy data How to determine the absolute value ?

Coincidence experiment (Hypernuclear -ray spectroscopy, weak decay)

The correction is almost enough to select the binding state. (Momentum resolution is not need to be so high)