Zhihong Ye Hampton University Feb. 16 th 2010, APS Meeting, Washington DC Data Analysis Strategy to Obtain High Precision Missing Mass Spectra For E05-115.

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Presentation transcript:

Zhihong Ye Hampton University Feb. 16 th 2010, APS Meeting, Washington DC Data Analysis Strategy to Obtain High Precision Missing Mass Spectra For E Experiment Spectroscopic investigation of Lambda hypernuclei in the wide mass region using the (e,e’K+) reaction (HKS-HES Collaboration)

OutlineOutline  Detector Calibration: Tracking, Timing, Particle Identification  Optics Calibration: Splitter, HKS, HES (Angle, Momentum, Time)  Kinematics Calibration: Beam energy offset, target effect, center momentum and center angle deviation.  Flow Chart  Current Status

Detectors Calibration  Tracking: --- Focal Plan Info  HKS : Two identical Wire Chambers Resolution: Position : x, y ~ cm, Angle : x ’, y ’ ~ 0.3 mrad  HES: Honeycomb Chamber + Wire Chamber Resolution: Position : x ~ cm, y ~ cm, Angle : x ’ ~ 0.5 mrad, y ’ ~ 0.9 mrad  Timing: -- Trigger, TOF HKS Hodoscopes: 1 X (17)+1 Y (9)+2 X (18) HES Hodoscopes: 1 X (25)+2 X (25) Time Correction: Pulse High Correction, Alignment, Offsets. Resolution: Single PMT ~ 110 ps,  ~ K1X(17) K1Y (9) K2X(18) 15.9 cm cm E1X (25) E2X(25) 30.0 cm KDC1(6)KDC2(6) cm EDC1(10)EDC2(6) ~30.0 cm K+ e’ K+ e’

 Particle ID:  Online Trigger: !(AC1+AC2+AC3) & (WC1+WC2) AC (  + < 99%), WC (p + < 99%),  Offline KID: Cuts on number of photon electrons (NPE) Optimize Cutting values – More Kaon, less Pion & Proton HKS X Kaon Beta WC NPEAC NPE  =0.027

Optics Calibration Splitter HKS / HES K + /e’ Beam  Optics:

Optics Calibration  Reconstruction: Angle: Splitter HKS / HES K + /e’ Beam  Optics: Momentum: Target Time:

Optics Calibration  Reconstruction: Angle: Splitter HKS / HES K + /e’ Beam  Optics:  Matrices: Optimized using  &  Spectra. Optimized using Sieve Slit data. Optimized using  &  Spectra. Path length correction using RF time. Momentum: Target Time: Generated from Geant4 simulation

CoincidentCoincident t 2 ns Electron pulse  RF Structure: Jlab electron beam has a 2ns pulse pattern. RF vs HES XRF vs HKS X After Path length correction

CoincidentCoincident t 2 ns Electron pulse  RF Structure: Jlab electron beam has a 2ns pulse pattern. RF vs HES XRF vs HKS X 2ns After Path length correction

CoincidentCoincident t 2 ns Electron pulse  RF Structure: Jlab electron beam has a 2ns pulse pattern. Real Events Accidental RF vs HES XRF vs HKS X  Coincident Time: 2ns After Path length correction Select coincident Kaon and electron events:

Kinematics Calibration E beam = GeV±0.01%; P k0 = 1.2GeV/c ± 12.5%; P e0 = GeV/c ±17%;  Missing Mass:

 Target effect: Due to Bremsstrahlung, Ionization, Multi-Scattering and so on.. Using SIMC (Hall-C standard Monte-Carlo simulation package), for different targets and thickness, we have: Kinematics Calibration E beam = GeV±0.01%; P k0 = 1.2GeV/c ± 12.5%; P e0 = GeV/c ±17%;  Missing Mass:

 Target effect: Due to Bremsstrahlung, Ionization, Multi-Scattering and so on.. Using SIMC (Hall-C standard Monte-Carlo simulation package), for different targets and thickness, we have: Kinematics Calibration  Beam Energy Offset: Two energy scan run: E = E beam ± 1.0 MeV, we have the correction function: E beam = GeV±0.01%; P k0 = 1.2GeV/c ± 12.5%; P e0 = GeV/c ±17%;  Missing Mass:

 Central Momentum & Angle Offsets:  Central Momentum:  Central Angle: Magnet field setting, Installation, and Coordinate definition…

 Central Momentum & Angle Offsets:  Central Momentum:  Central Angle: Magnet field setting, Installation, and Coordinate definition… Using the well-known  &  masses, define Chi-Square: And set  X’ k0,  Y’ k0,  P k0,  X’ e0,  Y’ e0,  P e0 as parameters, we can fit  &  data to minimize the Chi-Square, and obtain offset values:

 Central Momentum & Angle Offsets:  Central Momentum:  Central Angle: Magnet field setting, Installation, and Coordinate definition… Using the well-known  &  masses, define Chi-Square: And set  X’ k0,  Y’ k0,  P k0,  X’ e0,  Y’ e0,  P e0 as parameters, we can fit  &  data to minimize the Chi-Square, and obtain offset values: Missing Mass:

Flow Chart Tracking (KDC) Tracking (KDC) TOF (Hodoscopes) TOF (Hodoscopes) KID (AC,WC,LC) KID (AC,WC,LC) HKS Focal Plane (X,X’,Y,Y’,T fp ) HKS Focal Plane (X,X’,Y,Y’,T fp ) HKS Optics (HKS+Splitter) Optics (HKS+Splitter) HKS Target Plane (X’, Y’, P, T tar ) HKS Target Plane (X’, Y’, P, T tar ) Tracking (EDC) Tracking (EDC) TOF (Hodoscopes) TOF (Hodoscopes) HES Focal Plane (X,X’,Y,Y’, T fp ) HES Focal Plane (X,X’,Y,Y’, T fp ) HES Optics (HES+Splitter) Optics (HES+Splitter) HES Target Plane (X’, Y’, P, T tar ) HES Target Plane (X’, Y’, P, T tar ) Coincident (RF ) Coincident (RF ) Kinematics Correction (Beam, Target effects, Momentum, Angular) Kinematics Correction (Beam, Target effects, Momentum, Angular) Missing Mass Raw Data Need to do Data & Info Lambda&Sigma Spectra Lambda&Sigma Spectra Geant4 Simulation HKS Sieve Slit HES Sieve Slit

Current Status & Plan o We are currently working on precise calibration of all detectors. To Do: o Tracking: Solve HES y’ problem. o Timing: Improve timing and TOF resolution. o PID: Standardize AC, WC cutting values for different targets. o Optics: Optimizing matrices using Sieve Slit data o Kinematics: Improving minimization method.  ~1 MeV   P Shell? G.S? Need a lot of work to reach 350 KeV! Very Preliminary Thank you!