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K. LaihemPrinceton meeting Princeton meeting 22-05-2006 Status Report Simulation studies E166 experiment Karim Laihem.

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Presentation on theme: "K. LaihemPrinceton meeting Princeton meeting 22-05-2006 Status Report Simulation studies E166 experiment Karim Laihem."— Presentation transcript:

1 K. LaihemPrinceton meeting Princeton meeting 22-05-2006 Status Report Simulation studies E166 experiment Karim Laihem

2 K. LaihemPrinceton meeting What we have achieved in E166 ? (e+ and photon asymmetry) Convert the X axis from current to MeV Convert the asymmetry to polarization

3 K. LaihemPrinceton meeting Updated geometry E166_Geant4_Simulation

4 K. LaihemPrinceton meeting 18” Entrance region Exit region

5 K. LaihemPrinceton meeting Spectrometer Conversion target Reconversion target 3.6” 7.78” 7.9” 9.4” solenoid Entrance region Exit region

6 K. LaihemPrinceton meeting Solenoid Axial field. The fit function is a Gaussian profile Where the coordinate z is given in centimeter. Solenoid magnetic field. (SLAC’s measurements) (1) (2) (3)

7 K. LaihemPrinceton meeting MERMAID field map implementation into E166_G4_SIM X Y Z (i,j,k) (i+1,j,k) (i,j+1,k) (i+1,j+1,k) (i,j,k+1)(i,j+1,k+1) (i+1,j,k+1) (i+1,j+1,k+1) Z X Y e+/e- Track Figure 19. Scheme of one unitary segment for the 3D interpolation. Figure 20. Scheme of the 3D segmentation using the unitary cube method for the field map implementation

8 K. LaihemPrinceton meeting I L = 0 A I L = 150 A I L = 350 A Solenoid focusing effect. e+ 2D Spatial distribution at the Entrance of the spectrometer. For different IL value (IL = 0, 150, 350 A) (Spectrometer OFF). Focusing effect of the lens is shown

9 K. LaihemPrinceton meeting I S = 120 I L = 200 I S = 160 I L = 250 e+ spatial distribution showing the density (A), at the entrance of spectrometer (B) at the exit of spectrometer (C) and at the reconversion target for different setting points IS and IL. I S = 160 I L = 250

10 K. LaihemPrinceton meeting E166_G4_SIM Figure 33. Positron energy versus spectrometer current. E e+ (180)=7.4 MeV This point can not be seen by the simulation If we use the First harmonic (E cutoff = 8.3 MeV) ? To be clarified

11 K. LaihemPrinceton meeting (E166 Zeuthen group)

12 K. LaihemPrinceton meeting E166_G4_SIM 9 Xtals

13 K. LaihemPrinceton meeting 7% -7% N = 10 4 E e+ = 3.7 MeV P e+ = 70% N = 10 4 E e+ = 3.7 MeV P e+ = 70% 300 bunches CPU time ~24h Asymmetry % = 0.43 ± 1.3 Preliminary

14 K. LaihemPrinceton meeting 100% -100% N = 10 4 E e+ = 7 MeV P e+ = 100% N = 10 4 E e+ = 7 MeV P e+ = 100% 150 bunches CPU time ~17h Asymmetry % = 13 ± 1.4 Preliminary

15 K. LaihemPrinceton meeting Positron Energy [MeV] Positron Polarization [%] Iron Polarization [%] Asymmetry [%] Analyzing power [%] 3.77070.43 ± 1.38.77 799 13 ± 1.4 13 Electron Energy [MeV] Polarization [%] Iron Polarization [%] Asymmetry [%] Analyzing power [%] 799 15 ± 1.0 15 Preliminary Preliminary Test Without Annihilation (polarization=0)

16 K. LaihemPrinceton meeting Summary Code optimization Computer power to see these small asymmetries with reasonable errors. -……… -………….. -………………. -……………………


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