1. FNAL beam test simulation with Geant4.10.01 Aiwu Zhang Florida Tech 2015-01-20

2. Geant4 geometry All materials (mylar, Al drift, Cu/Ni/Au r/o, G10, FR4, Ar/CO2, etc…) are implemented. HoneyComb is replaced by 0.1mm mylar film. GEM holes are not implemented. No r/o strips. Origin is in the center. Input particle is set to be a point beam, normal incident, 20 mm in front of REF1. Physics list used is FTFP_BERT: http://geant4.cern.ch/support/proc_mod_catalog/physics_lists/hadronic/FTFP_BERT.html In which Multiple Scattering model (based on the Lewis theory) is included: http://geant4.cern.ch/G4UsersDocuments/UsersGuides/PhysicsReferenceManual/html/node34. html No resolution smearing on the detectors. The results will reflect the “intrinsic” resolutions. 2

3. What are studied at the first step: Build exclusive and inclusive residuals for: (1) four trackers (2) FITEIC, in Cartesian coordinates. Compared: [ 32GeV/c, 120GeV/c ] [pi-, proton] 20k events are simulated for each run. The plots in X coordinate will be shown in the following. (plots in Y are very similar). Both resolutions will be shown in tables. 3

4. 32GeV/c pi- position distributions REF1XREF2X REF3XREF4X FIT_EIC_X Divergence of the ‘beam’ is clear. Units in all plots are in mm. 4

5. 120GeV/c pi- position distributions REF1XREF2X REF3XREF4X FIT_EIC_X Divergence of the ‘beam’ is much smaller than the 32GeV/c case. Units in all plots are in mm. 5

6. 32GeV/c proton position distributions REF1XREF2X REF3XREF4X FIT_EIC_X Divergence of the ‘beam’ is clear and very similar to the 32GeV/c Pions. Units in all plots are in mm. 6

7. 120GeV/c proton position distributions REF1XREF2X REF3XREF4X FIT_EIC_X Divergence of the ‘beam’ is much smaller than the 32GeV/c case. Similar to the 120GeV/c pion case Units in all plots are in mm. 7

8. 32GeV/c pi- residual distributions REF1X Exclusive REF1X Inclusive Units all in um REF2X Exclusive REF2X Inclusive GeoMean: 45um GeoMean: 39um 8

9. 32GeV/c pi- residual distributions REF3X Exclusive REF3X Inclusive Units all in um REF4X Exclusive REF4X Inclusive GeoMean: 26um GeoMean: 41um 9

10. 32GeV/c pi- residual distributions for FITEIC FITEIC_X Exclusive FITEIC_X Inclusive Units all in um FITEIC_Y Exclusive FITEIC_Y Inclusive GeoMean: 56um 10

11. 120GeV/c pi- residual distributions REF1X Exclusive REF1X Inclusive Units all in um REF2X Exclusive REF2X Inclusive GeoMean: 12um GeoMean: 10um 11

12. 120GeV/c pi- residual distributions REF3X Exclusive REF3X Inclusive Units all in um REF4X Exclusive REF4X Inclusive GeoMean: 7um GeoMean: 11um 12

13. 120GeV/c pi- residual distributions for FITEIC FITEIC_X Exclusive FITEIC_X Inclusive Units all in um FITEIC_Y Exclusive FITEIC_Y Inclusive GeoMean: 15um 13

14. Comparison tables 32GeV/c pi-120GeV/c pi- ExEx_errInIn_errGMGM_errExEx_errInIn_errGMGM_err REF1X860.5230.1450.4230.160.0120.1 REF1Y870.5240.1450.4240.160.0120.1 REF2X460.3320.2390.3130.19 100.1 REF2Y470.3330.2390.3130.19 110.1 REF3X330.2200.1260.290.160.070.1 REF3Y330.2200.1260.290.160.070.1 REF4X630.4270.2410.3170.170.0110.1 REF4Y630.4280.2420.3170.170.0110.1 FITEIC_X630.4490.3560.5170.1130.1150.1 FITEIC_Y630.4500.3560.5170.1140.1150.1 32GeV/c proton120GeV/c proton REF1X870.5230.1450.4230.160.0120.1 REF1Y860.5230.1440.4230.160.0120.1 REF2X470.3330.2390.3120.19 100.1 REF2Y460.3320.2390.3130.19 100.1 REF3X330.2200.1260.290.150.070.1 REF3Y330.2200.1260.290.150.070.1 REF4X630.4280.2420.4170.170.0110.1 REF4Y620.4270.2410.3170.170.0110.1 FITEIC_X630.4500.3560.5170.1130.1150.1 FITEIC_Y620.4490.3550.5170.1130.1150.1 Units in um 14

15. Resolutions for trackers Ex_expIn_expGM_exp Ex_G4In_G4GM_G4 Corrected resolution 32GeV/c pion case REF1X1644486 2345 73 REF1Y1664587 2445 74 REF2X956679 463239 69 REF2Y976881 473339 71 REF3X825064 332026 59 REF3Y825064 332026 58 REF4X1265583 632741 72 REF4Y1185178 632842 65 Ex_expIn_expGM_exp Ex_G4In_G4GM_G4 120 GeV/c proton REF1X1343670 23612 69 REF1Y982752 23612 50 REF2X775465 12910 64 REF2Y624352 13910 51 REF3X684254 957 53 REF3Y744558 957 REF4X914161 17711 60 REF4Y934061 17711 60 15

16. Resolutions for FIT EIC chamber (zigzag) 16

17. Scattering angles Polar angle reflects the divergence of ‘beam’, ie., the scattering effect. The polar angle is also dependent on the distance between detectors. 17

18. Pi-, 32GeV/c Rho between REF2 and REF1 Pi-, 120GeV/c Rho between REF2 and REF1 Pi-, 32GeV/c Rho between REF4 and REF1 Pi-, 120GeV/c Rho between REF4 and REF1 Pi-, 32GeV/c Rho between REF4 and REF3 Pi-, 120GeV/c Rho between REF4 and REF3 Rho 18

19. Pi-, 32GeV/c theta between REF2 and REF1 Pi-, 120GeV/c theta between REF2 and REF1 Pi-, 32GeV/c theta between REF4 and REF1 Pi-, 120GeV/c theta between REF4 and REF1 Pi-, 32GeV/c theta between REF4 and REF3 Pi-, 120GeV/c theta between REF4 and REF3 Theta 19

20. Rho anglesunit in urad REF2-REF1REF4-REF1REF4-REF3 meanrmsmeanrmsmeanrms 32GeV/c pi- 34277650186107 120GeV/c pi- 91123325446 32GeV/c proton 33267651184106 120GeV/c proton 91024375554 Comparison tables Summary 20