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Status of the Simulations on Photo Injector Optimization for Low Charges Yauhen Kot BD Meeting, 01.02.2010.

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Presentation on theme: "Status of the Simulations on Photo Injector Optimization for Low Charges Yauhen Kot BD Meeting, 01.02.2010."— Presentation transcript:

1 Status of the Simulations on Photo Injector Optimization for Low Charges Yauhen Kot BD Meeting, 01.02.2010

2 Preliminary results work is not accomplished yet…

3 Optimization Code for the Photo Injector by M. Krasilnikov

4 BoosterACC13,9GHz Gun FLASH Photo Injector Booster phase is fixed Same gradient at booster and ACC1

5 + Bucking coil peak field E z1 (z=0)=45MV/m Optimization Code for FLASH Photo Injector

6 efld.dat FLASHgun_p12.dat Tuning parameters for efld Beam sizeXYrms0.170105 SolenoidMaxB(1)0.172724 Bucking Coil MaxB(2)0.019489 GunMaxE(1)45.00 Phi(1)-1.34264 BoosterMaxE(2)40.12 Phi(2)-14.85 Tuning parameters for FLASHgun_p12 Beam sizeXYrms0.15929 SolenoidMaxB(1)0.171247 Bucking Coil MaxB(2)0.015844 GunMaxE(1)45.00 Phi(1)-1.27222 BoosterMaxE(2)40.12 Phi(2)-14.85 horvert  0.32780.3273  reduced 0.29880.2982  37.5238.48  -2.204-1.792 horvert  0.31310.3128  reduced 0.2949  44.9745.87  -2.873-2.350 Field Files for the Gun Slightly different files but big consequencies

7 efld FLASHgun_p12 xx 37.52 yy 38.48 xx -2.204 yy -1.792 xx 20.61 yy 21.56 xx -0.509 yy -0.273  0.6356  reduced 0.4374  0.3266  reduced 0.2988 Calculated with best parameters for efld.dat. Comparison

8 Tuning Parameters ChargeXYrmsGun Phase, Phi(1) 1.1ps3.3ps4.4ps1.1ps3.3ps4.4ps 0.0200.1050.0700.071-0.945-0.231-0.289 0.0400.1110.1010.103-0.491-0.565-0.523 0.1000.1830.17410.170-1.435-1.519-1.348 ChargeBooster gradient, MaxE(2)Booster phase, Phi(2) 1.1ps3.3ps4.4ps1.1ps3.3ps4.4ps 0.02034.63839.8339.600.8870.3391.422 0.04022.27139.8336.880.867-0.7180.115 0.10034.58334.4039.600.1800.362-0.078 ChargeSolenoid MaxB(1)Bucking Coil, MaxB(2) 1.1ps3.3ps4.4ps1.1ps3.3ps4.4ps 0.0200.17020.17230.17200.06720.00690.0157 0.0400.17290.17200.17240.02020.02310.0148 0.1000.1740 0.1741-0.0381-0.034-0.0221 Field File efld.dat - Booster gradient and phase were considered as parameters to be optimized - Best value for booster gradient was found in the near of the desired 40.12MeV almost in all cases - Booster Phase seems not to affect the emittance significantly - Results after ~50 Iterations with Optimization Code with 2000 particles

9 Results after Booster at s=9.0m ChargeEmittanceBunch length 1.1ps3.3ps4.4ps1.1ps3.3ps4.4ps 0.0200.1800.1330.1260.6421.1121.254 0.0400.2540.1940.1890.9381.2221.342 0.1000.5330.3580.3171.0871.3361.478 ChargeBetaAlpha 1.1ps3.3ps4.4ps1.1ps3.3ps4.4ps 0.0209.8731.2222.93-1.435-4.393-3.292 0.04088.7619.9515.46-10.80-3.073-2.332 0.10017.5711.579.13-3.234-2.182-1.630 ChargeEnergy rmsmomentum 1.1ps3.3ps4.4ps1.1ps3.3ps4.4ps 0.02044.8566.41115.679.9291.1990.65 0.04060.6556.8878.2452.9791.2184.76 0.10088.0898.39100.879.7779.3590.65 Field File efld.dat - Run with 200000 particles with the best values from the optimization code

10 Bunch Shape for 4.4ps and 3.3ps 20pC, pulse length = 4,4ps 100pC, pulse length = 4,4ps 40pC, pulse length = 4,4 ps 40pC, pulse length = 3,3 ps100pC, pulse length = 3,3ps 20pC, pulse length = 3,3ps Optimization procedure was cut after 40-50 iterations  possibly not enough to find really best values

11 Slice Energy Emittance and Slice Energy Spread for 4.4ps and 3.3ps

12 Convergency: Slice Energy Spread and Slice Emittance Q=100pC Pulse Shape: Gaussian  =4.4ps N, x10 3 Mesh  m  mm  rms,mm E rms, keV  m  20015x250.3410.1321.47858.439.13-1.63 39221x350.3260.1291.48259.129.05-1.66 80030x500.3240.1291.48259.369.11-1.66 150041x680.3230.1291.48159.289.20-1.71 Main parameters after booster at s=9.00m

13 Sensitivity Test: Solenoid 100pC, 4.4ps I soll MaxB(1)  294.70.168220.445651.1691.3-40.86 296.50.169220.393933.6419.7-24.83 298.70.170470.328911.5148.3-9.294 299.60.170970.29891.3668.81-4.495 300.00.171220.29490.0044.97-2.873 300.40.171470.30473.3232.67-1.867 300.90.171720.324910.228.65-1.348 301.70.172220.387331.327.04-0.8815 303.50.173220.551887.112.25-0.4150 304.30.173720.752415511.31-1.099 Assume I soll (optimum)=300.0A - The accuracy of 0.1A of the set point of the solenoid current Should be sufficient to control the emittance - But big difference in the optics functions…

14 I soll MaxB(2)    5.60.005840.33997.90100.3-6.486 10.50.010840.32382.7975.99-5.010 16.00.016580.31500.0053.71-3.583 17.60.018340.31560.1348.21-3.211 20.10.020840.31991.5641.59-2.745 24.90.025840.34192.1932.25-2.025 29.80.030840.381821.227.12-1.557 34.60.035840.437038.724.51-1.269 Assume I soll (optimum)=16.0A Sensitivity Test: Bucking Coil 100pC, 4.4ps

15 Solenoid Test: Bunch Shape Still to clear up: if the emittance increase at higher solenoid field occurs only due to the tails of the bunch…

16 Bucking Coil Test: Bunch Shape

17 Summary Many open questions yet…


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