Gun Calculations by Poisson Model for Non-Uniform Distributions

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Presentation transcript:

Gun Calculations by Poisson Model for Non-Uniform Distributions animation cathode distributions tables many plots bunch prototype: XFEL bunch, 250 pC Gun Calculation with Astra “rz” and restarted “xyz” rz-case, without/with restart xyz: shifted solenoid (1mm) xyz: rotated solenoid (1mrad) but: more about the rz-case

Gun Calculations by Poisson Model for Non-Uniform Distributions an exemplary investigation the bunch (prototype): 250 pC, XFEL type, see http://www.desy.de/xfel-beam/s2e/xfel/Nominal/nom250pC.html longitudinally: z/m Astra generator Lt=20psec, rt=2psec Gun 60 MV/m, 0.2234 T transversely: uniform, R = 1 mm (rms = 0.5 mm) modifications: r(z)  halo & FLASH type xy(z)  odd & random fluctuations calculations with MATLAB code “stupid”, version=“less stupid”

r(z)-cathode distributions: uniform 90% uniform, 10% halo rms 80% uniform 20% halo Flash

xy(z)-cathode distributions: 10% rms, cutoff=0.2mm 20% rms, cutoff=0.2mm odd 20% rms, cutoff=0.4mm -10% +10%

slice parameters for |z|<1mm

uniform distribution, XFEL q/pC = 250 z/m = 2.6038 twiss,x,y/m= 2.1466, 2.144 E,slice/eV = 443.2164 averaged for |z|<1mm

90% uniform, 10% in halo q/pC = 250 z/m = 2.6038 twiss,x,y/m= 2.1828, 2.1819 E,slice/eV = 436.6104 averaged for |z|<1mm

80% uniform, 20% in halo q/pC = 250 z/m = 2.6038 twiss,x,y/m= 2.3359, 2.3303 E,slice/eV = 460.346 averaged for |z|<1mm

odd odd q/pC = 250 z/m = 2.6038 /m = 0.96395, 0.98515 twiss,x,y/m= 2.1079, 2.119 E,slice/eV = 463.0909 averaged for |z|<1mm -10% +10%

10% rms, cutoff=0.2mm q/pC = 250 z/m = 2.6038 twiss,x,y/m= 2.1291, 2.1505 E,slice/eV = 460.4812 averaged for |z|<1mm

20% rms, cutoff=0.2mm q/pC = 250 z/m = 2.6038 /m = 0.9507, 1.0129 twiss,x,y/m= 2.1997, 2.1453 E,slice/eV = 479.0362 averaged for |z|<1mm

20% rms, cutoff=0.4mm q/pC = 250 z/m = 2.6038 twiss,x,y/m= 2.1541, 2.1878 E,slice/eV = 478.8229 averaged for |z|<1mm

XFEL-bunch + Flash fields averaged for |z|<1mm uniform, XFEL-bunch with Flash fields q/pC = 250 z/m = 1.4553 /m = 1.0605, 1.0562 twiss,x,y/m= 2.1541, 2.1878 E,slice/eV = 240.8263

Flash-bunch + Flash fields averaged for |z|<1mm uniform, FLASH-bunch with Flash fields q/pC = 250 z/m = 1.4553 /m = 1.4711, 1.4739 twiss,x,y/m= 12.1024, 12.0782 E,slice/eV = 798.1202

uniform distribution, XFEL q/pC = 250 z/m = 2.6038 twiss,x,y/m= 2.1466, 2.144 E,slice/eV = 443.2164 averaged for |z|<1mm

90% uniform, 10% in halo q/pC = 250 z/m = 2.6038 twiss,x,y/m= 2.1828, 2.1819 E,slice/eV = 436.6104 averaged for |z|<1mm

80% uniform, 20% in halo q/pC = 250 z/m = 2.6038 twiss,x,y/m= 2.3359, 2.3303 E,slice/eV = 460.346 averaged for |z|<1mm

odd q/pC = 250 z/m = 2.6038 /m = 0.96395, 0.98515 twiss,x,y/m= 2.1079, 2.119 E,slice/eV = 463.0909 averaged for |z|<1mm

10% rms, cutoff=0.2mm q/pC = 250 z/m = 2.6038 twiss,x,y/m= 2.1291, 2.1505 E,slice/eV = 460.4812 averaged for |z|<1mm

20% rms, cutoff=0.2mm q/pC = 250 z/m = 2.6038 /m = 0.9507, 1.0129 twiss,x,y/m= 2.1997, 2.1453 E,slice/eV = 479.0362 averaged for |z|<1mm

20% rms, cutoff=0.4mm q/pC = 250 z/m = 2.6038 twiss,x,y/m= 2.1541, 2.1878 E,slice/eV = 478.8229 averaged for |z|<1mm

uniform, XFEL-bunch with Flash fields q/pC = 250 z/m = 1.4553 averaged for |z|<1mm uniform, XFEL-bunch with Flash fields q/pC = 250 z/m = 1.4553 /m = 1.0605, 1.0562 twiss,x,y/m= 2.1541, 2.1878 E,slice/eV = 240.8263

uniform, FLASH-bunch with Flash fields q/pC = 250 z/m = 1.4553 averaged for |z|<1mm uniform, FLASH-bunch with Flash fields q/pC = 250 z/m = 1.4553 /m = 1.4711, 1.4739 twiss,x,y/m= 12.1024, 12.0782 E,slice/eV = 798.1202

Gun Calculation with Astra “rz” and restarted “xyz” an other exemplary investigation the bunch: 250 pC, XFEL type, see http://www.desy.de/xfel-beam/s2e/xfel/Nominal/nom250pC.html as before longitudinally: z/m Astra generator Lt=20psec, rt=2psec Gun 60 MV/m, 0.2234 T transversely: uniform, R = 1 mm (rms = 0.5 mm)

case 1: axial gun solenoid case 2: 1 mm shift (not axial) case 3: 1 mrad rotation (not axial)

mirror charges are switched off at ~ 10cm case 1: fully 2d, restarted 2d (from z=1cm), restarted 3d (from z=1cm)  z = 1m mirror charges are switched off at ~ 10cm but: restart without mirror charges noise reduction (Hammersly), 1MP

as before, but solenoid is shifted by 1mm case 2: fully 2d, restarted 2d (from z=1cm), restarted 3d (from z=1cm)  z = 1m as before, but solenoid is shifted by 1mm noise reduction (Hammersly), 200kP

2d solution, without shift case 2  case 1 z = 1m ??? noise 2d, 1MP  3d, 200kP 2d solution, without shift

as before, but solenoid is rotated by 1mrad case 3: fully 2d, restarted 2d (from z=1cm), restarted 3d (from z=1cm)  z = 1m as before, but solenoid is rotated by 1mrad noise reduction (Hammersly), 200kP

2d solution, without shift case 3  case 1 z = 1m ??? noise 2d, 1MP  3d, 200kP 2d solution, without shift

BUT

case 1: fully 2d, restarted 2d (from z=1cm), restarted 3d (from z=1cm)  z = 1m & 2.6m

case 1:  z = 2.6m Astra with 1MP, Hammersly stupid with 3.2MP, no noise reduction (random generator)

?! case 1:  z = 2.6m, Astra with 1MP, Hammersly (a) rz, restart from 1cm & 1m (b) restart from 1m with doubled transverse resolution ?!