particle information from beamline simulations
DESCRIPTION
Particle Information from Beamline Simulations. K. Walaron Univ. of Glasgow/ R.A.L. Overview. Beamline introduction Details on beamline parameters for 6/10pi beamlines Beamline simulations XY plots (TOF0/TOF1/CKOV1) Ptot plots (TOF0/TOF1/CKOV1) TOF separation - PowerPoint PPT PresentationTRANSCRIPT
K.Walaron PID review (Oct 12th 2006) R.A.L
Particle Information from Beamline Simulations
K. WalaronUniv. of Glasgow/ R.A.L
Overview Beamline introduction Details on beamline parameters for
6/10pi beamlines Beamline simulations XY plots (TOF0/TOF1/CKOV1) Ptot plots (TOF0/TOF1/CKOV1) TOF separation TOF v Ptot with approximated resolution
Goals of beamline
Provide matched beams of variable emittance and momenta
P =140,200,240MeV/c. Emitt4D=Low,6,10pi mm mrad
Provide pion/muon separation
Beamline Layout
TOF1CKOV1 (old design)TOF0
Quad triplet
Quad triplet
Dipole 2
Beamline Simulations Tracking program used is G4Beamline (GEANT4 based) No sensitive detector implementation in G4beamline.
Only MC truth output of particles crossing planes. Analysis chain:Track beam using G4BLMany runs with Pi+ decay offRun with Pi+ decay onOutput ascii filesTo produce high pi+ stats ~100M pi+ tracked from targetTo produce mu+ stats ~10M pi+ tracked from targetC++/scripts order tracks and output Root fileAnalysis in rootDidn’t have time to make plots look nice. Apologies in
advance.
TOF’s and old CKOV implementation
Old CKOV implementation (z=21.060)
TOF0 & TOF1 implementation
TOF0 Polyethelene, density=0.93g/cm^3
50cmx50cm z=20.810m
TOF1 Polyethelene, density=0.93g/cm^3
48cmx48cm z=28.871m
New CKOV 1a and 1b implementation
Assumption
6pi 200 MeV/c (215.31 <Emu<252.2) Red=NEW, BLUE=OLD
TOF0 CKOV1 TOF1 TOF0 CKOV1 TOF1
TOF0 CKOV1 TOF1TOF0 CKOV1 TOF1
10pi 200 MeV/c (215.31 <Emu<252.2) Red=NEW, BLUE=OLD
TOF0 CKOV1 TOF1 TOF0 CKOV1 TOF1
TOF0 CKOV1 TOF1TOF0 CKOV1 TOF1
XY dist TOF0 (combined pi/mu for 6pi and 10pi
6pi 10pi
y (
cm
)
x (cm) x (cm)
CKOV1 beam spoty (
cm
)
x (cm)
No cut on singles
XY dist TOF1 (combined pi/mu for 6pi and 10pi
6pi 10pi
y (
cm
)
x (cm) x (cm)
Ptot dist TOF0 (combined pi/mu for 6pi and 10pi
6pi 10piPtot (MeV/c) Ptot (MeV/c)
Ptot dist CKOV1 (combined pi/mu for 6pi)
Ptot (MeV/c)
Ptot dist TOF1 (combined pi/mu for 6pi and 10pi
Ptot (MeV/c) Ptot (MeV/c)
6pi 10pi
TOF (combined pi/mu for 6pi and 10pi
6pi 10pi
Gaussian TOF spread
MC truth V MC truth_spread
TOF (MC truth) v Ptot@Tracker1 (MC truth) 6pi, 10pi.
Ptot (MeV/c)
T (
ns)
TOF (spread) v Ptot@Tracker1 (MC truth) 6pi, 10pi.
70ps gaussian spread on TOF0 & 1
6pi mm mradPtot (MeV/c)
T (
ns)
10pi mm mrad
70ps gaussian spread on TOF0 & 1
Beamline purity (sampled at TOF0)
Tune Particle % of beam content
CM14-200-6pi Proton 0
pi+ 0.2
mu+ 99.6
e+ 0.2
CM14-200-10pi Proton 0
pi+ 0.2
mu+ 99.7
e+ 0.1
Rates old/new CKOV designs (uncollimated)
OLD
NEW
Rates with new CKOV design and collimation (6pi tune only)
TOF0 1.591
CKOV1 1.511
TOF1 0.662
Tracker1a
0.634
Good mu+
0.493
TOF0 2.731
CKOV1 2.578
TOF1 1.061
Tracker1a
1.017
Good mu+
0.747
11cm horiz collimation 21cm horiz collimation
Conclusions Detector sizes are at least sufficiently wide
to capture the particles making it to tracker1. Make them smaller..
Implementation of new CKOV design should provide no problem for future tunes.
Singles rates are a problem for TOF0. Likely to need collimation to bring rate down to required 1.5 MHz.
Real conclusions should be from reviewers!