Upload
others
View
0
Download
0
Embed Size (px)
Citation preview
PTC-ORBIT Studies for the CERN LHC Injectors
Upgrade Project KEK: A.Molodozhentsev, E.Forest
CERN: G. Arduini, H. Bartosik, E.Benedetto, C.Carli, V.Forte, M.Fitterer, S.Gilardoni, M.Martini,
E.Metral, N.Mounet, F.Schmidt, R.Wasef
Outline Motivation Computational tools ‘Space-charge’ convergence study Machine study and the code benchmarking ‘Dynamic’ simulations of the Multi-turn injection for the CERN PS Booster Observation of the space charge effects for CERN PS and SPS Conceptual design of the CERN RCS
A.Molodozhentsev (KEK), ICFA HB12 workshop Beijing, China, September 17-21, 2012
Motivation CERN LHC (25nsec) beam upgrade scenario (LIU request)
A.Molodozhentsev (KEK), ICFA HB12 workshop Beijing, China, September 17-21, 2012
Motivation
A.Molodozhentsev (KEK), ICFA HB12 workshop Beijing, China, September 17-21, 2012
Space charge detuning estimations for the LHC Injectors
Computational tools
A.Molodozhentsev (KEK), ICFA HB12 workshop Beijing, China, September 17-21, 2012
‘Space-charge’ convergence study
A.Molodozhentsev (KEK), ICFA HB12 workshop Beijing, China, September 17-21, 2012
Space charge detuning for CERN PS-Booster (160MeV)
2D histogram
QV
QH 4 4.5
4
4.5
QH/QV=4.26/4.43
PTC-ORBIT(MPI)
‘Space-charge’ convergence study
RMS emittance evolution Evolution of the ‘halo’ part of the beam
RMS and 99% emittance evolution for different sets of the ‘space charge’ module of the code for the case of the lattice tunes QH / QV = 4.26 / 4.43 (CERN PS Booster)
A.Molodozhentsev (KEK), ICFA HB12 workshop Beijing, China, September 17-21, 2012
2.5D 2.5D
PTC-ORBIT(MPI)
Machine studies (MD-2012) and the PTC-ORBIT code benchmarking
LHC25 beam Bf ~ 0.4
A.Molodozhentsev (KEK), ICFA HB12 workshop Beijing, China, September 17-21, 2012
Motivation: reproduce the measured beam evolution
at 160MeV by the PTC-ORBIT tracking
Foot print QH/QV=4.18/4.23
4.5 4
4
4.5
Measured beam profile ‘Tomoscope’ image
Generated beam profile
Generated and measured transverse beam profile at the 160MeV energy
H V
-20 20 -10 10
PTC-ORBIT(MPI)
Machine studies (MD-2012) and the PTC-ORBIT code benchmarking
CERN PS-Booster
MD2
CERN PS-Booster H
V MD3
A.Molodozhentsev (KEK), ICFA HB12 workshop Beijing, China, September 17-21, 2012
… taken into account the random
error of the quadrupole strength of the PS Booster magnets
MD5
… including the random TILT of the PS Booster quadrupole magnets
[1,-1,0]
Linear coupling of the PS Booster:
QMIN 0.008
[1,0
,4] r
eson
ance
[2
,-2,0
] res
onan
ce
Accuracy of the RMS emittance measurements should be improved …
lattice with RANDOM errors { K1}QM #1: ‘ideal’ lattice #2 : 1Sigma = 1.0 10-3 (relative value) #3 : 1Sigma = 5.0 10-3
Up to 1Sigma = 4.28 10-5 rad
#2
#3
#1
Multi-turn injection for the CERN PS Booster with LINAC4
Significant improvement of the efficiency of the MT injection by using the H- stripping injection in the H-plane
Control over both transverse emittances Effects of the edge-focusing of the
‘slow’ bump-magnets, changing during the chicane reduction
A.Molodozhentsev (KEK), ICFA HB12 workshop Beijing, China, September 17-21, 2012
Multi-turn injection for the CERN PS Booster with LINAC4
0.000 0.001 0.002 0.003 0.004 0.005
-0.779
-0.778
-0.777
-0.776
-0.775
-0.774
-0.773
Qua
drup
ole
stre
ngth
[T/m
2 ]
Time [sec]
0 1000 2000 3000 4000 5000 6000
-80
-60
-40
-20
0
Hor
izon
tal c
hica
ne h
eigh
t [m
m]
Number of Turns
Begining of the MT Injection
End of the MT Injection
Lattice tunes: QH /QV =4.28/4.45 QV could be above 4.5 … Compensation the V beta-beating effect Active compensation scheme by
using 2 independent families of quads Reduction of the V-beta beat: 35% 5% Dynamic changing the quad strength
during the chicane’s fall from MAX ( -80mm) to ZERO
A.Molodozhentsev (KEK), ICFA HB12 workshop Beijing, China, September 17-21, 2012
#1 #2
V beta-beating around CERN PS Booster: #1 – before; #2 – after the ‘active’ correction
X-PX
<X> vz Nturns
KQ vz Time
PTC-ORBIT(MPI)
Multi-turn injection for the CERN PS Booster with LINAC4
Capture efficiency ~ 98%, Bf ~ 0.6
Double harmonic RF system with the longitudinal stacking of the bunches
A.Molodozhentsev (KEK), ICFA HB12 workshop Beijing, China, September 17-21, 2012
Particle distribution after 5520t
[rad]
W [G
eV]
PTC-ORBIT (space charge ON)
PTC-ORBIT(MPI)
A.Molodozhentsev (KEK), ICFA HB12 workshop Beijing, China, September 17-21, 2012
Multi-turn injection for the CERN PS Booster with LINAC4
0 1 2 3 4 5 6
1.20
1.25
1.30
1.35
1.40
1.45
Nor
mai
lzed
RM
S em
ittan
ce [u
m]
Time[msec]
H
V
0 1 2 3 4 5 6
6.0
6.5
7.0
7.5
8.0
8.5
9.0
Nor
mai
lzed
RM
S e
mitt
ance
[um
]
Time[msec]
V
H
Transverse emittance evolution (NO FOIL) V OFF-set ( 3mm) to control the Vertical emittance Space Charge effects ON (adapted grid) … 35.2e10ppb Incoherent space charge detuning < -0.5, Lattice tune QH / QV = 4.27 / 4.58
Effects of FOIL, Aperture limitation, machine imperfections should be analyzed
RMS Normalized Emittance 99% Normalized Emittance
PTC-ORBIT(MPI)
CERN PS: space charge effects and machine resonances
Tune scan at the energy 2.0GeV Typical tune-spread H,V ~(-0.18, -0.28)
Emittance growth near the [0,1,6] resonance has been studied experimentally … for the code benchmarking
Resonance Driving Terms: ‘pencil’ beam (LHC-INDIV) different horizontal kick strength
‘Realistic’ machine description by using the measured field nonlinearities of the PS magnets … … in progress … to reproduce the experimental observations.
A.Molodozhentsev (KEK), ICFA HB12 workshop Beijing, China, September 17-21, 2012
S.Gilardoni talk
CERN PS: space charge effects and machine resonances
0.2 0.4 0.6 0.8 1Frequency
0.002
0.004
0.006
0.008
0.01
edutilpmA
Resonanse_Basis
Observation of the [1,-1,0] resonance turn-by-turn data acquisition …
Turn-by-Turn data analysis
Linear coupling resonance observation (NO correction)
‘LHC-INDIV’ beam
A.Molodozhentsev (KEK), ICFA HB12 workshop Beijing, China, September 17-21, 2012
[1,-1,0] resonance observation
CERN SPS: space charge effects and machine resonances
• Tune scan for the Q20 SPS optics at 26GeV • Single bunch : 2.5-2.7e11 p/b • Normalized RMS emittance: 1.2 m in both planes • The incoherent space charge detuning: QH -0.15, QV -0.25.
A.Molodozhentsev (KEK), ICFA HB12 workshop Beijing, China, September 17-21, 2012
New scan
NO RMS emittance growth
NO RMS emittance growth
H.Bartosik talk
Losses !
RCS conceptual design Motivations (including the space charge at injection): alternative to the CERN PS Booster upgrade (160MeV-2GeV, 10Hz) effect the beam envelope modulations on the emittance growth effect of the super-periodicity
Qy -0.4
V [
m]
V [
m]
Variation of the beam size can lead to the emittance growth: the ‘TRIPLET’ features smallest variation of the transverse emittance compared to the ‘DOUBLET’ and the ‘FODO’ cell
‘Triplet’
‘FODO’ ‘Triplet’
Lattice tune above 2Qy=7 Including the Vertical
beta-beating correction …
Symmetry 1
Emittance growth due to excitation of ‘systematic’ resonances:
‘weak’ symmetry breaking in one cell with correcting the beat-beat
A.Molodozhentsev (KEK), ICFA HB12 workshop Beijing, China, September 17-21, 2012
PTC-ORBIT(MPI)
Injection
ExtractionRF
Conclusions
The performed benchmarking between the measured and simulated beam evolution for the CERN PS Booster at 160MeV shows very good agreement Optimization of main PS Booster setting has been performed to simulate the multi-turn injection process Data accumulation for the further study of the space charge effects for the LHC Injectors has been started to
perform extensive simulations during the ‘Shut-Down-1’ period
A.Molodozhentsev (KEK), ICFA HB12 workshop Beijing, China, September 17-21, 2012
A.Molodozhentsev (KEK), ICFA HB12 workshop Beijing, China, September 17-21, 2012