machine parameters and limitations in the eurisol beta-beam baseline
DESCRIPTION
Machine parameters and limitations in the EURISOL beta-beam baseline. A.Fabich AB department, CERN On behalf of the Beta-beam study group http://cern.ch/beta-beam. Outline. Conceptual Design study Beta-beam baseline design Machine parameters Ion intensities Limitations Production - PowerPoint PPT PresentationTRANSCRIPT
Machine parameters and limitations in the EURISOL beta-beam baseline
A.FabichAB department, CERN
On behalf of theBeta-beam study group
http://cern.ch/beta-beam
BENE week, Nov. 2005
A.Fabich, CERN
Beta-beam baseline:
Parameters & Limits, 2
Outline
Conceptual Design study Beta-beam baseline design Machine parameters Ion intensities
Limitations Production Decay losses Acceptance Tune shift
Conclusions
BENE week, Nov. 2005
A.Fabich, CERN
Beta-beam baseline:
Parameters & Limits, 3
Conceptual design study EURISOL Design Study
Within the 6th framework program of EU Conceptual Design Report for Beta-Beam
The baseline scenario is based on ISOL technique at CERN: usage of PS and SPS machines
The Beta-beam Design Study is aiming for: A beta-beam facility that will run for a “normalized” year of 107 s Providing an annual rate of
2.9*1018 anti-neutrinos (from 6He at =100) 1.1*1018 neutrinos (from 18Ne at =100)
BENE week, Nov. 2005
A.Fabich, CERN
Beta-beam baseline:
Parameters & Limits, 4
Beta-beam baseline design
Neutrino
Source
Decay Ring
Ion production
ISOL target & Ion source
Proton Driver
Decay ring
B = 1500 Tm B = ~5 T C = ~7000 m Lss= ~2500 m
6He: = 100 18Ne: = 100
SPS
Acceleration to medium
energy RCS
PS
Acceleration to final energy
PS & SPS
Beam to experiment
Ion acceleration
Linac
Beam preparation ECR
pulsed
Ion production Acceleration Neutrino source
Low-energy part
High-energy part
BENE week, Nov. 2005
A.Fabich, CERN
Beta-beam baseline:
Parameters & Limits, 5
mag
net
cyc
le (
abs
tra
ct)
cycle of 6He
Machine cycle
Baseline version:
Production 6He, 18Ne
ECR, Linac and RCS Cycling at 10 Hertz
Accumulation in the PS Accumulation of 20 RCS bunches (~2 seconds)
Acceleration through PS and SPS as fast as possible top = 100 for both isotopes
Injection into decay ring Merging with circulating bunches Every 6 s for 6He and every 3.6 s for 18Ne
BENE week, Nov. 2005
A.Fabich, CERN
Beta-beam baseline:
Parameters & Limits, 6
For the design goal of2.9*1018 antineutrinos/year1.1*1018 neutrinos/year
Required isotope intensities: Baseline version
Typical intensities of 108-109 ions for LHC injector operation (PS and SPS)
Ion intensities
6He 18Ne
Decay ring [ions stored] 9.7*1013 7.5*1013
SPS ej [ions/cycle] 9. 0*1012 4.3*1012
PS ej [ions/cycle] 9.5*1012 4.3*1012
Source rate [ions/s] 2*1013 2*1013
Top-dow
n
BENE week, Nov. 2005
A.Fabich, CERN
Beta-beam baseline:
Parameters & Limits, 7
Limitations
Isotope production
The self-imposed requirement to re-use a maximum of existing CERN
infrastructure
Cycling time, aperture limitations, collimation systems etc.
The high intensity ion bunches in the accelerator chain and decay ring
Space charge
Decay losses
BENE week, Nov. 2005
A.Fabich, CERN
Beta-beam baseline:
Parameters & Limits, 8
Ion production 6He figures have reached the design values but no safety margin is
yet provided.
18Ne figures are more than one order of magnitude below the desired performance. Missing factor (~25) for 18Ne production Within baseline:
Improvement of isotope production/preparation Possibly include an accumulation scenario at low energy
19Ne no immediate solution (for baseline scenario) Production rate much higher, but life time 10 times higher Acceleration of an order of magnitude more ions
Excluded by space charge limits in the PS and SPS
BENE week, Nov. 2005
A.Fabich, CERN
Beta-beam baseline:
Parameters & Limits, 9
Decay distribution
70% of first 6He bunch are lost before reaching decay ring Overall only 50% (6He) and 80% (18Ne) reach decay ring
Normalization Single bunch intensity to maximum/bunch Total intensity to total number accumulated in RCS
Bunch20th
15th
10th
5th1st
total
BENE week, Nov. 2005
A.Fabich, CERN
Beta-beam baseline:
Parameters & Limits, 10
Decay losses (1)
Relative decay distribution similar for both isotopes
~90% of all decays before entering decay ring occur in the PS
Can be translated into power losses and compared with “existing” high intensity operation
…
BENE week, Nov. 2005
A.Fabich, CERN
Beta-beam baseline:
Parameters & Limits, 11
In the PS most losses occur at low energy accumulation PS: (6He) [1.5 ; 9.3], (18Ne) [2.2 ; 15.5]
1st
20th
Decay losses (2)
1st
20th
BENE week, Nov. 2005
A.Fabich, CERN
Beta-beam baseline:
Parameters & Limits, 12
Power losses
Nucleon losses compared PS and SPS comparable for CNGS and bb operation PS exposed to highest power losses
cyclet
nucleonloss dttT
dt
dIcycleE )(/
machinecycle
lossloss ncecircumferet
cycleElP
*
//
Energy loss/cycle
Power loss
BENE week, Nov. 2005
A.Fabich, CERN
Beta-beam baseline:
Parameters & Limits, 13
H,V [µm] 6He 18Ne Cf., Acceptance
RCS inj 16.4, 8.8 16.4, 8.8 ?
PS inj 6.6, 3.5 4.0, 2.1 60, 20
SPS inj 0.8, 0.4 0.5, 0.3 28, 4.5
Scaling from normalized rms values of 7.8µm (H) and 4.2µm (V) for 11Tm 6He ions at PS injection, then
),(
),(*),(
machineion
PSinjrefmachineion
We assume the 18Ne has the same normalized emittance as the 6He because it comes from the Linac with identical βγ and is multi-turn injected into the RCS with the same geometrical set-up.
S.Hancock1σ Physical Emittance
BENE week, Nov. 2005
A.Fabich, CERN
Beta-beam baseline:
Parameters & Limits, 14
Max 6He ions Max 18Ne ions Max |QV|inj
RCS ej (1 bunch) 7×1012 0.8×1012 0.5 (?)
PS ej (20 bunches) 7×1012 3×1012 0.3
SPS ej (20 bunches) 6×1012 3×1012 0.2
Considering for simplicity a round Gaussian beam of fully stripped ions, the self-field incoherent (“Laslett”) tune shift is
V
b
b
p
pV
NR
c
r
A
ZQ
3
2
4
3
We assume τb = 80% of the rf bucket duration in all cases.
This allows upper limits on the total number of ions per shot to be estimated (taking into account unequal bunches) based on known limits at injection.
S.HancockLimits due to Tune Shift
BENE week, Nov. 2005
A.Fabich, CERN
Beta-beam baseline:
Parameters & Limits, 15
Solve tune shift limit
1. Two batches from the PS instead of one.
2. One could also imagine deliberately blowing up the emittance to improve the situation in the downstream machine.
6He 18Ne
required QV,inj limit required QV,inj limit
RCS ej (1 bunch) 0.63×1012 7×1012 0.16×1012 0.8×1012
PS ej (20 bunches) 6.7×1012 7×1012 2.6×1012 3×1012
SPS ej (40 bunches) 11×1012 10×1012 4.9×1012 5×1012
S.Hancock
BENE week, Nov. 2005
A.Fabich, CERN
Beta-beam baseline:
Parameters & Limits, 16
Conclusions
Baseline parameters fixed Study goes now into detail of different machines and aspects
Average power losses are comparable to CNGS case (which is accepted) PS has to stand the most demanding losses Power losses < 3 W/m
Limits set by space charge in both the PS and SPS machines.
Main efforts will now focus on 18Ne shortfall.