the decay ring -first design- a. chancé, j.payet cea/dsm/dapnia/sacm
DESCRIPTION
The Decay Ring -First Design- A. Chancé, J.Payet CEA/DSM/DAPNIA/SACM. Summary. General parameters Optical functions The injection system Optical properties Decay products losses. General parameters. Decay ring. Parameters of the radioactive ion beams. 688 m. 2385 m. - PowerPoint PPT PresentationTRANSCRIPT
March 16-18 1A. Chancé, J. Payet DAPNIA/SACM / Beta-beam ECFA/BENE Workshop
The Decay Ring -First Design-
A. Chancé, J.PayetCEA/DSM/DAPNIA/SACM
March 16-18 2A. Chancé, J. Payet DAPNIA/SACM / Beta-beam ECFA/BENE Workshop
Summary
•General parameters
•Optical functions
•The injection system
•Optical properties
•Decay products losses
March 16-18 3A. Chancé, J. Payet DAPNIA/SACM / Beta-beam ECFA/BENE Workshop
General parameters
• Total length 6931 m, arc length 1080 m.
• The injection is located in the arc.
• Low contribution of the optic to the ν-beam angular divergence.
• Free straight sections, at each arc entry, enable decay products extraction.
6He2+ 18Ne10+
100 100
Energie (GeV) 555 1669
BT.m) 931 559
(s) at rest 0.8 1.67
rmsmm.mrad) 0.233 0.465
N Injected (ions/batch) 0.9 1013 4.9 1011
N Stored (ions/batch) 1.3 1014 1.5 1013
688 m
2385 m
Parameters of the radioactive ion beams
injection
Decay ring
March 16-18 4A. Chancé, J. Payet DAPNIA/SACM / Beta-beam ECFA/BENE Workshop
At the injection point, dispersion is as high as possible (8.18 m) while the horizontal beta function is as low as possible (13.1 m).
Free straight sections behind the first bend, used as a dispersion suppressor, are designed to enable extraction of the decay products coming from the long straight sections.
Optical functions in the long straight sections keep the ν beam angle growth below 5%.
The arc is a 2 insertion. Optical functions in the arcs are smaller to reduce magnet apertures.
Optical functions
-5
0
5
10
15
20
0 500 1000 1500 2000 2500 3000
b1/2 (m) bx1/2
by1/2
Dx
nx = 18.23
ny = 10.16
s (m)
Half ring optical functions
Arc optical functions
-5
0
5
10
15
20
99,48 299,48 499,48 699,48 899,48 1099,48
b1/2 (m)
bx1/2
by1/2
Dx
s (m)
March 16-18 5A. Chancé, J. Payet DAPNIA/SACM / Beta-beam ECFA/BENE Workshop
Injection
-2,5
0,0
2,5
5,0
7,5
10,0
0 50 100 150
-2,5
0,0
2,5
5,0
7,5
10,0
0 50 100 150-2,5
0,0
2,5
5,0
7,5
10,0
0 50 100 150
Layout
deviated beam kicker
injectedbeam
SEPTUM E/E D
Dispersive area
Horizontal envelopes at injection
Deviated beam
Injected beam
Injected beam
after one turn
envelopes (cm)
Septum blade
s (m)
• Injection is located in a dispersive area
• The stored beam is pushed near the septum blade with 4 “kickers”. At each injection, a part of the beam is lost in the septum
• Fresh beam is injected off momentum on its chromatic orbit. “Kickers” are switched off before injected beam comes back
• During the first turn, the injected beam stays on its chromatic orbit and passes near the septum blade
• Injection energy depends on the distance between the deviated stored beam and the fresh beam axis
March 16-18 6A. Chancé, J. Payet DAPNIA/SACM / Beta-beam ECFA/BENE Workshop
Beam losses and beam size (in rms number)
Power lost by the stored beam on the septum blade
T
EN
a
aP
T
ITlosses
112
21
10
• T : repetition rate (8 s)
: half-life of the ion at rest
• NI : injected ions number at each injection
• a : transmission coefficient of the stored beam through the septum blade
• a is related to the number of rms, nm
• 1D Gaussian beam distribution assumed
mn
dxxfa
Then, with 4.1 rms for the stored beam and 3.3 rms for the injected beam, the deposited power on the septum blade is below 20 W.
The relative injection energy is then about 0.5%.
The “kicker” deviations are 1.1 mrad (0.5 T) and 0.41 mrad (0.38 T)
1E+0
1E+1
1E+2
1E+3
1E+4
1E+5
1E+6
0 1 2 3 4 5
Losses (W)
Number of rms
Helium
Neon
March 16-18 7A. Chancé, J. Payet DAPNIA/SACM / Beta-beam ECFA/BENE Workshop
Beam envelopes
-6
-4
-2
0
2
4
6
0 1000 2000 3000
envelopes (cm) Horizontal
Verticals(m)
Injected beam envelopes
Stored beam envelopes
In the long straight sections, the apertures (±5 cm in both planes) are defined by the stored beam sizes.
In the arc, the horizontal aperture is defined by the injected beam and the vertical one by the stored beam sizes.
By arc, there are 590 m of 5 T field bend with 4 cm radius aperture.
The injection septum is 22.5 m long and its field is 1 T.
-6
-4
-2
0
2
4
6
0 1000 2000 3000
envelopes (cm)Horizontal
Verticals (m)
March 16-18 8A. Chancé, J. Payet DAPNIA/SACM / Beta-beam ECFA/BENE Workshop
2nd order study
10
10,25
10,5
10,75
11
18 18,25 18,5 18,75 19
4th order
3rd order
2nd order
νx
νz
Chromaticity corrected by 2 families of sextupoles.
Arcs are 2Pi insertions. The tunes are given by the
straight sections phase advances.
It is quite easy to optimize the tunes.
The working point is chosen according to :
1. the dynamic aperture
2. the momentum acceptance
Physically, the momentum acceptance is limited by the septum position.0
0,02
0,04
0,06
0,08
0,1
0,12
-0,1 -0,05 0 0,05 0,1
z (m)
x (m)
Dynamic aperture at the injection point
Best point
March 16-18 9A. Chancé, J. Payet DAPNIA/SACM / Beta-beam ECFA/BENE Workshop
Decay products extraction
-0,1
0,0
0,1
0,2
0,3
2300 2350 2400
HorizontalVertical
s (m)
envelopes (m)
Fluorine extraction
Bρ(18F9+) ≈ 621 T.m
-0,3
-0,2
-0,1
0,0
0,1
2300 2350 2400
HorizontalVertical
s (m)
envelopes (m)
Lithium extraction
Bρ(6Li3+) ≈ 621 T.m
Two free straight sections after the first arc dipole enable the extraction of decay products coming from long straight sections.
Lithium extraction can be made without a septum.
Fluorine extraction needs an additional septum.
In the Lithium extraction case, the first bend aperture has to be increased to 5 cm.
The permanent septum for Fluorine extraction is 22.5 m long and its field is 0.6 T.
Fluorine extraction
Lithium extraction
March 16-18 10A. Chancé, J. Payet DAPNIA/SACM / Beta-beam ECFA/BENE Workshop
Decay products losses in the arcsLithium deposit
Fluorine deposit
We have begun studying the repartition of the disintegrations in the arcs.
Most of decay products deposits come into the dipoles.
Problem of radioprotection in the arc
Problem of dipole cooling
This design is not valuable due to this deposit level
0
25
50
75
100
35 45 55 65
Pdeposit (W/m)
s (m)
0
2,5
5
7,5
10
12,5
15
17,5
20
35 45 55 65
Pdeposit (W/m)
s (m)
March 16-18 11A. Chancé, J. Payet DAPNIA/SACM / Beta-beam ECFA/BENE Workshop
Decay products losses in the arcs (2)Most of Lithium is deposited at the middle of dipoles
we have divided the dipoles in two 6T bends and separated them with a drift.
The chamber sizes between the two dipoles are small to maximize the deposition here.
Problem of radioprotection
Fewer problems in the dipoles
The injection section must still be studied.
We have to compare with the TRIUMF results.
Helium decay
Neon decay0
25
50
75
100
125
150
175
200
35 45 55 65
0
0,5
1
1,5
2
2,5
3
3,5
4
4,5
5Pdeposit (W/m)
s (m)
Chamber size (cm)
0
2,5
5
7,5
10
12,5
15
17,5
20
35 45 55 65
0
0,5
1
1,5
2
2,5
3
3,5
4
4,5
5Pdeposit (W/m)
Chamber size (cm)
s (m)
March 16-18 12A. Chancé, J. Payet DAPNIA/SACM / Beta-beam ECFA/BENE Workshop
Conclusions
Some positive remarks can be made :
•The injection system and the bending magnet seem realistic.
•The contribution of the optic to the ν-beam angular divergence is low.
•The decay ring length, 6930 m, is what was expected.
•Free straight sections, at each arc entry enable the extraction of a part of decay products.
More studies are yet needed :
•The acceptable beam losses on the septum blade have to be defined according to the radio-protection.
•This can modify the beam sizes and then the injection energy, the apertures and the fields of the magnetic elements.
•A new design could focus most of losses outside the bends. Recently, we are working on this.