preliminary rp simulations concerning proton beam losses in awake
DESCRIPTION
Preliminary RP simulations concerning proton beam losses in AWAKE. Silvia Cipiccia 1,2 , Eduard Feldbaumer 2 , Helmut Vincke 2 1 University of Strathclyde 2 CERN DGS/RP. Outline. Implemented geometry Accident scenario Metal shielding effect Prompt dose Damage 2 Electronics - PowerPoint PPT PresentationTRANSCRIPT
Preliminary RP simulations concerning proton beam losses
in AWAKESilvia Cipiccia1,2, Eduard Feldbaumer2, Helmut Vincke2
1 University of Strathclyde2 CERN DGS/RP
Outline
• Implemented geometry• Accident scenario• Metal shielding effect– Prompt dose– Damage 2 Electronics
• Air Activation• Conclusions
Implemented Geometry
CNGS 2002:Simple clean geometry
80 cm thick concrete wall
50 cm Ø laser core
30 cm thick concrete wall
Preliminary AWAKE Geometry
Access gallery
p+ beam
e-gun room
CNGS target
Accident Scenario
• Beam Parameters:
• Copper target: Ø = 10 cm, l = 50 cm• Beam position: 10 cm before copper• 2 different scenarios (worst cases):– Full beam loss in front of big venting gallery– Full beam loss in front new electron gallery
• Dose conversion coefficient: EWT74 worst case scenario
p+ energy Energy spread Beam shape
400 GeV 0% Pencil beam
Dose limit for low-occupancy supervised radiation area: 15 Sv/h (to avoid future need for active dosimeter)
e- gallery big venting tunnel
Accident ScenarioEffective dose per incident proton (pSv/proton)
Accident scenario loosing 1 bunch of nominal beam (from Chiara):# Shots per Year
Bunch Intensity
Beam Lost per Shot
Total Loss
Steering 100 5E9 p+ 10% 5E10 p+
Accident 2 3E11 p+ 100% 6E11 p+
Target position dose/p+ @ access gallery
error Bunch intensity
Accident dose / bunch
e-BG 2.3e-4 pSv/p+ 9.9% 3e11 69 Sv
BVT 4.6e-4 pSv/p+ 4.9% 3e11 138 Sv
Safety Code F: Annual dose > 100 Sv Optimization required
Plasma cell
• P+ beam:– Beam size: s =250 mm
• Beam lost at the valve (valve fails opening)• Plasma Channel
• 5 m long• 4 cm Ø• Rb vapor (1015 cm-3 ->1.4x10-7 g/cm3)
• Fast Valve: 5 mm thick, 4 cm Ø, material steel AISI304• Metal shielding: cylinder
– inner diameter 30 mm, – thickness 2mm, – material steel AISI304 – length 6m
Fast valve close
Rbvapour
Metal shieldingFast valve open
vacuum
Proton beam evolution
From Alexey simulations:• Proton beam in plasma undergoes SMI->increasing in beam divergence
Initial distributions
sx,y 200 mm
0.024 mrad
0.36 mrad
sz 139 mm
Not-ionized
ionized
Proton beam evolution
Alexey-FLUKA Comparison
Proton distribution after plasma cell
Valve close accident scenario
Dose equivalent mSv/bunch (3e11 p+)
dose/p+ @ access gallery
error Bunch intensity
Accident dose / bunch
9.6e-6 pSv/p+ 10% 3e11 2.9 Sv
Preliminary: damage to electronics
From M. Brugger presentation for Cern Fluka user meeting 2008
commercial COTS hardened electronics
accelerators
!!! A Rough Overview Only !!!
Semiconductors
Polymers
Ceramics
Metals and alloys
• Cumulative damage
• Stochastic damage• From M. Brugger ‘Radiation Damage to electronics at the LHC’, IPAC2012:
– Commercial equipment: ~107 HEH/cm2/year
Closed valve accident scenario: D2E
1 MeV Neutron equivalent: safe limit 1013 n/cm2
HEH safe limit 107 cm-2 : exceeded in vicinity of plasma
0 10 20 30 40 50 60 70 80 90 1001.0E-04
1.0E-03
1.0E-02
1.0E-01
1.0E+00
Det1Det2Det3Det4
cm
Gy
Energy Deposited safe limit 102 Gy
Shielding radius [mm]
Shielding length [m]
Dose equivalent[pSv/p+]
Dose equivalent[mSv/h]
error
3 6 4.1e-5 1.5e3 18%10 6 2.1e-7 7.56 70% 15 6 6.9e-10 2.45e-2 39%
10 mm steel 6 m long
15 mm steel 6 m long
3 mm steel 6 m long
Metal shielding effect: Dose equivalent [mSv/bunch]
10 mm steel 6 m long3 mm steel 6 m long
15 mm steel 6 m longFor 15 mm radius around plasma cell still 1-2 orders of magnitude higher than recommended value
Metal shielding effect: HEH fluence per year
safe limit 107cm-2
Metal shielding effect: 1 MeV n-eq per year
3 mm steel 6 m long 10 mm steel 6 m long
15 mm steel 6 m long
safe limit 1013 n/cm2
No metal shielding15 mm radius shielding
• Without metal shielding around plasma cell HEH fluence still higher than 107 cm-2
• Looking at beam profile: halo due to the interaction of proton beam with gas:
• Gas interaction length for 400 GeV p+: 109 cm -> in 10 m 3x105 p+ per beam interact with the gas and broaden the beam
Scattered particles
Metal shielding and gas effect:HEH fluence
0 10 20 30 40 50 60 70 80 90 1001.0E+0
1.0E+2
1.0E+4
1.0E+6
Worst position detector after 1 year
Det 2 3mm 6 m
Det 2 10mm 6 m
Det 3 15 mm 6 m
Distance from proton beam
ener
gy D
epos
ited
[Gy]
shielding radius [mm]
plasma cell radius [cm]
Shielding length [m]
cm-2/p+ cm-2/year
3 2 6 1.80E-03 8.71E+13
10 2 6 5.20E-07 2.52E+10
15 2 6 2.11E-09 1.02E+08Still 1 order of magnitude too high
HEH fluence summary:
Energy deposition comparison:
Metal shielding summary
From preliminary studies level below damage limit
1 MeV neutron equivalent
Air ActivationAir Activation studies in the CNGS target chamber during AWAKE operation
CNGS target chamber
He Tube1
Target Horn
He Tube2 Decay TubeBeam
Reflector
SIMULATION PARAMETERS:
• Proton beam starting point: Beginning of Plasma cell 33.01m upstream from CNGS target
• Irradiation time 1h• Air exchange rate: 16000 m3/h (CNGS flush mode)
Dose rate AWAKE-CNGS
Collimator
Target
No Target
CNGS targetCollimator
CNGS target
Three scenarios:Implemented geometry
Air ActivationDose rate evolution collimator
0 100 200 300 400 500 600 7000.0
1.0
2.0
3.0
4.0
5.0
6.0
7.0
8.0
9.0
10.0
0
10
20
30
40
50
60
70
dose ratedose rate - Air exchangecumulative dosecumulative - Air exchange
Time (min)
Dose
Equ
ival
ent R
ate
(mSv
/h)
Cum
ulati
ve d
ose
equi
vale
nt (µ
Sv)
6.5h
40 min
Ultimate beam 1h: 3.5E11 p/bunch, 0.14 Hz Air volume: 2492 m3
Air exchange rate: 16000 m3/h
Air Activation
0 100 200 300 400 500 600 7000.0
1.0
2.0
3.0
4.0
5.0
6.0
7.0
8.0
9.0
10.0
0
5
10
15
20
25
30
35
40
45
50
dose ratedose rate - Air exchangecumulative dosecumulative - Air exchange
Time (min)
Dose
Equ
ival
ent R
ate
(mSv
/h)
Cum
ulati
ve d
ose
equi
vale
nt (µ
Sv)
Ultimate beam 1h: 3.5E11 p/bunch, 0.14 HzAir volume: 2493 m3
Air exchange rate: 16000 m3/h
4.5h
30 min
Dose rate evolution target
Air Activation
Ultimate beam 1h: 3.5E11 p/bunch, 0.14 HzAir volume: 2493 m3
Air exchange rate: 16000 m3/h
0 100 200 300 400 500 600 7000.0
1.0
2.0
3.0
4.0
5.0
6.0
7.0
8.0
9.0
10.0
0
1
2
3
4
5
6
7
8
9
10
dose ratedose rate - Air exchangecumulative dosecumulative - Air exchange
Time (min)
Dose
Equ
ival
ent R
ate
(mSv
/h)
Cum
ulati
ve d
ose
equi
vale
nt (µ
Sv)
20 min
1.5h
Dose rate evolution no target
PROMT DOSE AND D2E SIMULATIONS• The presence of the metal shielding for the electron beam creates hard
environment for electronics. The level of radiation depends on the geometry of the shielding
• The minimum level of HEH fluence due to gas effect: 1-2 orders of magnitude higher than recommended -> shielding may be required
• Which material to use for the plasma cell wall? More details needed• Preliminary results only: waiting for technical design to implement final geometry
AIR ACTIVATION • Air inside CNGS target chamber considered radioactive after 1h of nominal AWAKE
beam operation• Airborne radioactivity level inside CNGS target chamber
• Limited stay area• Ok, no access required during AWAKE operation
• Radioactive Air release through access gallery: no access during proton operation• Ventilation and access requirements: still under discussion• Collimator should be removed, CNGS target removal not necessary
Conclusion
Thanks for your attention!