2. !
potential to deliver beams of several MW
drivers for a large variety of applications:
Power Energy
Condensed matter spallation neutrons ~ 1 MW ~ 1 GeV
materials irradiation neutrons from stripping reaction 2 x 5 MW 40 MeV
RIBs for nuclear & astro-physics with neutrons 4 MW ~ 1 GeV
secondary beams for particle
muon, neutrino production 4 MW 5 GeV
physics
hybrid subcritical reactors for
demonstrator 5 MW 0.6
transmutation
Note: superconducting (SRF) technology
higher gradient capabilities & lower operational costs wrt. NC
adopted in most of the designs for the major part of the linac
32. "-
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General Design:
H& . (
• Houses 6 HWR and 3
superconducting solenoids
• Very compact design in N/P
M 4 )5 . *
longitudinal direction
N /6 P (
M 4 )5 .
3 *
• Cavity vacuum and insulation
vacuum separated
M. Pekeler, LINAC 2006
ACCEL Instruments GmbH
((
36. quot; 2 5
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$ %C
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A B B
BGA GA
( 2 86 2 2 2
-.
MEBT: 2 options (MCG type / solenoid-triplet type)
. .!
DTL: 4 tanks at 19.40, 37.68, 56.43 & 74.8 MeV, 6 cells
CCL: At 972 MHz: > 60, 14 cell cavities, 3.5 separations, spoke option ?
SPL: ~ 70, 4/6 cell cavities, doublet focusing, ~ 23 cells
Beam power for 2 MW, 30 Hz, 3.2 GeV RCS 0.5 MW
Beam pulse current before MEBT chopping 43.0 mA
Beam pulse current after MEBT chopping 30.0 mA
Number of injected turns for a 370 m RCS ~500 turns
Beam pulse duration at the 30 Hz rep rate ~700.0 s
Duty cycle for the extent of the beam pulse ~2.1 %
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To Ring
402.5 MHz 805 MHz
HEBT
MEBT
DTL CCL
RFQ SCL, ß=0.61 SCL, ß=0.81
Linac dump
Injector 2.5 MeV 86.8 MeV 186 MeV 391 MeV 1 GeV
β =0.55 β =0.71 β =0.87
Length ~260 m, 96 independently phased RF cavity/tanks
Normal conducting linac from the H- ion source to 186 MeV
Superconducting linac from 186 MeV to 1 GeV
Beam commissioning of the SCL began in August 2005
Achieved the design repetition rate 60 Hz, maximum beam
energy 1.01 GeV, peak beam current 40 mA, pulse length 1 ms,
beam power on the mercury target 520 kW.
(
40. ->
>-
A #
6 :-0 5
60 mA
LP
SP
Funnel
CCDTL CCL1 CCL2
IS RFQ Chopper DTL
114 mA
2 x 57 mA
SP
100 MeV 252 MeV 1 334 MeV
60 mA
2.5 MeV 20 MeV
LP
280 MHz 560 MHz
770 m
A (6 # 3
8 :- 5
60 mA
LP
RFQ
Chopper
SP
Funnel
RFQ
DTL
DTL SCL1
CCL SCL2
RFQ DTL
LP H+
114 mA
2 x 57 mA
SP
85 MeV 185 MeV 450 MeV 1 334 MeV
5 MeV
2 MeV
20 MeV
LP
352 MHz 704 MHz
430 m
3
43. ''
Test Modules
G
-68-I 2$ 0> <
A! E
Accelerator based neutron source 8B . *8G B . *8G B A3:
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using the D-Li stripping reaction
G5 B
intense neutron flux with the
5 . 76 5
appropriate energy spectrum
)= 5*
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44. 2.
5 !
5
1. Injector 3. DTL
O. Delferriere (Cea) N. Chauvin (Cea)
IFMIF
accelerator
PROTOTYPE accelerator
Simulations all along the linac
from source to target/beam dump
2. RFQ 5
4. HEBT
5 -
57 . Gquot;
C. Oliver (Ciemat)
M. Comunian (Infn)
33
53. n.c. DTL replaced by s.c. HWR DTL
MS 4 cryomodules
LEBT
Li
Target
s.c. HWR Linac
Ion source RFQ
G 55 .
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-
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5H
. Cryomodules 1 2 3&4
Cavity β 0.094 0.094 0.166
Cavity length (mm) 180 180 280
Beam aperture (mm) 40 40 48
Nb cavities / cryostat 1x8 2x5 3x4
Nb solenoids 8 5 4
. . P 3/ 25
6 # Cryostat length (m) 4.64 4.30 6.03
Output energy (MeV) 9 14.5 26 / 40
B P 3 6 55
6(
54. $ * 5& H
4 !R
peak surface fields sufficiently reduced
Geometry optimisation
(determine the maximum reachable accelerating field)
Ep/Eacc=4.4 & Bp/Eacc=10.1
Tuning method chosen: plunger at the opposite of the coupler port,
in a region of high electric field (tuning range easily achieved)
Tuning system actuator
beam
Cavity with Helium vessel Power coupler
63
55. $ * 5 . *
Vacuum tank
He phase separator
Tuning system
Collecting volume:
large enough to well
separate gas and liquid
Exhaust pipes :
diameter & path for
He 2-phase flow
Cavity Supply pipe + tank :
minimum pressure drop
Support
Coupler Horizontal supply pipe:
diameter large enough to be
quasi isobaric on its length
Solenoid magnetic design with passive shielding
! quot;
On-axis field profile
with passive shielding
! quot;
66
56. B E$ A
•
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9 .-
&' . 150
Cavity Power (kW)
125
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75
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50
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8 x 200 kW 2 x 105 kW 8 x 105 kW 12 x 200 kW
RF Chains RF Chains RF Chains RF Chains
175 MHz
INJ RFQ MS CM 1 CM 4
100 keV 5 MeV 9 MeV 40 MeV
6
57. RF System implementation
A 5- 5 45 .4 !
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195MHz 175MHz
Timing Systems
(Digital + Analog) Vacuum & Arcs Interlocks
Host PC Windows
80 MHz
Pin
Digital I/O
cPCI Bus Switch
Digital Board
Analog
Analog
FPGA Front End
8 DACs
Front End 8 ADCs
Digital IQ Demodulation IQ Ctrl 80 MHz DC
80 MHz 175 MHz
Up
and Control Loops
Down
Conversion
Conversion
Tuning Loop
IF
175 MHz
RF Reflected Circulator Voltage 1 (175MHz)
RF Reflected Cavity Voltage 1 (175MHz)
RF Forward Cavity Voltage 1 (175 MHz)
CAVITY
RF Cavity Voltage 1 (175 MHz)
RF Reflected Circulator Voltage 2 (175MHz)
RF Reflected Cavity Voltage 2 (175MHz)
RF Forward Cavity Voltage 2 (175 MHz)
CAVITY
RF Cavity Voltage 2 (175 MHz)
68
58. HEBT & Beam Dump - P. A.
B E$ A
H25 5 -
H -P*
> 5 4.
; 5
H ;E *
55 F7 .
Beam Dump @ < 88 I
7- G 5quot; 5
H *5 VM( 5B / 5
M6
1! / VM(5
movable Gamma shield
H 5
4 F 55 !
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5 *
H 5.
7 5.
cooling system
Beam
4! .
AM Y M 4 65#
S
Water shield tank
γ*
H *5E ; *F
) )
Beam Dump Cartridge
6
59. Beam Instrumentation
B E$ A#
Objectives
linac tuning & commissioning
beam loss minimization
beam characterization (emit, energy)
Current, Position, Profile monitors
Beam Loss, Halo, bunchlength
Diagnostics Plate
Detector : microstrips, grid
specific beamline for a set of diags resistors for uniform electric field
installed at 2 different locations
(downstream RFQ and downstream DTL)
Beam Transverse Profilers
2 types are developed (ionization & fluorescence) R&D started
6
60. 3 B 4
beam intensity : 125 mA
resolution ~ 0.1-0.3 mm
non interceptive diag
residual gas ionization
Detector : microstrips, grid
resistors for uniform electric field
beam profile
1st proto test on Silihi source at Saclay
Eproton = 75 - 95 keV 1 s (32 pads = 40 mm)
I < 100 mA (cw or pulsed - test < 12 mA)
trigger signal
61. the P.A. of the EVEDA phase
' B''
8 . * *
H * &
• Ion Source & LEBT
• RFQ & MS
• Cryomodule
• transport line to
• 1.12 MW beam dump
• 175 MHz RF system
• Cryogenic plant
• beam instrumentation