Title: Design and construction of
1Design and construction of Nuclotron-based Ion
Collider fAcility (NICA) and Mixed Phase Detector
(MPD)
Conceptual design proposal by AC WG-II
A.D. Kovalenko
ROUND TABLE DISCUSSION-2, JINR, Dubna, October 6-
7, 2006.
2NICA general layout by WG-II
NOTE THE IDEA TO CONSIDER ION COLLIDER BASED ON
THE NUCLOTRON WAS PUT FORWARD BY THE ACCELERATOR
WORKING GROUP II
- The possibility of fixed target experiments is
exist - The investigation of light and middle weight ion
collisions including polarized deuterons
(collision energy and luminosity will be larger
in the case) - The experiments at the internal target installed
inside one the collider rings can be considered
as well
ROUND TABLE DISCUSSION-2, JINR, Dubna, October 6-
7, 2006.
A.D. Kovalenko
3NICA cost schedule by WG-II
- Cost of the booster is based on the Nuclotron
project cost scaled as ratio of the lengths. - The collider rings cost is estimated based on the
LHC cost. The two main scale factors were used
ratio of the lengths (k1) and ratio of the
magnetic fields ( kB 2), i.e. CNICA CLHC /
k1kB 2 . Cost of RD, preparatory work, transfer
lines, injection and extraction systems,
radiation safety conditions unexpected works will
increase this cost by a factor of 2-2.5.
- The design and construction of magnets and
cryogenic systems of the both as booster and
collider can be made by JINR and JINR
member-countries. Part of special works on RF
system, fast kickers, special SC magnets and
some other systems should be performed by those
collaborating Laboratories who have more
experience in the mentioned directions.
ROUND TABLE DISCUSSION-2, JINR, Dubna, October 6-
7, 2006.
A.D. Kovalenko
4The essential cost saving factors
- No new buildings, no additional power supply
lines, heat, water cooling - The U-beam peak energy (2.5 GeV/u) used in the
colliding mode is much less than that was
discussed preliminary for fixed target
experiments (5-10 GeV/u) thus, the problems of
radiation safety will take less cost - The needed upgrade of the Nuclotron ring
including ion source has been considered and
presented within the project Nuclotron-M - The design of a fast-cycling superferric 84 m
booster for the Nuclotron was made earlier,
although the lattice should be redesigned based
on the new specification and the recent data
obtained at BNL, CERN and GSI - The JINR has a long-term experience in
superconducting cables and magnets design and
fabrication, thus magnet-cryostat systems of both
as booster and collider rings can be manufactured
by the Institutes workshops - Additional high capacity cryogenic plant is not
necessary.
ROUND TABLE DISCUSSION-2, JINR, Dubna, October 6-
7, 2006.
A.D. Kovalenko
5The existing Nuclotron facility
- The Nuclotron was built for five years
(1987-1992), the main equipment of its magnetic
system, and many other systems as well, was
fabricated by the JINR central and the LHE
workshops without having recourse to specialized
industry. The Nuclotron ring of 251.5 m in
perimeter is installed in the tunnel with a
cross-section of 2.5m x 3 m that was a part of
the Synchrophasotron infrastructure
- The main design criteria specified for the
Nuclotron construction were the following - Much less electric power consumption
- Substantial improvements of vacuum
inside a beam pipe - Faster ramp and longer flat top of the
magnetic field - Cost saving for materials and work
- Maximum use of the existing facilities
and infrastructure of the Synchrophasotron.
All the mentioned conditions were realized in
1987-93 within the project Replacement of the
Synchrophasotron magnetic system by a
superconducting one Nuclotron.
NOTE the injector (ion sources, linac upgrade,
booster) and slow extraction system as were not
included in the project due to lack of money
ROUND TABLE DISCUSSION-2, JINR, Dubna, October 6-
7, 2006.
A.D. Kovalenko
6ROUND TABLE DISCUSSION-2, JINR, Dubna, October 6-
7, 2006.
A.D. Kovalenko
7NUCLOTRON MAIN PARAMETERS
ROUND TABLE DISCUSSION-2, JINR, Dubna, October 6-
7, 2006.
A.D. Kovalenko
8SYNCHROPHASOTRON/NUCLOTRON ANNUAL RUNNIG TIME
ROUND TABLE DISCUSSION-2, JINR, Dubna, October 6-
7, 2006.
A.D. Kovalenko
9SEARCHING for the MIXED PHASE
ACCELERATOR RD GOAL DISCUSSED AT THE ROUND
TABLE-I Au, , U ion beams at the energies
above 5 GeV/u
- THE MAIN NECESSARY NUCLOTRON DEVELOPMENT
- ION SOURCE KRION
- VACUUM IN THE RING
- FIELD RAMP B ? 2 T/s
- LINAC LU-20 UPGRADE
- BEAM DIAGNOSTICS etc.
ROUND TABLE DISCUSSION-2, JINR, Dubna, October 6-
7, 2006.
A.D. Kovalenko
10Reaching 5 Gev/u for heavy ions ( A 200)
pc(GeV/cu) 0.3B?(z/A) (Tm), where ?
L(B)N/2p
Operation of the Nuclotron magnetic system at 2.2
T make it possible to reach 6.527 GeV/u if
z/A0.5. Thus, 5 GeV/u can be reached for z/A
0.383.
- The number of dipoles in the Nuclotron ring, N
96 - L(_at_2T) 1.396 m, ? 29.917 m and pc
12.55(z/A) - L(_at_2.2T) 1.385 m,? 21.17 m and pc 13.96(z/A)
ROUND TABLE DISCUSSION-2, JINR, Dubna, October 6-
7, 2006.
A.D. Kovalenko
11PROJECT NUCLOTRON-M
- The project include
- improvement of the beam pipe pumping system
- structural magnets power supply upgrade
- beam extraction system
- beam diagnostic and control system
- RF system
- beam transfer line from the Nuclotron ring to the
main - experimental area
- radiation shield ( F3 area mainly)
- cryogenic supply system
- ion source development
- booster magnets RD
The project Nuclotron-M has been prepared for
the approval procedure. The project cost is about
3.0 M USD for two years starting from 2007.
ROUND TABLE DISCUSSION-2, JINR, Dubna, October 6-
7, 2006.
A.D. Kovalenko
12Ion source KRION
- The improved EBIS-type ion source KRION is
chosen for generation of the primary beam of
highly charged state ions.
- We consider as practically feasible for
realization within the coming two years the new
ion source with 6 T solenoid and pulse
repetition rate of 5-10 Hz, i.e. (4-8)1010 U30
ions per second.
ROUND TABLE DISCUSSION-2, JINR, Dubna, October 6-
7, 2006.
A.D. Kovalenko
13NUCLOTRON HEAVY ION INJECTION SCHEME
LIMITATION by KRION higher charge
state lower intensity
LIMITATION from LU-20 Z/A gt 0.3
LIMITATION by the NUCLOTRON
single-turn injection ( 8.3 mks )
ROUND TABLE DISCUSSION-2, JINR, Dubna, October 6-
7, 2006.
A.D. Kovalenko
14Booster/Nuclotron/Collider
ROUND TABLE DISCUSSION-2, JINR, Dubna, October 6-
7, 2006.
A.D. Kovalenko
15Booster/Nuclotron/Collider
ROUND TABLE DISCUSSION-2, JINR, Dubna, October 6-
7, 2006.
A.D. Kovalenko
16FAST CYCLING BOOSTER
The maximum operating current was increased to 12
kA. The current ramp rate of 120 kA/s was
obtained at cycled operation at 3 Hz. Limitation
from the power supply voltage ( 40 V)
ROUND TABLE DISCUSSION-2, JINR, Dubna, October 6-
7, 2006.
A.D. Kovalenko
17BOOSTER
- The version is similar to that presented earlier
at ASC2000, EPAC2000 and EPAC2002. - The circumference of the booster ring is 1/3
of the Nuclotron. - The large aperture of both lattice dipole and
quadrupole magnets is one of the main design
features. - the magnet cold mass consisting of a SC-winding,
a beam pipe, a reinforcing shell and correcting
windings (if needed), is fabricated as a common
rigid unit separated from the iron yoke. - The yoke temperature of 80 K.
- The cold mass having a substantially lower weight
and surface and the cooled iron yoke are
suspended inside the cryostat, - The two substantial features should be realized
in the new design 1) pulse repetition rate of 5
Hz and 2) high level of vacuum in a beam pipe. - The possibility to construct superferric magnet
operating at 3-5 Hz have been demonstrated at our
Laboratory. The 80K yoke magnet models have been
tested also. The new 12 kA NbTi composite hollow
cable have been manufactured and tested. The new
booster lattice of DF-type is under
optimization. The maximum energy of the booster
should exceed 100 MeV/u to provide reasonable
(practically achievable) vacuum level in the
Nuclotron beam pipe.
ROUND TABLE DISCUSSION-2, JINR, Dubna, October 6-
7, 2006.
A.D. Kovalenko
18ROUND TABLE DISCUSSION-2, JINR, Dubna, October 6-
7, 2006.
A.D. Kovalenko
19NICA 4 T COLLIDER DIPOLE
THE CONCEPT OF HOLLOW CABLE COOLED WITH TWO-PHASE
HELIUM FLOW IS USED. NEVERTHELESS, THE SC WIRES
ARE DIVIDED INTO THREE ELECTRICALLY INSULATED
GROUPS.
ROUND TABLE DISCUSSION-2, JINR, Dubna, October 6-
7, 2006.
A.D. Kovalenko
20NICA OPERATION CYCLE COOLIG POWER
The total equivalent refrigerator load needed to
cool the NICA facility will be 3290 W at 4.5 K.
Taking into account also about 30 capacity
reserve, necessary equivalent capacity of the
refrigerators estimated to 4.3 kW at 4.5 K.
3 x 7 SC wires of 1.04 mm equivalent diameter
each. Io 5 kA, Ic 7.89 kA
ROUND TABLE DISCUSSION-2, JINR, Dubna, October 6-
7, 2006.
A.D. Kovalenko