Mikhail Itkis

105th Session of the JINR Scientific Council

Preparation of the seven-year programme for the development of

JINR for 2010-2016

Number of observed decay chains Element 118 3 Element 116 26 Element 115 4 Element 114 43 Element 113 2 Element 112 8

Heavy Ion

Physics

The basic role in realization of the plan of researches is associated with creation of accelerator complex DRIBs-III.

The purpose of the project is expansion of a set of accelerated ions, both of stable, and radioactive isotopes, essential increase of intensity and quality of beams.

Realization of project DRIBs-III provides:

• a new experimental hall,•development of new generation experimental set-ups,•completion of modernization of cyclotrons U400 and

U400М, •new high-intensity universal accelerator of heavy ions.

Heavy ion Physics – Basic Facilities

1. Modernization of accelerator U400M.The basic purposes of the modernization started in 2007 are: increase of

intensity of light ion beams by a factor of 4 – 5, increase of the maximal energy of light ions up to 100 MeV/A and, acceleration of lowered (6 – 15 MeV/A) energy ions, increase of stability of parameters of beams, extraction of beams in the second direction.

2. Modernization of accelerator U400.The basic purposes of planned in 2010 – 2011 modernization of the

accelerator are: improvement of quality and intensity of stable and radioactive beams, providing of a smooth variation of energy of ions in the range 0.8 – 25 MeV/A, decrease in the consumption of rare isotopes, decrease in power consumption by a factor of 3 – 4.

3. Development of highly effective multi charged ion sources

Heavy ion Physics – Basic Facilities

New FLNR experimental hall

The small area of the existing U400 experimental hall (nearby 150 м2) does not allow to place new experimental set-ups and leads to significant losses of time due to impossibility to work on another set-up if an experiment is running on one of them.

For the radical solving of this problem construction of a new experimental hall having the area 2500 м2 is planned. It will be used for work with beams of radioactive and exotic nuclei using new experimental set-ups, including those from other research centers.

Heavy ion Physics – Basic Facilities

43

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12 метров

226

224

223

222

221

220

219

218

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2600м2

New FLNR experimental hall

New high-intensity accelerator of heavy ions

Principal cause demanding creation of the new accelerator, is the impossibility of essential increase in intensity of beams of accelerated ions on existing accelerators (even after their modernization) owing to problems with injection into and extraction of ions from the accelerator. It should have an opportunity of stand-alone operation; work as the driver accelerator for producing ions of radioactive isotopes, and as postaccelerator in DRIBs-III complex; produced beams should be transported to available experimental halls. It is necessary to provide acceleration of ions from carbon up to uranium up to energy 5 – 10 MeV/A with stepwise and smooth variation. For ions with masses A<100 the beam intensity should be not below 5·1013/s.

Heavy ion Physics – Basic Facilities

Main components:Main components:

• Room temperature RFQ and IH-DTL at 108 MHzRoom temperature RFQ and IH-DTL at 108 MHz

• Superconducting CH-DTL (324 MHz) and QWR (108 MHz)Superconducting CH-DTL (324 MHz) and QWR (108 MHz)

Main components:Main components:

• Room temperature RFQ and IH-DTL at 108 MHzRoom temperature RFQ and IH-DTL at 108 MHz

• Superconducting CH-DTL (324 MHz) and QWR (108 MHz)Superconducting CH-DTL (324 MHz) and QWR (108 MHz)

Possible solution for a new acceleratorPossible solution for a new accelerator(proposed by GSI and University of Frankfurt)(proposed by GSI and University of Frankfurt)

Possible solution for a new acceleratorPossible solution for a new accelerator(proposed by GSI and University of Frankfurt)(proposed by GSI and University of Frankfurt)

0 5 10 15 20

Z / m

Energy MeV/u

1.8 2.4 3.3 4.2 5.2 6.1 7.1

CH DTL, supercond.324 MHz 108 MHz

DebuncherIH DTL,108 MHz

1.40.30.003

25 30

RFQ,108 MHz

ECR source

QWR Cavities

cyclic or linear? “cold” or “warm”?cyclic or linear? “cold” or “warm”?cyclic or linear? “cold” or “warm”?cyclic or linear? “cold” or “warm”?

next generation experimental set-ups

•Universal gas-filled separator for synthesis and studying of properties of SHE;

•Preseparator for radiochemical and mass-spectrometric researches; •Cryogenic detector for studying chemical properties of SHE;•Systems for collecting and production of single-charged ions in gas media

(gas catcher);• Radiochemical laboratory of II class;•Separator of radioactive neutron rich nuclei for RIB production;•Spectrometer for studying reactions induced by RIBs;•Wide aperture spectrometer of fission fragments

Heavy ion Physics – Basic Facilities

187 189 191 193

41 .0%

1.64%

16 .1%

13 .3%

26 .4%

195 197

41 .0%O s - iso topes at the focal p laneof M ASHA

Fra

ctio

n%

187 189 191 193

41 .0%

1.64%

16.1%

13.3%

26.4%

Isotope m ass num ber195 197

41.0%O s - iso topes at the focal p lane

of M ASHA

Fra

ctio

n%

Q 1 Q 2

Q 3

D1

D 2

D 3A

D 3BS1

S2

0 1 2 m

Q 1 Q 2

Q 3

D 2

D 3A

D 3BS1

S2

intermediate focus

beam

focal plane

Detector

array

SC D0

Gas Catcher

MASHA

M A S H AM A S H A

1. Synthesis and studying of properties of superheavy elementsIn 2010-2016 efforts will be concentrated on further more detailed studying of

already opened isotopes of superheavy elements, and also on search of new methods of synthesis of heavier elements. Planned experiments will be aimed at synthesis of nuclei with Z=110–120 in reactions between 232Th, 236,238U, 237Np, 242,244Pu, 241,243Am, 246,247,248Cm, 249Вк and 249Cf with 36S, 48Ca, 50Ti, 58Fe and 64Ni.

The significant attention will be given to synthesis of an element with Z=117.2. Characteristics of the spontaneous and induced nuclear fissionMechanisms of formation and decay of heavy and superheavy nuclei in

reactions with heavy ions will be studied on CORSET (+ DEMON +HENDES) and FOBOS set-ups which allow to study mass-energy distributions of fission fragments, preequilibrium, pre- and post scission neutrons, and also multiplicities and energy of γ-quanta

3. Chemical properties and identification of superheavy elementsFor the comparative studying of chemical properties of superheavy

elements and their light homologues compounds methods of gas phase termohromatography, and also methods of an ionic exchange and extraction from solutions are applied.

4. Mass spectrometry of isotopes of superheavy elementsFor precision measurement of masses and studying of physical and chemical

properties of these elements separator MASHA at the beam of the modernized cyclotron У400М will be used. In experiments with the use of a plasma ion source for isotopes of Kr, Xe and Hg at the test bench the mass resolution Δm/m≈3 10∙ -4 has been reached. The «MASHA» set-up considerably surpasses known similar devices by efficiency of separation of superheavy atoms and completeness of the information on characteristics of their decay.

5. Nuclear spectroscopy of isotopes of heavy and transfermium elementsTogether with IN2P3 (France) will proceed the realization of the project GABRIELA on α-, β- and γ-spectroscopy of transfermium isotopes with the use of the separator VASSILISSA.

6. Mechanisms of reactions with stable and radioactive nucleiExperiments with beams of radioactive isotopes will be carried out on ACCULINA set-up. Secondary beams of ions 6,8He, 9,11Li, 12,14Be, 8B with energy in the range 25-35 MeV/A are produced by irradiation of targets with primary beams of 7Li, 11B, 13C, 15N and 18O ions, generated by the cyclotron U400М. For ions 6He and 8He with the energy 25 Mev/A intensities of 1.5106 and 7103 particles/s were reached. Mechanisms a nucleon-nuclear interactions at energy in the near to Fermi's domain are studied on a fragment separator COMBAS allowing also to produce secondary beams of neutron rich nuclei with 2≤ Z≤11

FundingFunding22010010 22011011 22012012 22013013 20142014 22015015 201620165.05.0 11.011.0 11.011.0 11.011.0 16.016.0 3.03.0 3.03.0

60.060.0

Modernization of existing heavy ion accelerators:Modernization of existing heavy ion accelerators:building of complete set of equipments and building of complete set of equipments and manufacturing of U400R systems manufacturing of U400R systems

2.02.0

installation, adjustment of systems, launching of installation, adjustment of systems, launching of U400RU400R

1.01.0

Supporting of running experimentsSupporting of running experiments 1.01.0 1.01.0 1.01.0 1.01.0 1.01.0 1.01.0 1.01.0Creation of a new FLNR experimental hall:Creation of a new FLNR experimental hall:technical requirements, projecttechnical requirements, project 1.01.0civil workcivil work 55.0.0 55.0.0gallery, beam linesgallery, beam lines 2.02.0Development and creation of next generation Development and creation of next generation long acting experimental set-ups: "physical" and long acting experimental set-ups: "physical" and "chemical" separators, systems of collecting and "chemical" separators, systems of collecting and transport of nuclear reaction products, transport of nuclear reaction products, radiochemical laboratory of II-class, etc.radiochemical laboratory of II-class, etc.

1.01.0 3.03.0 2.02.0 2.02.0 3.03.0 2.02.0 2.02.0

New high-intensity heavy ion acceleratorNew high-intensity heavy ion accelerator

((AA≤100, ≤100, EE≤10 ≤10 MeVMeV··AA, , II≥10 ≥10 ppµµAA))technical requirements, projecttechnical requirements, project 1.01.0manufacturingmanufacturing 3.03.0 6.06.0 10.010.0installationinstallation, , beam lines, launchingbeam lines, launching 2.02.0Development of a FLNR experimental base for Development of a FLNR experimental base for radiation-physical and radioisotopic researchesradiation-physical and radioisotopic researches Performance of works under orders and contractsPerformance of works under orders and contracts

Δ

νe νµ ντ

I inverted hierarchy

Δ12

Δ

Δ12

N normal hierarchy

δ=π

23eV102,5

25eV107,7

)limit (Chooz

132 0.04)(θsin

1501322

sin .)θ(

?

23

m

22

m

21

m

21

m

22

m

23

m

?

0

δ=0

?

δ=0

δ=0

δ=π

δ=π

δ=0

δ=π

2e

m

2,

m

2e

m

250 meV

Neutrino

Neutrino

physics and

physics and

rare rare

phenomena

phenomena

Present Limits: T1/2() > 5.8 1023 yr (90 % CL) <m> < 0.6–1.3 eV

Expected 2009-2010: T1/2() > 2.0 1024 yr (90 % CL) <m> < 0.3 –0.7 eV

NEMO 3 Experiment

100Mo 6,914 кг Q= 3034 кэВ

82Se 0,932 кг Q= 2995 кэВ

116116CdCd 405 405 гг QQ= 2805 = 2805 кэВкэВ

9696Zr 9,4 Zr 9,4 гг QQ= 3350 = 3350 кэВкэВ

150150Nd 37,0 Nd 37,0 гг QQ= 3367 = 3367 кэВкэВ

4848Ca 7,0 Ca 7,0 гг QQ= 4272 = 4272 кэВкэВ

130130TeTe 454 454 гг QQ= 2529 = 2529 кэВкэВ

CuCu 621 621 гг

From NEMO 3 to Super NEMOFrom NEMO 3 to Super NEMO

100100MoMo 150150Nd or Nd or 8282SeSe

7 kg7 kg 100-200 kg100-200 kg

8% efficiency8% efficiency 30% efficiency30% efficiency

8%@3MeV8%@3MeV 4%@3MeV4%@3MeV

T1/2() > (1-2) x 1026 ans<m> < 0.06 - 0.10 eV

2011 – First Module in place of NEMO 32012-2014 – Installation in New Laboratory

Startup of experiment at Startup of experiment at Gran Sasso underground Gran Sasso underground laboratory in 2009. laboratory in 2009.

Phase 1:Phase 1: 2009-20112009-2011

~17.9 kg ~17.9 kg 7676GeGe enriched detector enriched detector

TT1/21/2 > 3 > 3 xx10102525

mmνν < 0. < 0.2-0.5 eV2-0.5 eV

(definite test of KKGH result) (definite test of KKGH result)

Phase 2: 2012-2016

~40 kg 76Ge

mν < 0.07-0.2 eV

GERDA: Search for 0νββ in 76Ge detectors

Search for Neutrino Magnetic Search for Neutrino Magnetic MomentMoment

GEMMA experimentGEMMA experiment

Experiment at Kalinin Nuclear Experiment at Kalinin Nuclear StationStation

Power of 3 GWPower of 3 GW On/OffOn/Off. 315. 315/50/50 daysdays Distance from reactor coreDistance from reactor core

– 14– 14,,5 м5 м 70 м70 мwe overburden we overburden

GEMMA II 2009 - 2010GEMMA II 2009 - 2010 ~~ 6,0×1013 6,0×1013 / cm2 / s / cm2 / s t ~ 2 years t ~ 2 years

B ~ 0,2 keV -1 kg -1 day-1 B ~ 0,2 keV -1 kg -1 day-1

m ~ 6 kg (two detectors)m ~ 6 kg (two detectors) TTthth ~ 1,5 keV ~ 1,5 keV

GEMMA IIIGEMMA III m ~ m ~ 20 kg , 20 kg , Tth ~ Tth ~ 100 eV100 eV

1,5 10 -11 B

~ 5 10 -12 B

8 cm (10X0)

Pb ES ESPb

x~ 5 mrad x~ 0,5 m

emulsion “grains”

track segment

44 200 44 (m)

1 mm

~15 grains/50 m

e , h

e,

decay “kink”

>25 mrad

OPERA ECC brick

152000 bricks in total

OPERA: Direct search for OPERA: Direct search for ννμμ→→ννττ oscillationsoscillations

Precision studies of rare muon and pion Precision studies of rare muon and pion decaysdecays

Present Limit:

<1.2·10-11

Plans• Present data taking to reach 10-13 • Obtain a “significant” result before the LHC era • Eventual reach of 10-14 during LHC era

UHECR and Dark Matter UHECR and Dark Matter SearchSearch

EDELWEISS-II : Search for Weakly Interacting Massive Particles (WIMP) with cryogenic Ge detectors at 20 mK, used for calorimetric and ionization measurements.

Present limit: ~10-6 pb

Expected by 2012 : 4x10-9 pb.

UHECR and Dark Matter UHECR and Dark Matter SearchSearch

BAIKAL Physics issues:

• Search for local sources of high energy neutrinos (>15 GeV)

• Search for Weakly Interacting Massive Particles and Monopoles

• Search for neutrino fluxes of Ultra High Energies (>10 TeV)

1 Gt (km3) Detector, which will use new strings design and instrumentation

Neutrino&Rare Neutrino&Rare phenomenaphenomena

2010 2011 2012 2013 2014 2015 2016

Direct costs 800 1300 1800 2300 2300 2300 2300

NEMO3: Data taking for mν < 1 eV100 100

SuperNEMO: construction, installation, data taking for mν < 0.1 eV 300 400 500 300 200 200

GERDA1: Data taking for mν < 0.5 eV50

GERDA2: increase of detector and data taking for mν < 0.2 eV 100 100 100 100 100

Future Double beta decay searches 200 300 300

GEMMA2: μν<1.5x10-11μB 50

GEMMA3: Increase of detector and data taking: μν<5x10-12μB 100 100 100

EDELWEISS: 4x10-9 pb for WIMP cross section

50 50 50

EURECA: 10-10 pb for WIMP cross section50 300 400 400 400

BAIKAL: Data taking and construction of 1 Gt detector 50 100 100 100 100 100 100

OPERA: Data Taking: Search for ~10 τ-lepton events 150 200 200 200 200 100

Daya Bay: Construction, Data Taking: Search for θ13<10-2 150 100 100 100 100 100 100

Future CP and θ13 projects 300 300 300 400 500

BOREXINO: Data Taking: 5% measurement of 7Be flux, check of season variations of SN flux, search for geo, supernova neutrino 50 50 100 100 100 100 100

Rare decays: CP/PEN/MEG: Search for μ→eγ at 10-13 150 300 300

Future of Rare decays: Search for μ→eγ at 10-14 500 500 500 500

Nuclear P

hysics w

ith

Nuclear P

hysics w

ith

Neutrons

Neutrons

IREN- 2009 2015 Since June 2009 to Since June 2009 to start regular two-shift start regular two-shift operation for operation for experiments at beam experiments at beam #3 and gamma #3 and gamma producing target;producing target;

Average energy of the Average energy of the electrons 50 MeV;electrons 50 MeV;

Peak current 2.8 A;Peak current 2.8 A; Operation frequency Operation frequency

50 Hz;50 Hz; Beam power 1.4 kWBeam power 1.4 kW Pulse width 200 nsPulse width 200 ns Intensity some above Intensity some above

10101212 n/s; n/s;

Implementation of the Implementation of the nonmultiplying Unonmultiplying U target;target;

Average energy about Average energy about 200 MeV;200 MeV;

Peak current 5.0 A;Peak current 5.0 A; Operation frequency Operation frequency

150 Hz;150 Hz; Beam power about 30 Beam power about 30

kW;kW; Pulse width 200 ns;Pulse width 200 ns; Intensity about 7Intensity about 710101313

n/sn/s

Works 2009 2010 2011 2012 2013 2014 2015 2016 Σ

Engineering infrastructure 20 70 130 220 200 300 700 1100 2740

Maintenance and operation 40 70 130 170 220 240 270 300 1430

Accelerator control system 25 40 70 130 80 50 20 20 435

Vacuum system 25 30 75 90 50 50 50 50 420

Pneumatic transport system 87 0 0 0 0 0 0 0 87

Experimental pavilion 30 0 0 0 0 0 0 0 30

2-klystrons assembly 0 130 0 0 0 0 0 0 130

Second 2-klystrons assembly

0 0 180 120 0 0 0 0 300

Klystron modulators 0 0 50 150 570 590 110 0 1470

Uranium target 0 0 0 0 0 40 120 180 340

Total: 227 340 635 880 1120 1270 1270 1650 7392

2009

2010

2011

2012

2013

2014

2015

2016

Carrying out of the first experiments at IREN xDetermination of the weak interaction constants in P-violation experiments. Determination of the asymmetry at the level of 10-8.

x

Search for rare fission modes. Determination of the probabilities of exotic decay modes.

x x

Program on measurements of (n,p), (n,) total, partial and differential cross sections for astrophysics, nuclear data etc. 2-3 isotopes/year.

x x x x x x x

Search for neutron resonances with different structure of the wave function, for various isotopes.

x x x x x

Search for deuteron singlet state. Determination of its life-time or setting the upper limit.

x

Obtaining of nuclear data for reactor and construction materials. x x x x x x x

IREN- Studies of neutron-induced nuclear reactions

2010

2011

2012

2013

2014

2015

2016

Direct measurement of the n-n scattering amplitude with accuracy 5-10%.

x

Investigation of the effect of accelerating matter in neutron optics, in particular with giant acceleration g ~105.

x

Verification of the weak equivalence principle for the neutron with accuracy 10-4 at first stage / 10 -5 at the final stage.

x x

Measurement of double differential scattering cross sections for UCN and VCN at nanostructures. Development a new type of UCN sources.

x x

New type of measurement of the n,e scattering length. Determination of the n,e scattering length with accuracy ~2-3%.

x

IREN- fundamental properties of the neutron, UCN physics

2010

2011

2012

2013

2014

2015

2016

Total

 1

Fundamental studies of neutron-induced nuclear reactions

35 80 125 170 185 255 280113

0

2 

Investigation of the fundamental properties of the neutron, UCN physics

45 80 90 95 95 100 155 660

3 

Methodical works and applied research

65 110 155 210 255 275 315138

5

  Total  145 270 370 475 535 630 750317

5

Nuclear Physics with Neutrons – direct costs

Condensed M

atter

Condensed M

atter

Physics

Physics

IBR-2 pulsed reactor will continue to play its role as the IBR-2 pulsed reactor will continue to play its role as the JINR core basic facility for condensed matter researchJINR core basic facility for condensed matter research

Parameters

Reactor core

Main movable reflector

Additional movable reflector

Fuel PuO2

Active core volume 22 dm3

Cooling liquid Na

Average power 2 МW

Pulsed power 1500 MW

Repetition rate 5 s-1

Average flux 8·1012 n/cm2/s

Pulsed flux 5·1015 n/сm2/s

Pulse width

(fast / therm.) 215 / 320 μs

Number of channels 14

Results of Results of modernizationmodernization

New reactor elementsNew reactor elements Impact on reactor parametersImpact on reactor parameters

New compact core higher thermal neutron flux on the moderator surface (up to 1.5 times higher as compared to IBR-2)

Reduced speed rotation of movable reflector (MR)

increase of MR lifetime by a factor of 2.5,

higher safety level

Use of fuel pellets with central hole

increased burn-up depth up to 9 % (1.5 times longer service time)

Use of two safety blocks rea-lizing functions of fast and slow emergency protection system

Increase of reliability of the emergency protection mechanism, much simpler design of a stationary reflector

Use of rolling moderators easy change of moderators

Cold neutron moderators up to 25 times increase in cold neutrons flux

Main stages of the IBR-Main stages of the IBR-2M development 2M development iin n

2010-20162010-2016

20102010 completion of the theme - 0851

2011 – 20132011 – 2013new theme “ Development of the

cryogenic moderators complex and research of the IBR-2M characteristics”

after 2013after 2013 operational cost only

№ Works 2010 2011 2012 2013 Σ

1.Control and protection system

60 50 - 110

2.Technological equipment and materials

70 - - 70

3. System of radiation control 350 300 - 650

4.Installation and adjustment works

80 - - 80

5. Start-up and first power 100 50 50 200

6.Research of the IBR-2M characteristics

60 60

7.Cryogenic moderator complex, new refrigerator for moderator serving beams 4-6

300 175 380 330 1185

  Total : 960 575 490 330 2355

Required resources for the Required resources for the IBR-2IBR-2M M theme in 2010-20theme in 2010-20113, k$3, k$

Expenditures 2010 2011 2012 2013 2014 2015 2016 Σ

Annual repair 100 100 100 100 100 100 100 700

Start of creation of new movable reflector (MR-4)

100 100 500 500 1200

Renewal of old equipment

300 300 300 200 200 200 300 1800

Subcontracts 100 100 100 100 100 100 100 700

 Total : 500 500 500 500 500 900 1000 4400

IBR-2IBR-2M operating costs 2010-20M operating costs 2010-20116 (k$)6 (k$)

IBR-2MIBR-2M R&D activities R&D activities 2010-20162010-2016 (4 220 k$) (4 220 k$)

Simulation and optimization of the spectrometers of the IBR-2M reactor, development of methods of neutron spectrometry

Modernization of elements of spectrometers and exploitation of present equipment

R&D of novel neutron and X-ray detectors and DAQ, increasing of effectiveness of their application

Cryogenic investigations

R&D of cold moderators, installation and performance control of new equipment

Development of the network and computer infrastructure of the IBR-2M spectrometer complex (remote control, new network technologies, software, hardware)

Condensed Matter Physics at IBR-2M in Condensed Matter Physics at IBR-2M in 2010-20162010-2016 (total requirement 5 598.3 k$) (total requirement 5 598.3 k$)

Pri

ori

ty d

irec

tio

ns

of

res

ea

rch

Pri

ori

ty d

irec

tio

ns

of

res

ea

rch

I. Nanosystems and Nanotechnologies

II. Biomedical Research

III. Novel Materials

IV. Engineering Diagnostics. Earth Sciences

Fe(3-5 нм)

Сr(1-2 нм)

Directions for development of Directions for development of spectrometers complexspectrometers complex

1. First priority projects – creation of new high intensity diffractometer for microsamples DN-6, new multifunctional reflectometer GRAINS, upgrade of SKAT/EPSILON spectrometers complex (with external funding from BMBF)

2. Second priority projects – completion of the FSD diffractometer project, upgrade of the spectrometers HRFD, DN-2, YuMO, REMUR, REFLEX, NERA-PR, DIN-2PI

3. Development of the projects of new small angle neutron scattering spectrometer and neutron reflectometer with atomic resolution

4 Development of new neutron scattering methods for studies of structure and dynamics of nanosystems and novel materials

1 м

32 м8 м

Background chopper

Neutron guide

Detector system Layout of the new high

intensity diffractometer for microsamples DN-6 project

2010 2011 2012 2013 2014 2015 2016

1 DN-6 diffractometer project (1 670 th. $ ): fabrication and installation of mirror neutron guide fabrication and installation of detector system fabrication and installation of mechanical part fabrication and installation of electronics blocks

250 100

70

250 100 100

50

50 100 250

150

50 100 50

2 EPSILON/SCAT project: completion of neutron guide

new DAQ electronics

80 20

20

3 GRAINS reflectometer project (1646.3 th. $ ): fabrication and installation of neutron guide system fabrication and installation of mechanical part fabrication and installation of PSD detector fabrication and installation of sample holder unit

32.9

51

112.4

150

150 100 50

150

150 150 50

200 150 50

100

Planned financing schedule for the first Planned financing schedule for the first priority projects (k$)priority projects (k$)

RADIATIO

N

RADIATIO

N

BIOLO

GY

BIOLO

GY

Fields of research:

Research into the mechanisms of the genetic action of accelerated multi-charge ions and neutrons with different energies.

Study of the action of heavy particles and neutrons on the eye's lens and retina.

Research into the regularities of the biological action of accelerated heavy ions on the central nervous system.

Mathematical modelling of biophysical systems.

Radiation research.

LABORATORY OF RADIATION BIOLOGYLABORATORY OF RADIATION BIOLOGYLRB

Confocal CARS microscope

Ready for users by the end 2009

Total costs, k$: 1281 1455 1717 2019 2444 2889 3416

Staff wages fund 992 1171 1398 1651 2005 2387 2837

International collaboration 30 30 30 30 30 30 30

Material and equipment costs

93 115 139 170 209 256 314

Power consumption40 47 53 64 90 99 110

Operational expenses126 92 97 104 110 117 125

2010 2011 2012 2013 2014 2015 2016

RADIATION BIOLOGYRADIATION BIOLOGY

Theoretical

Physics

Theory of Elementary Particles D.Kazakov, O.Teryaev Nuclear Structure and Dynamics V.Voronov, A.Vdovin

Theory of Condensed Matter

and New Materials V.Priezzhev, V.Osipov

Modern Mathematical Physics A.Sorin, A.Isaev

Dubna InternationalAdvanced Schoolof Theoretical Physics (DIAS-TH) A.Sorin, V.Voronov

Theoretical support

Funding(k$)

4581.8 5168.8 5907.8 6669.8 7618.8 8610.8 9710.8

Staff 201 198 195 193 191 189 187

Salary (k$) 3700 4170 4835 5540 6425 7360 8400

Int. Sc. Coop. (k$) 250.8 250.8 250.8 250.8 250.8 250.8 250.8

Materials (k$) 121 153 182 209 233 260 280

Energy (k$) 180 205 220 240 260 280 310

Executive Expenses (k$)

330 390 420 430 450 460 470

Theory - costs

Concluding remarks Presented draft planning is based on the current vision

of the JINR budget for years 2010-2016, proposed to the Committee of Plenipotentiaries by JINR Directorate and based on the constantly increasing contributions of JINR’s Member States year by year. Security of the budget is of primary importance here.

Planed distribution of funds between topics and their financial profiles have to be made consistent with overall budget limitations.

It is clear that timely execution of presented tasks requires further concentration of human and material resources.

Fresh young personnel from Member States is highly welcome.

Thank you for your attention!