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1 Compressed Baryonic Matter at FAIR:JINR participation Hadron Structure 15, 29 th June- 3 th July, 2015 P. Kurilkin on behalf of CBM JINR group VBLHEP,

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Presentation on theme: "1 Compressed Baryonic Matter at FAIR:JINR participation Hadron Structure 15, 29 th June- 3 th July, 2015 P. Kurilkin on behalf of CBM JINR group VBLHEP,"— Presentation transcript:

1 1 Compressed Baryonic Matter at FAIR:JINR participation Hadron Structure 15, 29 th June- 3 th July, 2015 P. Kurilkin on behalf of CBM JINR group VBLHEP, JINR ITEP, Moscow

2 Introduction: CBM physics case and observables. Experimental requirements. JINR participation in CBM experiment: SC dipole magnet. Muon detection system. Development of STS. TRD. Methods and algorithms for global tracking. Study of multiparticle dynamics at CBM. Conclusion. Outline 2

3 The CBM Collaboration: 59 institutions, 500 members

4 Charm production and propagation at threshold energies  excitation function in p+A collisions (J/ψ, ψ', D 0, D  )  charmonium suppression in cold nuclear matter The equation-of-state at neutron star core densities  collective flow of hadrons  particle production at threshold energies (multi-strange hyperons) Onset of chiral symmetry restoration at high  B  in-medium modifications of hadrons ( , ,   e + e - (μ + μ - )) New /mixed phase of strongly-interacting matter  excitation function and flow of lepton pairs  excitation function and flow of strangeness (K, , , ,  ) Strange matter  (double-) lambda hypernuclei  strange meta-stable objects CBM physics case and observables at SIS100 4 https://www.gsi.de/documents/DOC-2009-Sep-120-1.pdf

5 10 5 - 10 7 Au+Au reactions/sec determination of displaced vertices (σ  50  m) identification of leptons and hadrons fast and radiation hard detectors free-streaming readout electronics high speed data acquisition and high performance computer farm for online event selection 4-D event reconstruction Experimental requirements 5

6 Time of Flight Projectile Spectator Detector DAQ/FLES HPC cluster Dipole Magnet Silicon Tracking System Experimental requirements Micro Vertex Detector Ring Imaging Cherenkov Transition Radiation Detector (4/12) Muon Detector

7 Study of multi-particle dynamics in heavy ion collisions at CBM Design and production of SC dipole magnet Development, design and production of a straw tube tracker prototype Development of methods and algorithms for global tracking R&D, beam tests JINR participation in CBM 7

8 Steps after CBM Dipole Magnet TDR approval approved in 2014 Technical Design Report for CBM superconducting dipole magnet was approved in the final form 2014 year. This document is a good base for the further work on the design of the magnet and preparation of the FAIR-JINR contract. 1. First meeting on the contract documentation preparation took place at GSI in April 2014. A lot of work during last year. Now we have draft of the specification for the FAIR-JINR contract. 2. Works on the further design of the magnet, cryostat, support as well as on quench and magnetic field calculations were continued at JINR and GSI. 3. Seach for the potential manufactors of the different CBM magnet parts: coils, cryostats and magnet yoke was very active. 8

9 9 FAIR-JINR Contract is in preparation CBM Superconducting Dipole Magnet

10 The magnet weigth - 150 t The beam axis from the floor - 2600 mm The height of the support - 750±20 mm The support points - 3 The maximal load on point - 85 t The vertical adjustment - ±20 mm The horizontal adjustment - ±20 mm The adjustment process is divided on two main stages: horizontal and vertical movements. The magnet support CBM Superconducting Dipole Magnet 3 roller skid for horizontal adjustment 3 hydraulic jacks for vertical adjustment 10

11 CBM Superconducting Dipole Magnet (quench protection) 11

12 The CBM Muon Detection System Stations 4 & 5: straw-tube tracker Institutions: Indian muon consortium (12 Univ. and labs), PNPI Gatchina, JINR Dubna Funding: FAIR contributions (India, Russia) TDR: is in progress (will be resubmitted in 2014) 12

13 Development of the Silicon Tracking System for CBM Sensor development: Double-sided microstrips 60 μm pitch, 300 μm thick, read- out via ultra-thin micro-cables STS in thermal enclosure (-10 o C) Detector layers: Low-weight carbon structures Institutions: GSI, JINR, KRI SPb, SPbSPU, AGH Krakow, JU Krakow, Moscow St. U, KINR, U Tübingen, industrial partners (Erfurt, Kharkov, Minsk, …) Funding: FAIR contributions (Germany, Russia, Poland), German BMBF Univ. funds, TDR is approved. Many FAIR – Institutes Contracts 13

14 The CBM TRD (R&D for SIS300) Requirements: e/π discrimination of > 100 (p > 1.0 GeV/c) active area ~1000 m 2 (12 stations) rate capability up to 100 kHz/cm 2 position resolution about 200 μm Prototype detectors: no drift region thickness of gas volume ~1 cm Test of different small prototype TRDs at CERN Institutions: U Frankfurt, U. Heidelberg, U Münster, NIPNE Bucharest, JINR Dubna Funding: German BMBF Univ. funds, Romanian FAIR contribution TDR: internal report in progress 14

15 15 Development of methods and algorithms for global tracking Development of the algorithms and software for track and ring reconstruction in MUCH, TRD, RICH, MVD detectors as well as global track reconstruction. Track reconstruction method is based on the track following and Kalman filter procedures. Ring reconstruction is based on the Hough Transform method. Feasibility study of the J/ψ→e + e - decay in AuAu collisions using developed software. FLES software development using different manycore CPUs and GPUs platforms. 4D event reconstruction (with time slices information). Data bases for CBM.

16 C 2 for high P T pions STS-TOF-RICH for pion ID STS-RICH for pion ID tritons deuterons Study of multiparticle dynamics at CBM at SIS100 16

17 Conclusions The CBM research program aims at the exploration of the structure of high density matter. For these purpose the advanced experimental setup will be build for high counting rate conditions expected at FAIR. JINR participated in the CBM project very actively and its contribution is large. The ultimative goal for 2016-2020 is to construct CBM detector to be ready for data taking at SIS100. Experience of the construction of many elements of the CBM (the Superconductive Dipole Magnet, MUCH,STS ) is used for the BM@N at the external Nuclotron beams and MPD (NICA). 17

18 18 Thank you for the attention!


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