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C ompressed B aryonic M atter at FAIR:JINR participation

C ompressed B aryonic M atter at FAIR:JINR participation. P. Kurilkin on behalf of CBM JINR group. VBLHEP, JINR ITEP, Moscow. Hadron Structure 15, 29 th June- 3 th July, 201 5. 1. Outline. Outline. Introduction: CBM physics case and observables. Experimental requirements.

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C ompressed B aryonic M atter at FAIR:JINR participation

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

  2. Outline Outline • 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.

  3. The CBM Collaboration: 59 institutions, 500 members

  4. CBM physics case andobservables at SIS100 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, , , , ) Charm production and propagation at threshold energies  excitation function in p+A collisions (J/ψ, ψ', D0, D)  charmonium suppression in cold nuclear matter Strange matter  (double-) lambda hypernuclei  strange meta-stable objects https://www.gsi.de/documents/DOC-2009-Sep-120-1.pdf

  5. Experimental requirements • 105 - 107 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 performancecomputer farm for online event selection • 4-D event reconstruction

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

  8. Steps after CBM Dipole Magnet TDR approval 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 theFAIR-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. approved in 2014

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

  10. CBM Superconducting Dipole Magnet The magnet weigth - 150 t The beamaxis 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 magnet support 3 hydraulic jacks for vertical adjustment The adjustment process is divided on two main stages: horizontal and vertical movements. 3 roller skid for horizontal adjustment

  11. CBM Superconducting Dipole Magnet (quench protection)

  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)

  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 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 STS in thermal enclosure (-10oC)

  14. The CBM TRD (R&D for SIS300) Requirements: • e/π discrimination of > 100 (p > 1.0 GeV/c) • active area ~1000 m2 (12 stations) • rate capability up to 100 kHz/cm2 • 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

  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. Study of multiparticle dynamics at CBM at SIS100 STS-TOF-RICH for pion ID deuterons STS-RICH for pion ID tritons C2 for high PT pions

  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).

  18. Thank you for the attention! 18

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