1 / 14

D. Novinsky (PNPI)

PSTP-2011.

nuwa
Download Presentation

D. Novinsky (PNPI)

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. PSTP-2011 PNPI polarized target for pion-nucleon scattering measurements at intermediate energies A.V Aldushchenkov, A.G. Dernyatin, A.I. Kovalev, D.V. Novinsky, I. Okunev, V.A. Shchedrov, V.V. Sumachev, V.Yu. Trautman. Petersburg Nuclear Physics Institute, Gatchina, Leningrad district, 188350, Russia.E-mail : dimanov@pnpi.spb.ruI.G. Alekseev, P.E. Budkovsky, V.P. Kanavets, L.I. Koroleva, B.V. Morozov, V.M. Nesterov, V.V. Ryltsov, D.N. Svirida, A.D. Sulimov.Institute for Theoretical and Experimental Physics, Moscow, 117218, Russia.N.A. Bazhanov, E.I. BunyatovaJoint Institute for Nuclear Research, Dubna, Moscow district, 141980, Russia. D. Novinsky (PNPI)

  2. Preface PSTP-2011 • The polarization parameters (P, R, A) measurement results above pion momentum above 1000 MeV/c made it possible to resolve part of discrete ambiguities in existing partial-wave analyses (PWA’s) • The polarization experiments at N-elastic scattering use the proton polarized target. • The experiment uses a polarized proton target in which free protons have vertical polarization or polarization in the elastic scattering plane. • Uncertainty (abs.) is ±~2% at 70% of polarization magnitude. • The area under the PMR curve is determined using a Q meter. D. Novinsky (PNPI)

  3. The physics goals PSTP-2011 D. Novinsky (PNPI)

  4. Experimental Setup, ITEP (Moscow) PSTP-2011 MAIN ELEMENTS: • Vertically polarized proton target PT • 4 sets of wire chambers for tracking • Trigger scintillation counters Beam Arm Pion Beam Proton Arm Pion Arm I TARGET: • Cylinder 30mm, h=30mm, propanediole C3H8O2, free proton density 10 % • Magnetic field 2.5 T • 3He evaporation type cryostat at 0.5 K • Dynamic nuclear orientation • Polarization (70-80) %, measurement accuracy ±2 % • Sign reverse once per day Pion Arm II D. Novinsky (PNPI)

  5. Cryostat in the vertical sectional view PSTP-2011 1 – helium-3 pump-out 2 – neck 3 – helium-4 pump-out 4,11 – nitrogen screens 5,21 – helium inputs 6– nitrogen tank 7– magnet 8 – window 9 – magnet frame 10 – housing 12 – indium compaction 13 – rotating tee-joint 14 – helium-4 output through current-input 15 – connection to current source 16 – current-input compaction and helium-4 output 17 – current-input 18 – helium tank (at 4.2 K) 19 – refrigerator 20 – appendix with target (C3H8O2) matter D. Novinsky (PNPI)

  6. Target: topview plane PSTP-2011 1 – target window, 2 – nitrogen screen, 3 – magnet area, 4 – container with the target (C3H8O2) matter inside superconductive Helmholz coils D. Novinsky (PNPI)

  7. Polarization measurements PSTP-2011 • polarization pumpby the dynamic nuclear orientation method up to absolute value 70–80% • method of proton magnetic resonance (PMR), • measurements are based on the calculations of square under the PMR curve: the system containing Q-meter with sequential contourand signal digitalization • Calibration is based on the equilibrium state at temperature 0.8 – 1.4 K D. Novinsky (PNPI)

  8. Polarization measurements PSTP-2011 • Signal and background • Background: to take away signal from center by means of the magnetic field change D. Novinsky (PNPI)

  9. Polarization measurements PSTP-2011 • Calibration: the equilibrium state D. Novinsky (PNPI)

  10. Electronic providing of the polarized target PSTP-2011 • Modernization of the target measurements • Two PCI-cards are inserted into the PC-board (Remote computer PC1 ). • Usage of PCI-card DAS6036 and the PCI-card PCI-1723 ADC and DAC with grade ≥ 14 bit, transformation is run by timer FIFO Transformation time ≤ 8 s • Usage of the new current source “Lambda-Genesys” for power supply of superconductive coils D. Novinsky (PNPI)

  11. Current situation PSTP-2011 • PCI-cards and programs are tested at PNPI • Current source is tested at PNPI and ITEP (Moscow) • Target location: ITEP • To continue spin rotation parameters mearurements, e.g. J-PARC • at PNPI accelerator • Cryostat at PNPI Netron Physics Department D. Novinsky (PNPI)

  12. Conclusions PSTP-2011 • Successful target work > 20 years • Modernization and new tests are required • New physics tasks • In memory of A.I. Kovalev (1936-2011) • More than 20 years experiments Acknowledgements • GREAT THANKS to the Organizing Committee ! ! ! D. Novinsky (PNPI)

  13. PCI-card PCI-DAS6036 PSTP-2011 • Low-cost, 16-channel, 200 kS/s analog I/O boards with two 16-bit analog outputs, eight digital I/O, and two counter/timers • 16 channels of 16-bit A/D resolution • 200 kS/s maximum sample rate • 2 channels of 16-bit D/A at 10 kHz • 8 bits DIO • 2 16-bit counters D. Novinsky (PNPI)

  14. PCI-card PCI-1723 (Advantech) PSTP-2011 • 16-bit, 8-channel Non-isolated Analog Output CardMain Features • Auto calibration function • A 16-bit DAC is equipped for each analog output channel • Synchronized output function • Output values retained after system hot reset • 2-port (16-channel) user-defined digital input/output • Board ID D. Novinsky (PNPI)

More Related