THE DOUBLE-POLARIZED DD-FUSION EXPERIMENT + DETECTOR SYSTEM

Similar documents
Experiment POLFUSION

Petersburg Nuclear Physics Institute DOUBLE POLARIZED DD-FUSION. Status report

First experiments with the polarized internal gas target at ANKE/COSY

Status of the Source of Polarized Ions project for the JINR accelerator complex (September 2013)

POLARIZED DEUTERONS AT THE NUCLOTRON 1

Polarized Molecules: A new Option for Internal Storage-Cell Targets?

D- Charge Exchange Ionizer for the JINR Polarized Ion Source POLARIS

Møller Polarimetry on Atomic Hydrogen

Spin Filtering at COSY - First Results

Commissioning of the Polarized Internal Gas Target (PIT) of ANKE at COSY

RCNP cyclotron facility

Commissioning of RHIC p-carbon CNI Polarimeter 1 H. Huang 1, I. Alekseev 2, G. Bunce 1, A. Deshpande 1, D. Fields 3, K. Imai 4, V. Kanavets 2, K. Kuri

Polarised Gas Targets and Polarised Ion Sources for Accelerators

MIDAS-NA: MInimization of Destructive plasma processes in ECR ion source

Neutron Structure Functions and a Radial Time Projection Chamber

Møller Polarimetry in Hall A and Beyond

arxiv: v2 [physics.ins-det] 8 Feb 2013

Silicon Detectors. Particle Physics

Nuclear Fusion with Polarized Fuel

Progress of the interaction between e - and molecule in Fudan University

Hall-D Update. Eric Pooser. Joint Hall A/C Summer Collaboration Meeting 07/18/2015

Proton Polarimetry for the EIC

Background reduction by a getter pump around the ionization volume of a Lamb-shift polarimeter and possible improvements of polarized ion sources

Infrastructure of Thin Films Laboratory in Institute of Molecular Physics Polish Academy of Sciences

Polarimetry in Hall A

The Hermes Recoil Silicon Detector

Joint Institute for Nuclear Research. Flerov Laboratory of Nuclear Reactions. University Center LABORATORY WORK

Ion Implanter Cyclotron Apparatus System

Enhancement of an IEC Device with a Helicon Ion Source for Helium-3 Fusion

FARCOS Femtoscope Array for Correlations & Spectroscopy

Møller Polarimetry for PV Experiments at 12 GeV

First measurement of spinexchange collision cross section in the low temperature region

P-Carbon CNI Polarimeter Operation Experience

arxiv: v1 [physics.ins-det] 3 Dec 2018 Fast Interaction Trigger for the upgrade of the ALICE experiment at CERN: design and performance

Progress in April December 2007 Schedule in Jan. March 2008

The Cylindrical GEM detector for the KLOE-2 Inner Tracker

A Report On DESIGN OF NEUTRON SOURCES AND INVESTIGATION OF NEUTRON BASED TECHNIQUES FOR THE DETECTION OF EXPLOSIVE MATERIALS

MTV - S1183 Beam Time Summary. Performance test of MTV new detector : CDC. Yumi Totsuka. Department of Physics, Rikkyo University, Tokyo, Japan

Polarized ion source with nearly resonant chargeexchange plasma ionizer: parameters and possibilities for improvements

Electric Rocket Engine System R&D

Micro Pixel Chamber with resistive electrodes for spark reduction

CYCLOTRON DEVELOPMENT PROGRAM AT JYVÄSKYLÄ

arxiv: v2 [nucl-ex] 6 Oct 2008

Diamond Neutral Par0cles Spectrometer at JET and proposal for ITER

Development of a new MeV gamma-ray camera

Ion Beam Cocktail Development and ECR Ion Source Plasma Physics Experiments at JYFL

The EDM Polarimeter Development at COSY-Jülich

D1. TASCA Focal Plane Detector Setup (Physics) - first mounting and detector tests

Developments of the RCNP cyclotron cascade

MOCD223M Dual-channel Phototransistor Small Outline Surface Mount Optocouplers

Requirements for the Final Phase of Project 8

Long term performance of the COSY/Jülich polarized ion source

Electron screening effect in nuclear reactions and radioactive decays

Electron Beam Polarimetry: Status and Prospects. DIS 2005, Madison, April 2005 E. Chudakov (JLab)

Progress Report on the A4 Compton Backscattering Polarimeter

RITU and the GREAT Spectrometer

Dual Isotope Imaging with LaBr3:Ce Crystal and H8500 PSPMT

DUBNA CYCLOTRONS STATUS AND PLANS

Pulse Height Analysis System (PHA) designed for W7-X Presented by Monika KUBKOWSKA

The light nuclei spin structure from the hadronic interactions at intermediate energies

Research and Development for the ATLAS Forward Calorimetry at the Phase-II LHC

Møller Polarimetry for PV Experiments at 12 GeV

Design of a Sector Magnet for High Temperature Superconducting Injector Cyclotron

The Compton backscattering Polarimeter of the A4 Experiment

ARTICLE IN PRESS. Nuclear Instruments and Methods in Physics Research A

Hard Xray Diagnostic for Lower Hybrid Current Drive on Alcator C- Mod

Mass Determination of Rn and Hg isotopes using MASHA

Pulse-shape shape analysis with a Broad-energy. Ge-detector. Marik Schönert. MPI für f r Kernphysik Heidelberg

Introduction Polarimeters at MAMI Analysis Future Conclusion. Polarimetry at MAMI. V. Tyukin, Inst. of Nuclear Physics, Mainz, Germany

NGRM Next Generation Radiation Monitor new standard instrument for ESA

Formation of High-b ECH Plasma and Inward Particle Diffusion in RT-1

Peter Fischer, ziti, Universität Heidelberg. Silicon Detectors & Readout Electronics

Challenges in optics requirement and control of Storage Rings for Precision Measurement of EDM

pp physics, RWTH, WS 2003/04, T.Hebbeker

DATA ACQUISITION SYSTEM FOR THE TUNKA-133 ARRAY

arxiv:physics/ v1 3 Aug 2006

The ALICE Forward Multiplicity Detector from Design to Installation. Christian Holm Christensen

RANGE OF ALPHAS. Advanced Laboratory, Physics 407 University of Wisconsin Madison, Wisconsin 53706

KEK isotope separation system for β-decay spectroscopy of r-process nuclei

positron source EPOS - general concept - timing system - digital lifetime measurement

TIMEPIX3 First measurements and characterization of a hybrid pixel detector working in event driven mode

PoS(TIPP2014)033. Upgrade of MEG Liquid Xenon Calorimeter. Ryu SAWADA. ICEPP, the University of Tokyo

Luminosity measurement in ATLAS with Diamond Beam Monitor

Ion Polarization in RHIC/eRHIC

A CYCLOTRON TEST SITE FOR NEUTRINO EXPERIMENTS

Performance of a Si PIN photodiode at low temperatures and in high magnetic fields

Storage Ring Based EDM Search Achievements and Goals

Acceptance test of the AGATA Ge detectors

1. Polarimetry Strategy 2. Møller Polarimeter 3. Compton Polarimeter 4. Summary

X-ray fluorescence analysis - calibration of the X-ray energy detector

The Silicon Tracking System of the CBM experiment at FAIR

4-PIN PHOTOTRANSISTOR OPTOCOUPLERS

X-band Experience at FEL

Performance of the ANL ECR Charge Breeder. with Low Mass Beams. Investigations with low mass species. Review of charge breeder design

Prospects for a Storage Ring EDM-Facility at COSY

BALKAN PHYSICS LETTERS Bogazici University Press 15 November 2016 BPL, 24, , pp , (2016)

The heavy ion irradiation facility at KVI-CART

Status Report: Charge Cloud Explosion

EXPERIMENTS CHARACTERIZING THE X-RAY EMISSION FROM A SOLID-STATE CATHODE USING A HIGH-CURRENT GLOW DISCHARGE


Transcription:

Petersburg Nuclear Physics Institute THE DOUBLE-POLARIZED DD-FUSION EXPERIMENT + DETECTOR SYSTEM P. Kravtsov for the PolFusion collaboration 1

The experiment goal Investigation of 4-nucleons reaction with polarization of the both initial particles at 10-100 kev energy (center of mass). 3 He p d + d t + p 3 He + n d d t n 2

dd-fusion experiments Unpolarized beam, unpolarized solid target Unpolarized beam, unpolarised gas target Polarized beam, unpolarized solid target Polarized beam, unpolarized gas 3

The Quintet suppression factor QSF 1,1 0 1 9 2 0 1,1 4 1,0 0,0 2 1, 1 Direct experiment required! 4

PolFusion collaboration Petersburg Nuclear Physics Institute, Russia Forschungszentrum Jülich, Germany Cologne University, Germany University ITMO, St.Petersburg, Russia ABS, CELGAS students Polarimetry PolFusion POLIS KVI, Gronningen, Netherlands ABS Detector POLIS Exp. Hall Polarimetry Ferrara University, Italy Financial support: RSF (2014-2016) 5

The layout of the experiment 3 2+ He (0.8 MeV), 3 H + (1.0 MeV) d 0 (0.1 ev) ABS Ferrara (IUCF) ABS 16 I ~ 4 10 a t/s Target density ~ 2.7 10 a t/cm Vector polarization: ± 0.7 11 2 dd-polarimeter or LSP 25 2 Luminosity: 3.3 10 1/cm s count rate: ~ 120/h (30keV) 3 week beam time (60000 events) d 3 0 He d d 3 H d 0 (0.1 ev) LSP 2 n p Lamb-Shift Polarimeter e e d (1-32 kev) n (2.4 MeV), p (3.0 MeV) Ion source Polarized Ion Source Ion beam: I = 20 μa ( 1. 3 10 14 d/s) E beam = 32 kev Vector polarization: ± 0.7 6

Polarized ion source (POLIS) POLIS Ion current at the source up to 20uA Magnets power supplies Vacuum system problems Unstable beam New ionizer for energy up to 100keV 7

POLIS. New ECR Ionizer Atomic beam High voltage (100kV) Microwave 2.45GHz ~200W Uniform magnetic field (875G) Gradient magnetic field Helium for plasma ignition 8

Polarized atomic beam source (ABS) Ferrara ABS Dissociator upgrade Nozzle cooling Control system Vacuum system RF transition units 9

ABS nozzle cooling Stable temperature down to 55K 10

ABS. Dissociator upgrade New schematic for better matching with generator Geometry optimization of RF circuit Reflected power decreased from 150W to 3W (@250W) Two-channel RF matchbox with splitter to feed both dissociators from single generator 11

Polarimetry Normal operation POLIS Tuning ABS ABS POLIS Detector Deflector POLIS LSP Ioniser NRP LSP 12

Polarimetry. LSP ionizer Magnets (1000G) Extractor and focusing Ionizer cell Cathode 13

Polarimetry. LSP Na cell 14

Polarimetry. Deflector for NRP 15

Analysis The observables in the d+d -> 3 He+n and d+d-> 3 H+p reactions with polarized deuterons 16

Detector system design Readout electronics connectors Helmholtz coils NdFeB permanent magnets Detector system Detector chamber 17

Magnetic field, G Magnet system B =300 G = 2.5 Bc Magnet field is generated by 24 permanent magnets with dimensions 80х40х10 mm 3 with pole tip field of 1.25 T at the surface (NdFeB N40) 350 300 Btotal Btransverse 250 200 150 100 50 0-150 -100-50 0 50 100 150 Axis coordinate, mm 18

Detector system. PIN diodes version. 4- detector with 51% filling 576 Hamamatsu PIN-diodes (S3590-09) PIN-diode active area: 1 cm 2 depleted layer: 300 um energy resolution: <50keV low reverse voltage (<=50V) Square detector elements (4x4 diodes) Standard PCB assembly with spring through-hole mounting (no solder!) 19

Simulation of the detector system 20

PIN-diodes test bench Preamplifier Vacuum chamber Detector Bleeding valve O scilloscope a H 2 PC Turbopump Forepump Alpha-source: 239 Pu + 240 Pu = 80.4% 238 Pu + 241 Am = 19.6% 234 U + 235 U + 238 U 241 Am 21

PIN diode test measurements Dead layer thickness measurement (D 1μm) P. Monich. Bachelor thesis (ITMO university). Active area uniformity tests Inhomogeneity <0.5% for the whole active area Hydrogen vacuum performance Better 0.16% stability at hydrogen pressure of 10-4 mbar. Expected vacuum in the experiment 10-5 10-6 mbar. 22

Detector system assembly 23

Readout electronics Readout requirements: 600 channels Total count rate 1kHz Standard interface (Ethernet?) Event synchronization for coincidence trigger CSP from ATLAS CSC [BNL] Junnarkar et al. IEEE Nuclear Science Symposium Conference Record (2005) 48 channel Waveform digitizer (WFD) Concentrator Detector ADC FPGA FPGA 2x24-channel CSP Charge Sensitive Preamplifier + Shaper ASF-48 6 x 8-channel pipeline ADC 12 bit, 65MHz Self-triggered WFD 12 bit resolution count rate up to 50 khz 24

ASF48 readout board 25

Readout signal processing Benefits Precise analytical fit No baseline dependence Best resolution (<=5LSB) 26

Energy resolution Test pulse E=1000keV RMS=0.49%=4.9keV (15 kev with cable and C det =40pF) 27

Signal quality Signal quality checks: ADC range clipping Signal shape (derivatives) Peaks position 28

Solid target experiment Target: deuterated polymethylmethacrylate Deuteron beam 15keV ~5uA 03.02.2017 А. Васильев 29

Solid target results 50 3 2+ He t p 40 30 20 10 0 0 500 1000 1500 2000 2500 3000 3500 4000 30

Full scale readout electronics (ASF-48) Concentrator CROS3 Power distributor (5V 40A) ASF48 (12+1) 31

Optimizations (grounding, pickups ) 32

Data acquisition software ASF48 test software Full scale DAQ software based on MIDAS (Maximum Integrated Data Acquisition System) http://midas.psi.ch Flexible distributed DAQ system Web interface for run control and monitoring Data transfer / logging capability Online data monitoring Online database Message logging Alarms 33

Data acquisition software 34

Thank you! 35

36

BACKUP 37

Hyperfine states ABS 85% value HFS after HFS after MFT Sextupole 1 Sextupole 2 SFT WFT HFS after ABS Pz Pzz Pz Pzz Beam 1, 2, 3 --- 1, 2, 3 --- --- 1, 2, 3 +1/3-1/3 0.272-0.332 0 1, 2, 3 1-4 2, 3 --- --- 2, 3 0-1 -0.02-0.85 1 1, 2, 3 3-4 1, 2 --- --- 1, 2 +2/3 0 +0.561-0.02 2 1, 2, 3 3-4 1, 2 --- on 3, 4-2/3 0-0.561 +0.02 3 1, 2, 3 3-4 1, 2 2-6 --- 1, 6 +5/6 +0.5 +0.714 +0.434 4 1, 2, 3 1-4 2, 3 2-6 --- 3, 6 +1/6-0.5 +0.145-0.391 5 1, 2, 3 1-4 2, 3 3-5 --- 2, 5-1/6-0.5-0.145-0.459 6 HFS after Sextupole 1 MFT HFS after Sextupole 2 POLIS 75% value SFT WFT HFS after ABS Pz Pzz Pz Pzz Beam 1, 2, 3 --- 1, 2, 3 --- --- 1, 2, 3 0 0 0 0 0 1, 2, 3 1-4 2, 3 --- --- 2, 3-0.5-0.5-0.375-0.375 1 1, 2, 3 3-4 1, 2 --- --- 1, 2 +0.5-0.5 +0.375-0.375 2 1, 2, 3 3-4 1, 2 --- on 3, 4-1 +1-0.75 +0.75 3 1, 2, 3 3-4 1, 2 2-6 --- 1, 6 +1 +1 +0.75 +0.75 4 1, 2, 3 1-4 2, 3 2-6 --- 3, 6 0 +1 +0.02 +0.75 5 1, 2, 3 1-4 2, 3 3-5 --- 2, 5 0-2 -0.02-1.5 6 38

, mb Unpolarized cross sections 10 2 H d, n 3 He 2 H d, p 3 H 1 0.1 0 20 40 60 80 100 120 Ed, kev R. E. Brown, N. Jarmie, Phys. Rev. C 41 N4 (1990) 39