Discussion ITPA-10 in Troitsk 11 of April 2006 (Neutron Working Group)

Slides:



Advertisements
Similar presentations
Time-of-flight measurement of ion energy Tim Freegarde Dipartimento di Fisica Università di Trento Italy.
Advertisements

S. Popovichev 10th Meeting of ITPA Topical Group on Diagnostics, Moscow, April Neutron yield measurements and absolute calibration issues.
W. Heidbrink, G. Kramer, R. Nazikian, M. Van Zeeland, M. Austin, H. Berk, K. Burrell, N. Gorelenkov, Y. Luo, G. McKee, T. Rhodes, G. Wang, and the DIII-D.
TOF spectrometers for measurement of n d /n t ratios K.Okada, T.Nishitani 2, K. Ochiai 2, K.Kondo 2, M.Sasao, M. Okamoto, K.Shinto, S.Kitajima Tohoku Univ.
Advanced GAmma Tracking Array
6 th ITPA MHD Topical Group Meeting combined with W60 IEA Workshop on Burning Plasmas Session II MHD Stability and Fast Particle Confinement General scope.
Experimental Status of Deuteron F L Structure Function and Extractions of the Deuteron and Non-Singlet Moments Ibrahim H. Albayrak Hampton University.
Cross section measurements for analysis of D and T in thicker films Liqun Shi Institute of Modern Physics, Fudan University, Shanghai, , People’s.
Precise neutron inelastic cross section measurements A.Negret 1 1 “Horia Hulubei” National Institute for Physics and Nuclear Engineering, Bucharest, ROMANIA.
FREE CARRIER ABSORPTION TECHNIQUES - MICROWAVE & IR –
D. Borba 1 21 st IAEA Fusion Energy Conference, Chengdu China 21 st October 2006 Excitation of Alfvén eigenmodes with sub-Alfvénic neutral beam ions in.
Spectrum Analyzer Basics Copyright 2000 Agenda Overview: What is spectrum analysis? What measurements do we make? Theory of Operation: Spectrum analyzer.
C Gormezano, S Ide ITPA SSO&EP IEA-LT/ ITPA Collaboration 1 Steady State Operation & Energetic Particles Advanced Scenario need the same development path.
Presented by Y. Kamada Large Tokamak Meeting June 2006 JT-60U contribution to ITPA/IEA inter-machine experiments and related study for ITPA/IEA.
Kaschuck Yu.A., Krasilnikov A.V., Prosvirin D.V., Tsutskikh A.Yu. SRC RF TRINITI, Troitsk, Russia Status of the divertor neutron flux monitor design and.
ITPA Diagnostics 4/06 The Importance of Fast-Ion Profile Measurements in ITER W. Heidbrink Three examples from DIII-D Conclusion Fast-ion D  (FIDA) Technique.
J A Snipes, 6 th ITPA MHD Topical Group Meeting, Tarragona, Spain 4 – 6 July 2005 TAE Damping Rates on Alcator C-Mod Compared with Nova-K J A Snipes *,
NEW COMMENTS TO ILC BEAM ENERGY MEASUREMENTS BASED ON SYNCHROTRON RADIATION FROM MAGNETIC SPECTROMETER E.Syresin, B. Zalikhanov-DLNP, JINR R. Makarov-MSU.
CAE/GAE modes – link to electron transport in MAST? A.R. Field 1, R.J. Akers 1, L. Appel 1, D. Dunai 3, H. Smith 2, M. Turnyanskiy, M.Valovic 1, E. Verwichte.
Direct Reactions with ORRUBA and GRETINA Steven D. Pain Oak Ridge National Laboratory GRETINA Workshop, ANL, February 2013.
1 Atomic Emission Spectroscopy Lecture Advantages of Plasma Sources 1.No oxide formation as a result of two factors including Very high temperature.
9th ITPA Confinement Database and Modelling Topical Physics Group meeting in St. Petersburg 1/5 NF paper on H-mode confinement DB3 Darren McDonald.
ITPA-Moscow Role of neutron emission spectrometry on ITER and instrumental requirements Göran Ericsson E.Andersson Sundén, A.Combo 2), S.Conroy,
1 ITPA St Petersburg April 2009G.Gorini JET results on the determination of thermal/non-thermal fusion yield from neutron emission spectroscopy.
Discussions and Summary for Session 1 ‘Transport and Confinement in Burning Plasmas’ Yukitoshi MIURA JAERI Naka IEA Large Tokamak Workshop (W60) Burning.
V.Grishin, A.Koshelev, A.Larionov A.Pushkarev, V.Seleznev, M.Sleptsov A.Sytin.
Neutron inelastic scattering measurements at the GELINA facility of EC-JRC-IRMM A. Negret 1, C. Borcea 1, A. Plompen 2 1 NIPNE-HH, Romania 2 EC-JRC-IRMM,
Tools for Discovery CAEN solutions for Diamond Detectors June 24 th 2011, Viareggio Giuliano Mini.
Studies on fast ion distribution Correlated with the spectroscopy diagnostics measurements Gerarda Apruzzese CRE Frascati.
Lawrence Livermore National Laboratory Nicholas Scielzo Lawrence Fellow Physics Division, Physical Sciences LLNL-PRES Lawrence Livermore National.
Active Beam Spectroscopy in Hot Fusion Plasmas (Introduction) Seminar-I Institute for Plasma Physics Academy of Sciences Hefei, China May, 5, 2007 Acknowledgement:
Pellet Charge Exchange Measurement in LHD & ITER ITPA Tohoku Univ. Tetsuo Ozaki, P.Goncharov, E.Veschev 1), N.Tamura, K.Sato, D.Kalinina and.
RF codes for Transp Transp User Course 2014 Jim Conboy.
PPPL International Collaboration Activities J. R. Wilson Head Off-site Research Department Princeton Plasma Physics Laboratory 4th US-PRC Magnetic Fusion.
FOM - Institute for Plasma Physics Rijnhuizen Association Euratom-FOM Diagnostics and Control for Burning Plasmas Discussion All of you.
Overview of the GlueX Tagger and Photon Beamline..
Objectives Much better spatial resolution Velocity space discrimination W. Heidbrink, M. Van Zeeland, J. Yu FIDA Imaging Proposal.
Neutron inelastic cross section measurement on 28 Si Alexandru Negret Horia Hulubei National Institute for Physics and Nuclear Engineering, Bucharest,
Absolute neutron yield measurement using divertor NFM Kaschuck Yu.A., Krasilnikov A.V., Prosvirin D.V., Tsutskikh A.Yu. SRC RF TRINITI, Troitsk, Russia.
Neutron diagnostics for fusion experiments
PERSISTENT SURVEILLANCE FOR PIPELINE PROTECTION AND THREAT INTERDICTION International Plan for ELM Control Studies Presented by M.R. Wade (for A. Leonard)
DISCUSSION OF ISSUES, OPPORTUNITIES AND CONCLUSIONS FOR ROTATION AND MOMENTUM TRANSPORT SESSIONS 10th ITPA Transport Physics and CDBM TG Meetings Princeton.
Prospects to measure 8 B production VLADIMIR KRAVCHUK Laboratori Nazionali di Legnaro, Italy EUROnu week in Strasbourg 1-4 June 2010.
Fusion Neutronics Activity at JAERI from October 2000 to September 2001 Peseted by Takeo NISHTANI IEA International Work Shop on Fusion Neutronics The.
Luminosity measurement at LHC (The machine point of view) Enrico Bravin AB/BDI Large part of the material presented here has been produced by the LBNL.
Slide 1 The Heavy Ion Fusion Science Virtual National Laboratory Why heavy ions? Target requires: 3.5 – 6 MJ in ~ 10 ns  500 TW Range ~ 0.02 – 0.20 g/cm.
045-05/rs PERSISTENT SURVEILLANCE FOR PIPELINE PROTECTION AND THREAT INTERDICTION Taming The Physics For Commercial Fusion Power Plants ARIES Team Meeting.
Moving fast in fusion reactors: ASCOT – race track for fast ions
Mass Spectrometry Relative atomic masses and the mass of individual isotopes can be determined using a mass spectrometer. The principle behind mass spectrometry.
NSTX Meeting name – abbreviated presentation title, abbreviated author name (??/??/20??) Goals of NSTX Advanced Scenario and Control TSG Study, implement,
Status of NSTX/DIII-D/MAST aspect ratio core confinement comparison studies M. Peng, for E.J. Synakowski For the ITPA Transport Physics Working Group Kyota,
NSTX-U Waves & Energetic Particles Theory/Experiment Joint Research Topics Supported by Gary Taylor Mario Podestà Nikolai Gorelenkov NSTX-U NSTX-U Theory.
Localised Neutron Emission at the edge of high density JET Trace Tritium - ELMy H-mode plasmas A.Murari 6 on the behalf of G. Bonheure 1, S. Popovichev.
48 Ti(n, xnyp  ) reaction cross sections using spallation neutrons for E n = 1 to 20 MeV Excitation functions have been measured for the interaction of.
The 14 MeV Frascati Neutron Generator (FNG)
6 th ITPA MHD Topical Group Meeting combined with W60 IEA Workshop on Burning Plasmas Summary Session II MHD Stability and Fast Particle Confinement chaired.
Gamma Ray Spectrometry System Design for ITER Plasma Diagnostics
Activities on straw tube simulation
Associazione EURATOM-ENEA sulla Fusione
Maximum sample volume: 1.57 cm3 (20φ, 5 mm thickness)
K2K and JHF-nu muon monitor
大強度
Status of Vertical Neutron Camera Integration
Luminosity measurement at LHC (The machine point of view)
D. S. Darrow Princeton Plasma Physics Laboratory
I-mode regime has many attractive features for fusion:
Neutron spectrometry in fusion energy research
Mirko Salewski Technical University of Denmark Department of Physics
GALACTIC ASTRONOMY (II): PULSARS
PS-Booster Measurements for the LHC -BLM October 2002
Presentation transcript:

Discussion ITPA-10 in Troitsk 11 of April 2006 (Neutron Working Group)

I. Absolute Neutron yield measurements 1. Number of NFM is preferable External NFM (U-235, U-238) Internal (Microfission chambers (array) U- 235) Divertor (U-235, U-238) NDD, Si in number of positions 2. RNC + VNC 3. Neutron spectrometer + (RNC+VNC) 4. Activation method

Absolute calibration DT neutron generator ~ 10**11 n/s Cf and / or Am-Be neutron source ~ 10**10 n/s MCNP calculation for NFM, RNC+VNC, Spectrometer, Activation technique Activation technique will provide check of calibration coefficients change in time NTA Neutron generator and neutron source (same as will be used for in-situ calibration)

Spectrometers Fast ions (Beam deuterons) Ti AKN Vrot D/T ratio

Fast ions NBI deuteron spatial distribution during AE activity (for current drive, for transport studies, confinement) (JT-60U, D-IIID (FIDA, W.H.), JET, N.Gorelenkov) Advance regime (D-IIID, current hole at JET) ICRH (fundamental for D and second harmonic for T) (JET)

Lost alpha detectors

New measurement technologies CVD diamond (increase of sensitivity) Digital Signal Processing (increase of dynamic range and time resolution)