Use of Neutron Beams for Low and Medium Flux Research Reactors

Total Page:16

File Type:pdf, Size:1020Kb

Use of Neutron Beams for Low and Medium Flux Research Reactors IAEA-TECDOC-836 Use neutronof beamsfor mediumand low flux research reactors: R&D programmes in materials science Report of an Advisory Group meeting held Vienna,in arch-1 M 29 April 1993 INTERNATIONAL ATOMIC ENERGY AGENCY The IAEA does not normally maintain stocks of reports in this series. However, microfiche copie f thesso e reportobtainee b n sca d from ClearinghousS I N I e International Atomic Energy Agency Wagramerstrasse5 0 10 P.Ox Bo . A-1400 Vienna, Austria Orders should be accompanied by prepayment of Austrian Schillings 100, for e for cheque a th f m th IAEf m o n i o n i r eAo microfiche service coupons which may be ordered separately from the INIS Clearinghouse. The IAEA doe t normallsno y maintain stock f reportso thin si s series. However, microfiche copie f thesso e reportobtainee b n sca d from ClearinghousS I N I e International Atomic Energy Agency Wagramerstrasse 5 P.O. Box 100 A-1400 Vienna, Austria Orders should be accompanied by prepayment of Austrian Schillings 100, for e fore chequa th f m th IAEf mo n i o n i r eAo microfiche service coupons which may be ordered separately from the INIS Clearinghouse. originatine Th g Sectio f thino s publicatio IAEe th An i was : Physics Section International Atomic Energy Agency Wagramerstrasse 5 P.O. Box 100 A-1400 Vienna, Austria NEUTROF O MEDIUE D US AN NW M BEAM LO FLU R XSFO RESEARCH REACTORS: R&D PROGRAMME MATERIALSN I S SCIENCE IAEA, VIENNA, 1995 IAEA-TECDOC-836 ISSN 1011-4289 ©IAEA, 1995 Printe IAEe th AustriAn y i d b a October 1995 FOREWORD Research reactors have been playin importann ga developmente rolth n ei scientifif o t c technologicad an l infrastructur traininn i d ean manpowef g o introductioe th r rfo nucleaf no r powe mann ri y countries. Currently operationa4 , ther28 e ear l research reactor worlde th n si , includin 8 researc8 g h reactor 9 developin3 i h s g countries e numbeth ; f reactoro r n i s developing countrie s increasini s s morga e countries embar programmen ko nuclean i s r scienc technologyd ean . However, full utilizatio f thesno e facilitie r fundamentafo s d an l applied research has seldom been achieved. In particular, the utilization of beam ports has been quite low. Neutron beam based researc mose th regardef ths i o importan e on s da t programme areas that can be implemented even at low and medium flux reactors. The range of activities possibl thin ei s widfielo s s dei generallthas i t ti y feasibl definprogrammeo et D eR& suio st t different needs and conditions. It is, therefore, important and of direct benefit to identify effective way improvo st e utilizatio beaf nresearco e mth f tubeo d h sreactorsan thio T .s end, the International Atomic Energy Agency organized two meetings during 1993. First, an Advisory Group Meetin gf Researc o (AGMe Us hn )o Reactor Solir sfo d State Studied san second Technicaa , l Committee Meetin Researcf go (TCMe Us n h)o Reacto r Neutron Beams for Radiograph Materiald yan revieo st Characterizations d wwa an M AG e goae th f Th .o l provide recommendation neutron o s n scattering techniques focuseM , TC whiln o de th e neutron radiography and other simple methods and applications. presene Th t repor Advisorresule e th th f s i to t y Group Meeting held durin 9 Marcg2 h - 1 April 1993 in Vienna with subsequent contributions from the experts. The Physics Section of the Department of Research and Isotopes was responsible for the co-ordination and compilatio reporte th f no . The report is intended to provide guidelines to research reactor owners and operators for promotin developind an g g neutron beam based research programme r solifo s d state studies using neutron scattering techniques expectes i t I . benefio dt t ongoing facilitied an s programme encouraginy sb f unproveo e gus d technique r detectionsfo , signal acquisition, signal processing, etc. and new programmes by assisting in the selection of appropriate equipment, instrument design and research plans. EDITORIAL NOTE In preparing this publication press,for staff, IAEAofthe have pages madethe up from the original manuscripts submittedas authors.the viewsby The expressed necessarilynot do reflect those governmentsofthe nominatingthe of Member nominating the States of or organizations. Throughout the text names of Member States are retained as they were when the text was compiled. Theof use particular designations countriesof territoriesor does imply judgementnot any by publisher,the legalthe IAEA,to status the as of such countries territories,or of their authoritiesand institutions or of the delimitation of their boundaries. The mention of names of specific companies or products (whether or not indicated as registered) does not imply any intention to infringe proprietary rights, nor should it be construed as an endorsement recommendationor partthe IAEA. ofon the The authors are responsible for having obtained the necessary permission for the IAEA to reproduce, translate materialuse or from sources already protected copyrights.by CONTENTS 1. INTRODUCTION ....................................... 7 . FRAMEWOR2 SUSTAINABLR KFO ......................D ER& 7 . 2.1. Importance of neutron scattering techniques .................... 7 2.2. Minimum siz researcf eo h groups ..........................8 . 2.3. Infrastructural facilities ................................8 . 2.4. Essential investment needs ............................... 8 2.5. Reverse mobility of scientists ............................. 9 2.6. Interdisciplinary collaboration ............................. 9 3. FUTURE RESEARCH PROGRAMMES ......................... 9 3.1. Magnetic compounds .................................0 1 . 3.2. Magnetically disordered systems ........................... 10 3.3. Magnetic thin films and superlattices ......................... 11 3.4. Ceramic (high T,.) superconductors .......................... 11 3.5. Texture and residual stress in fabricated materials ................. 12 3.6. Zeolites .........................................2 1 . 3.7. Petrogenic materials ..................................2 1 . 3.8. Minerals, polymer amorphoud san s systems ...................2 1 . 4. METHODS AND INSTRUMENTATION ........................ 13 4.1. Overview ........................................3 1 . 4.2. Methods .........................................3 1 . 4.3. Technique instrumentatiod san n details ......................5 1 . 4.4. Data acquisition and control .............................. 24 5. CONCLUSIONS .......................................5 2 . REFERENCES ........................................... 25 ANNEX: PAPERS PRESENTED AT THE ADVISORY GROUP MEETING Fundamenta applied an l d neutro TRIGW k n0 A researc 25 reacto e th t ha r 9 Vienn2 . .. a G. Badurek Use of research reactors for solid state physics studies at Bhabha Atomic Research Centre, India .................................... 41 K.R. Rao Solid state physics around Pakistan Research Reacto t PINSTECa r H ..........5 5 . N.M. Butt, Bashir,J. NasirM. Khan Framework for a sustainable development of neutron beam work in the smaller research reactors ........................................ 81 Carvalho,G. F. P.M.A. Margaça Basic research in solid state physics using a small research reactor ............ 91 V. Dimic The new Swiss spallation neutron source SINQ and its planned day-one instruments — Statuf sprino s sa g 1993 ..................................7 9 . G.S. Bauer Neutron scattering research with low to medium flux reactors ...............115 J.J. Khyne The ORPHEE versatile low-cost multiprocessor system for data acquisition and contro neutrof o l n spectrometers .............................5 12 . G. Koskas List of Participants ........................................ 143 1. INTRODUCTION Worldwide there are 284 operable nuclear research reactors of which 88 are located in developin0 39 g countries. These research reactor laboratoriee th d san s around them represent a significant research potential and a source of highly qualified and trained manpower not onl activitier yfo s relate nucleao dt r field alst severar sbu o fo l conventional technologiese Th . acquisition of a nuclear research reactor, in a developing country, is generally justified on the basis that it is a necessary tool for: • Fundamental and applied research in various disciplines; • Training of young scientists in nuclear sciences; • Production of radioisotopes; • Supporting activities related to nuclear power including operator training; • Engineering experiments. These objectives have been achieved with different degrees of success in different countries. Among several factors that contribute toward underutilization of these facilities, mose th t obvious ones are: inappropriate research programmes, lac adequatf ko e equipment and laboratories, relatively low neutron fluxes, non-availability of sufficiently trained manpower. In particular, the utilization of neutron beam ports remains very low. This is in spite of the fact that neutron beam based research is one of the most important programme areas e implementedwhicb n hca mediud an , w mevelo t fluna x reactors e rangTh .f o e activities possibl thin ei s wido ares generas n aei i thas i t i t l possibl defino et carrd t ean you programmeD R& suio st t specific need conditionsd san . This report covers various aspects of neutron beam research applicable to materials science specifiet .I s minimal requirements concerning infrastructures, personnel, funding, etc. as these conditions must coexist for a viable research programme over a period of several years
Recommended publications
  • The Theoretical Foundation of Spin-Echo Small-Angle Neutron
    The Theoretical Foundation of Spin‐Echo Small‐Angle Neutron Scattering (SESANS) Applied in Colloidal System Wei‐Ren Chen, Gregory S. Smith, and Kenneth W. Herwig (NSSD ORNL) Yun Liu (NCNR NIST & Chemistry, University of Delaware) Li (Emily) Liu (Nuclear Engineering, RPI) Xin Li, Roger Pynn (Physics, Indiana University) Chwen‐Yang Shew (Chemistry, CUNY) UCANS‐II Indiana University July 08th 2011 Bloomington, IN Outline 1. Motivation — why Spin-Echo Small-Angle Neutron Scattering (SESANS)? 2. Basic Theory — what does SESANS measure? 3. Results and Discussions — what can SESANS do? (1). Straightforward observation of potential (2). Sensitivity to the local structure (3). Sensitivity to the structural heterogeneity 4. Summary Outline 1. Motivation — why Spin-Echo Small-Angle Neutron Scattering (SESANS)? 2. Basic Theory — what does SESANS measure? 3. Results and Discussions — what can SESANS do? (1). Straightforward observation of potential (2). Sensitivity to the local structure (3). Sensitivity to the structural heterogeneity 4. Summary Neutron Scattering Structure (Elastic Scatt.) Dynamics (Inelastic Scatt.) Small‐Angle Neutron Quasi‐Elastic Neutron Unpolarized Scattering (SANS), Scattering (QENS), beam Neutron Diffraction, Inelastic Neutron Scattering Neutron Reflectometry (INS) Polarized Spin‐Echo Small‐Angle Neutron Spin‐Echo (NSE) beam Neutron Scattering (SESANS) Neutron Scattering Structure (Elastic Scatt.) Dynamics (Inelastic Scatt.) Small‐Angle Neutron Quasi‐Elastic Neutron Unpolarized Scattering (SANS), Scattering (QENS), beam Neutron
    [Show full text]
  • Neutron Scattering
    Neutron Scattering John R.D. Copley Summer School on Methods and Applications of High Resolution Neutron Spectroscopy and Small Angle Neutron Scattering NIST Center for NeutronNCNR Summer Research, School 2011 June 12-16, 2011 Acknowledgements National Science Foundation NIST Center for Neutron (grant # DMR-0944772) Research (NCNR) Center for High Resolution Neutron Scattering (CHRNS) 2 NCNR Summer School 2011 (Slow) neutron interactions Scattering plus Absorption Total =+Elastic Inelastic scattering scattering scattering (diffraction) (spectroscopy) includes “Quasielastic neutron Structure Dynamics scattering” (QENS) NCNR Summer School 2011 3 Total, elastic, and inelastic scattering Incident energy Ei E= Ei -Ef Scattered energy Ef (“energy transfer”) Total scattering: Elastic scattering: E = E (i.e., E = 0) all Ef (i.e., all E) f i Inelastic scattering: E ≠ E (i.e., E ≠ 0) D f i A M M Ef Ei S Ei D S Diffractometer Spectrometer (Some write E = Ef –Ei) NCNR Summer School 2011 4 Kinematics mv= = k 1 222 Emvk2m==2 = Scattered wave (m is neutron’s mass) vector k , energy E 2θ f f Incident wave vector ki, energy Ei N.B. The symbol for scattering angle in Q is wave vector transfer, SANS experiments is or “scattering vector” Q =Q is momentum transfer θ, not 2θ. Q = ki - kf (For x-rays, Eck = = ) (“wave vector transfer”) NCNR Summer School 2011 5 Elastic scattering Q = ki - kf G In real space k In reciprocal space f G G G kf Q ki 2θ 2θ G G k Q i E== 0 kif k Q =θ 2k i sin NCNR Summer School 2011 6 Total scattering, inelastic scattering Q = ki - kf G kf G Q Qkk2kkcos2222= +− θ 2θ G if if ki At fixed scattering angle 2θ, the magnitude (and the direction) of Q varies with the energy transfer E.
    [Show full text]
  • The Jules Horowitz Reactor Project, a Driver for Revival of the Research Reactor Community
    THE JULES HOROWITZ REACTOR PROJECT, A DRIVER FOR REVIVAL OF THE RESEARCH REACTOR COMMUNITY P. PERE, C. CAVAILLER, C. PASCAL AREVA TA CEA Cadarache - Etablissement d'AREVA TA - Chantier RJH - MOE - BV2 - BP n° 9 – 13115 Saint Paul lez Durance - France CS 50497 - 1100, rue JR Gauthier de la Lauzière, 13593 Aix en Provence cedex 3 – France ABSTRACT The first concrete of the nuclear island for the Jules Horowitz Reactor (JHR) was poured at the end of July 2009 and construction is ongoing. The JHR is the largest new platform for irradiation experiments supporting Generation II and III reactors, Generation IV technologies, and radioisotope production. This facility, composed of a unique grouping of workshops, hot cells and hot laboratories together with a first -rate MTR research reactor, will ensure that the process, from preparations for irradiation experiments through post-irradiation non-destructive examination, is completed expediently, efficiently and, of course, safely. In addition to the performance requirements to be met in terms of neutron fluxes on the samples (5x1014 n.cm-2/sec-1 E> 1 MeV in core and 3,6x1014 n.cm-2/sec-1 E<0.625 eV in the reflector) and the JHR’s considerable irradiation capabilities (more than 20 experiments and one-tenth of irradiation area for simultaneous radioisotope production), the JHR is the first MTR to be built since the end of the 1960s, making this an especially challenging project. The presentation will provide an overview of the reactor, hot cells and laboratories and an outline of the key milestones in the project schedule, including initial criticality in early 2014 and radioisotope production in 2015.
    [Show full text]
  • Optimizing Crystal Volume for Neutron Diffraction: D-Xylose Isomerase
    Eur Biophys J (2006) 35:621–632 DOI 10.1007/s00249-006-0068-4 ARTICLE Optimizing crystal volume for neutron diffraction: D-xylose isomerase Edward H. Snell Æ Mark J. van der Woerd Æ Michael Damon Æ Russell A. Judge Æ Dean A. A. Myles Æ Flora Meilleur Received: 15 February 2006 / Revised: 27 March 2006 / Accepted: 4 April 2006 / Published online: 25 May 2006 Ó EBSA 2006 Abstract Neutron diffraction is uniquely sensitive to studies for a larger number of samples that require hydrogen positions and protonation state. In that information on hydrogen position and/or protonation context structural information from neutron data is state. complementary to that provided through X-ray dif- fraction. However, there are practical obstacles to overcome in fully exploiting the potential of neutron diffraction, i.e. low flux and weak scattering. Several approaches are available to overcome these obstacles Introduction and we have investigated the simplest: increasing the diffracting volume of the crystals. Volume is a quan- Neutron diffraction tifiable metric that is well suited for experimental de- sign and optimization techniques. By using response X-ray structural crystallography is a powerful tech- surface methods we have optimized the xylose isom- nique to visualize the machinery of life on a molecular erase crystal volume, enabling neutron diffraction scale. However, hydrogen atoms are not usually seen while we determined the crystallization parameters because X-ray scattering from hydrogen atoms is weak with a minimum of experiments. Our results suggest a compared to other atoms. Knowledge of the location of systematic means of enabling neutron diffraction hydrogen atoms and water molecules is often necessary to completely understand the reaction mechanisms, pathways and structure–function relationships.
    [Show full text]
  • Neutron Scattering Facilities in Europe Present Status and Future Perspectives
    2 ESFRI Physical Sciences and Engineering Strategy Working Group Neutron Landscape Group Neutron scattering facilities in Europe Present status and future perspectives ESFRI scrIPTa Vol. 1 ESFRI Scripta Volume I Neutron scattering facilities in Europe Present status and future perspectives ESFRI Physical Sciences and Engineering Strategy Working Group Neutron Landscape Group i ESFRI Scripta Volume I Neutron scattering facilities in Europe - Present status and future perspectives Author: ESFRI Physical Sciences and Engineering Strategy Working Group - Neutron Landscape Group Scientific editors: Colin Carlile and Caterina Petrillo Foreword Technical editors: Marina Carpineti and Maddalena Donzelli ESFRI Scripta series will publish documents born out of special studies Cover image: Diffraction pattern from the sugar-binding protein Gal3c with mandated by ESFRI to high level expert groups, when of general interest. lactose bound collected using LADI-III at ILL. Picture credits should be given This first volume reproduces the concluding report of an ad-hoc group to D. Logan (Lund University) and M. Blakeley (ILL) mandated in 2014 by the Physical Science and Engineering Strategy Design: Promoscience srl Work Group (PSE SWG) of ESFRI, to develop a thorough analysis of the European Landscape of Research Infrastructures devoted to Neutron Developed on behalf of the ESFRI - Physical Sciences and Engineering Strategy Scattering, and its evolution in the next decades. ESFRI felt the urgency Working Group by the StR-ESFRI project and with the support of the ESFRI of such analysis, since many reactor-based neutron sources will be closed Secretariat down in the next years due to national decisions, while the European The StR-ESFRI project has received funding from the European Union’s Spallation Source (ESS) in Lund will be fully operative only in the mid Horizon 2020 research and innovation programme under grant agreement or late 2020s.
    [Show full text]
  • Recent Progress in X-Ray and Neutron Phase Imaging with Gratings
    Review Recent Progress in X-Ray and Neutron Phase Imaging with Gratings Atsushi Momose 1,*, Hidekazu Takano 1, Yanlin Wu 1 , Koh Hashimoto 1, Tetsuo Samoto 1, Masato Hoshino 2, Yoshichika Seki 3 and Takenao Shinohara 3 1 Institute of Multidisciplinary Research for Advanced Materials, Tohoku University, 2-1-1 Katahira, Aoba-ku, Sendai, Miyagi 980-8577, Japan; [email protected] (H.T.); [email protected] (Y.W.); [email protected] (K.H.); [email protected] (T.S.) 2 JASRI, 1-1-1 Kouto, Sayo-cho, Sayo-gun, Hyogo 679-5198, Japan; [email protected] 3 J-PARC Center, Japan Atomic Energy Agency, 2-4 Shirakata, Tokai-mura, Naka-gun, Ibaraki 319-1195, Japan; [email protected] (Y.S.); [email protected] (T.S.) * Correspondence: [email protected] Received: 29 December 2019; Accepted: 4 February 2020; Published: 10 February 2020 Abstract: Under the JST-ERATO project in progress to develop X-ray and neutron phase-imaging methods together, recent achievements have been selected and reviewed after describing the merit and the principle of the phase imaging method. For X-ray phase imaging, recent developments of four-dimensional phase tomography and phase microscopy at SPring-8, Japan are mainly presented. For neutron phase imaging, an approach in combination with the time-of-flight method developed at J-PARC, Japan is described with the description of new Gd grating fabrication. Keywords: phase imaging; phase tomography; grating; interferometry; synchrotron radiation; neutron; X-ray; microscopy; radiography 1.
    [Show full text]
  • Conceptual Design Report Jülich High
    General Allgemeines ual Design Report ual Design Report Concept Jülich High Brilliance Neutron Source Source Jülich High Brilliance Neutron 8 Conceptual Design Report Jülich High Brilliance Neutron Source (HBS) T. Brückel, T. Gutberlet (Eds.) J. Baggemann, S. Böhm, P. Doege, J. Fenske, M. Feygenson, A. Glavic, O. Holderer, S. Jaksch, M. Jentschel, S. Kleefisch, H. Kleines, J. Li, K. Lieutenant,P . Mastinu, E. Mauerhofer, O. Meusel, S. Pasini, H. Podlech, M. Rimmler, U. Rücker, T. Schrader, W. Schweika, M. Strobl, E. Vezhlev, J. Voigt, P. Zakalek, O. Zimmer Allgemeines / General Allgemeines / General Band / Volume 8 Band / Volume 8 ISBN 978-3-95806-501-7 ISBN 978-3-95806-501-7 T. Brückel, T. Gutberlet (Eds.) Gutberlet T. Brückel, T. Jülich High Brilliance Neutron Source (HBS) 1 100 mA proton ion source 2 70 MeV linear accelerator 5 3 Proton beam multiplexer system 5 4 Individual neutron target stations 4 5 Various instruments in the experimental halls 3 5 4 2 1 5 5 5 5 4 3 5 4 5 5 Schriften des Forschungszentrums Jülich Reihe Allgemeines / General Band / Volume 8 CONTENT I. Executive summary 7 II. Foreword 11 III. Rationale 13 1. Neutron provision 13 1.1 Reactor based fission neutron sources 14 1.2 Spallation neutron sources 15 1.3 Accelerator driven neutron sources 15 2. Neutron landscape 16 3. Baseline design 18 3.1 Comparison to existing sources 19 IV. Science case 21 1. Chemistry 24 2. Geoscience 25 3. Environment 26 4. Engineering 27 5. Information and quantum technologies 28 6. Nanotechnology 29 7. Energy technology 30 8.
    [Show full text]
  • Decommissioning of Nuclear Facilities in Switzerland – Lessons Learned
    WIR SCHAFFEN WISSEN – HEUTE FÜR MORGEN Fritz Leibundgut :: Decommissioning Officer :: Paul Scherrer Institut Decommissioning of Nuclear Facilities in Switzerland – Lessons learned HRP/IAEA/NEA Decommissioning workshop – February 7, 2017 Overview Basel Germany Aarau/Bern Zürich material sciences nanotechnology radio chemistry hotlab radio pharmacy biology PSI east solar concentrator energy research SwissFEL particle physics proton accelerator neutron source muon source proton therapy PSI west synchrotron light source Page 2 Nuclear installations on the PSI area • (ZWILAG) • AERA with VVA* • Hotlabor • DIORIT* • SAPHIR* • PROTEUS* *Post-operation phase/ Decomm./Dismantling Page 3 SAPHIR: 1957-1993 First reactor in Switzerland; used for isotope production, reactor training, neutron source for various experiments 1955 USA exposed a reactor at the “Atoms for Peace” conference in Geneva 1956 Laying of the cornerstone in Würenlingen 1957 First criticality 1960 Approval by Swiss government 1985 Approval for 10 MW 1993 Final shutdown 2000 Decommissioning ordinance 2008 Dismantling of the pool completed 2015 Cleanout of the KBL (“Kernbrennstofflager”) Page 4 SAPHIR: Status 2016 ENSI-Inspection at 7. of April, 2016 Page 5 DIORIT: 1960-1977 Proprietary Swiss development. Goal was the construction of industrial applicable reactors for material testings and experiments. 1960 Operation with natural uranium and D2O as coolant and moderator. 1966 Uprating from 20 MW to 30 MW. 1972 (after modification): Operation with LEU. 1977 Final shutdown. 1982 Partial dismantling; continued 1988-1993. 1994 Approval of dismantling the reactor. 2005 Asbestos was found interruption until 2009. 2013 Dismantling of biological shielding 2016 Cutting of the „Arbeitsboden“ (22 t activated Fe) 2019 (?) 2. Decommissioning ordinance for greenfield Page 6 DIORIT PSI, 23.10.2016 Page 7 Biol.
    [Show full text]
  • German Research Reactor
    German Research Reactor Back-end Provisions RERTR 2002 San Carlos de Bariloche, Argentina Nov-3/8 Authors: Siegfried Koester/German Federal Ministry of Economics and Technology Gerhard Gruber/RWE NUKEM GmbH On behalf of the German Working Group Back-end for Research Reactors Fuel Cycle History of Half a Century US 'Atoms for Peace Program', President Eisenhower 1953 HEU for peaceful research and development (R&D) First RR built in Germany in the late 1950s US supplied fuel on a lease basis until 1974 Until 1987 fuel sale with option to return spent HEU + LEU fuel 1987-Dec-31: DOE's policy for receipt of FRR SNF expires without prior notice German RR Back-end History 1960s: US Reprocessing, no return of waste 1960/70s: UK Reprocessing, no return of waste 1970s: Belgium + France Reprocessing, no return of waste 1980s: US Reprocessing, no return of waste 1990s: UK Reprocessing, mandatory waste return Current German Back-end Solution 1996 - 2006: Return SNF to US under 'FRR SNF Return Policy' (US-origin) Non-Proliferation: Return of all HEU to the US 2 Promote RR conversion to LEU 10 yrs to provide for national Back-end solutions Establish int. Back-end solutions (e.g. IAEA promotion) German Spent RR Fuel Output Current Reactors (operation time): 'BER-II' (2015), 'FRG-1' (> 2010), 'FRJ-2' (2005?), 'TRIGA-MZ' (>2010), 8 'SUR’ Future Reactors: 'FRM-II' (2003-2033), 'NN' (possibly needed > 2010) Fuels: U-Al, U-Si, U-ZrH, U-PE, U-Mo in future US- and RUS-origin RUS-origin: 'FRM-II' + 'RFR' (shut down) with 1,000 FE leftover
    [Show full text]
  • Overview of Neutron Interferometry at NIST
    EPJ Web of Conferences 219, 06001 (2019) https://doi.org/10.1051/epjconf/201921906001 PPNS 2018 Overview of neutron interferometry at NIST Michael G. Huber1,a, Shannon F. Hoogerheide1, Muhammad Arif1, Robert W. Haun2, Fred E. Wietfeldt2, Timothy C. Black3, Chandra B. Shahi4, Benjamin Heacock5,6, Albert R. Young5,6, Ivar A.J. Taminiau7, Dusan Sarenac8,9, David G. Cory8,9,10,11, and Dmitry A. Pushin8,9 1 National Institute of Standards and Technology, Gaithersburg, MD 20899, USA 2 Tulane University, New Orleans, LA 70188, USA 3 University of North Carolina Wilmington, Wilmington, NC 28403, USA 4 University of Maryland, College Park, MD 20742, USA 5 North Carolina State University, Raleigh, NC 27695, USA 6 Triangle Universities Nuclear Laboratory, Durham, NC 27708, USA 7 Neutron Optics LP, Waterloo, ON N2L0A7, Canada 8 University of Waterloo, Waterloo, ON N2L3G1, Canada 9 Institute for Quantum Computing, University of Waterloo, Waterloo, ON N2L3G1, Canada 10 Perimeter Institute for Theoretical Physics, Waterloo, ON N2L2Y5, Canada 11 Canadian Institute for Advanced Research, Toronto, ON M5G1Z8, Canada Abstract. Neutron interferometry at the National Institute of Standards and Technology is a well-established program that performs experiments in a wide range of areas including materials science, quantum information, precision measurements of coherent and incoherent scattering lengths, and dark energy/fifth force searches. Central to the continued success of this program is the further understanding and elimination of instabilities and coherence-losses whether they are from thermal, vibrational, or dynamical sources. We have spent considerable effort in fabricating new interferometer crystals which have higher maximum fringe visibilities and that can be tailored to specific experiments.
    [Show full text]
  • Small Angle Scattering in Neutron Imaging—A Review
    Journal of Imaging Review Small Angle Scattering in Neutron Imaging—A Review Markus Strobl 1,2,*,†, Ralph P. Harti 1,†, Christian Grünzweig 1,†, Robin Woracek 3,† and Jeroen Plomp 4,† 1 Paul Scherrer Institut, PSI Aarebrücke, 5232 Villigen, Switzerland; [email protected] (R.P.H.); [email protected] (C.G.) 2 Niels Bohr Institute, University of Copenhagen, Copenhagen 1165, Denmark 3 European Spallation Source ERIC, 225 92 Lund, Sweden; [email protected] 4 Department of Radiation Science and Technology, Technical University Delft, 2628 Delft, The Netherlands; [email protected] * Correspondence: [email protected]; Tel.: +41-56-310-5941 † These authors contributed equally to this work. Received: 6 November 2017; Accepted: 8 December 2017; Published: 13 December 2017 Abstract: Conventional neutron imaging utilizes the beam attenuation caused by scattering and absorption through the materials constituting an object in order to investigate its macroscopic inner structure. Small angle scattering has basically no impact on such images under the geometrical conditions applied. Nevertheless, in recent years different experimental methods have been developed in neutron imaging, which enable to not only generate contrast based on neutrons scattered to very small angles, but to map and quantify small angle scattering with the spatial resolution of neutron imaging. This enables neutron imaging to access length scales which are not directly resolved in real space and to investigate bulk structures and processes spanning multiple length scales from centimeters to tens of nanometers. Keywords: neutron imaging; neutron scattering; small angle scattering; dark-field imaging 1. Introduction The largest and maybe also broadest length scales that are probed with neutrons are the domains of small angle neutron scattering (SANS) and imaging.
    [Show full text]
  • The Past and the Future of the TRIGA Reactor in Vienna
    Journal of Energy and Power Engineering 7 (2013) 654-660 D DAVID PUBLISHING The Past and the Future of the TRIGA Reactor in Vienna Helmuth Böck, Yuj Hasegawa, Erwin Jericha, Georg Steinhauser and Mario Villa Vienna University of Technology, Vienna 1020, Austria Received: July 23, 2012 / Accepted: October 16, 2012 / Published: April 30, 2013. Abstract: During the past five decades, the TRIGA reactor Vienna has reached a top place in utilization among low power research reactors. This paper discussed the highlights of the major neutron physics experiments in the field of neutron interferometry and ultra-small angle neutron scattering as well as in the field of radiochemistry, education and training and research in the field of nuclear safeguards and nuclear security. Potential further directions of research are outlined where the Atominstitut of Vienna might concentrate in future. Key words: TRIGA reactors, research reactors, neutron and solid state physics, neutron interferometry, ultra small-angle neutron scattering, education and training. 1. Introduction discussed in detail in Section 2.1. After the “Atoms for Peace” speech of President 2. Major Neutron Physics Experiments Eisenhower in December 1963, many low power 2.1 Interferometer research reactors were built all over the world, this was the boom-time for TRIGA reactors. Totally about 70 In 2011, 37 years have passed since the first perfect TRIGA reactors were built world-wide, later some crystal neutron interferometer was tested by an other research reactors were converted to TRIGA type Austrian-German cooperative group at the 250 kW fuel, today about 35 TRIGA reactors are still in TRIGA reactor in Vienna [1, 2].
    [Show full text]