000836117 001__ 836117
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000836117 037__ $$aFZJ-2017-05241
000836117 041__ $$aEnglish
000836117 1001_ $$0P:(DE-Juel1)168124$$aGutberlet, Thomas$$b0$$eCorresponding author
000836117 1112_ $$aInternational Conference on Neutron Optics$$cNara$$d2017-07-05 - 2017-07-08$$gNOP2017$$wJapan
000836117 245__ $$aThe Jülich High Brilliance Neutron Source Project – A challenge for neutron optics
000836117 260__ $$c2017
000836117 3367_ $$033$$2EndNote$$aConference Paper
000836117 3367_ $$2DataCite$$aOther
000836117 3367_ $$2BibTeX$$aINPROCEEDINGS
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000836117 3367_ $$2ORCID$$aLECTURE_SPEECH
000836117 3367_ $$0PUB:(DE-HGF)6$$2PUB:(DE-HGF)$$aConference Presentation$$bconf$$mconf$$s1501742354_30362$$xOther
000836117 520__ $$aNeutrons can be produced by fission in nuclear reactors, by spallation using high-power proton accelerators, and by nuclear reactions with low-energy proton accelerators. While the first two techni¬ques can offer the highest neutron flux production, current state-of-the-art accelerator technology offers the opportunity for a new landscape of novel and unique high-brilliance neutron sources based on low-energy proton accelerators. The Jülich Centre for Neutron Science has started a project to develop and design compact accelerator driven high-brilliance neutron sources as an efficient and cost effective alternative to current low- and medium-flux reactor and spallation sources. Such compact sources have the potential to offer access of science and industry to neutrons as local national or regional medium-flux, but high-brilliance neutron facilities. The project aims to deliver a “High-Brilliance Neutron Source (HBS)”, where a compact neutron production and moderator system provide thermal and cold neutrons with high brilliance efficiently extracted in an optimized neutron transport system. With shaping the experiment from the source to the detector a holistic neutron experiment could be set-up for the specific scientific requirements in a flexible and efficient way for the neutron user. This presents a particular challenge for the appropriate neutron transport systems to deliver the full brilliance of the source to the sample. Neutron lenses, ballistic guides and focusing systems will be requested to minimize any loss in brilliance and neutron flux. In this report we will present a brief outline of the JCNS HBS project and discuss resulting requirements on neutron transport devices.
000836117 536__ $$0G:(DE-HGF)POF3-524$$a524 - Controlling Collective States (POF3-524)$$cPOF3-524$$fPOF III$$x0
000836117 536__ $$0G:(DE-HGF)POF3-6212$$a6212 - Quantum Condensed Matter: Magnetism, Superconductivity (POF3-621)$$cPOF3-621$$fPOF III$$x1
000836117 536__ $$0G:(DE-HGF)POF3-6G15$$a6G15 - FRM II / MLZ (POF3-6G15)$$cPOF3-6G15$$fPOF III$$x2
000836117 536__ $$0G:(DE-HGF)POF3-6G4$$a6G4 - Jülich Centre for Neutron Research (JCNS) (POF3-623)$$cPOF3-623$$fPOF III$$x3
000836117 536__ $$0G:(DE-Juel1)HITEC-20170406$$aHITEC - Helmholtz Interdisciplinary Doctoral Training in Energy and Climate Research (HITEC) (HITEC-20170406)$$cHITEC-20170406$$x4
000836117 65027 $$0V:(DE-MLZ)SciArea-220$$2V:(DE-HGF)$$aInstrument and Method Development$$x0
000836117 65017 $$0V:(DE-MLZ)GC-2002-2016$$2V:(DE-HGF)$$aInstrument and Method Development$$x0
000836117 693__ $$0EXP:(DE-MLZ)NOSPEC-20140101$$5EXP:(DE-MLZ)NOSPEC-20140101$$eNo specific instrument$$x0
000836117 7001_ $$0P:(DE-Juel1)130928$$aRücker, Ulrich$$b1
000836117 7001_ $$0P:(DE-Juel1)131055$$aZakalek, Paul$$b2
000836117 7001_ $$0P:(DE-Juel1)164368$$aCronert, Tobias$$b3
000836117 7001_ $$0P:(DE-Juel1)131018$$aVoigt, Jörg$$b4
000836117 7001_ $$0P:(DE-Juel1)169802$$aBaggemann, Johannes$$b5
000836117 7001_ $$0P:(DE-Juel1)169952$$aDoege, Paul$$b6
000836117 7001_ $$0P:(DE-HGF)0$$aBöhm, Sarah$$b7
000836117 7001_ $$0P:(DE-HGF)0$$aDabruck, J.-P.$$b8
000836117 7001_ $$0P:(DE-Juel1)130386$$aNabbi, Rahim$$b9
000836117 7001_ $$0P:(DE-Juel1)130572$$aBrückel, Thomas$$b10
000836117 909CO $$ooai:juser.fz-juelich.de:836117$$pVDB$$pVDB:MLZ
000836117 9101_ $$0I:(DE-588b)5008462-8$$6P:(DE-Juel1)168124$$aForschungszentrum Jülich$$b0$$kFZJ
000836117 9101_ $$0I:(DE-588b)5008462-8$$6P:(DE-Juel1)130928$$aForschungszentrum Jülich$$b1$$kFZJ
000836117 9101_ $$0I:(DE-588b)5008462-8$$6P:(DE-Juel1)131055$$aForschungszentrum Jülich$$b2$$kFZJ
000836117 9101_ $$0I:(DE-588b)5008462-8$$6P:(DE-Juel1)164368$$aForschungszentrum Jülich$$b3$$kFZJ
000836117 9101_ $$0I:(DE-588b)5008462-8$$6P:(DE-Juel1)131018$$aForschungszentrum Jülich$$b4$$kFZJ
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000836117 9101_ $$0I:(DE-588b)5008462-8$$6P:(DE-Juel1)169952$$aForschungszentrum Jülich$$b6$$kFZJ
000836117 9101_ $$0I:(DE-588b)5008462-8$$6P:(DE-Juel1)130386$$aForschungszentrum Jülich$$b9$$kFZJ
000836117 9101_ $$0I:(DE-588b)5008462-8$$6P:(DE-Juel1)130572$$aForschungszentrum Jülich$$b10$$kFZJ
000836117 9131_ $$0G:(DE-HGF)POF3-524$$1G:(DE-HGF)POF3-520$$2G:(DE-HGF)POF3-500$$3G:(DE-HGF)POF3$$4G:(DE-HGF)POF$$aDE-HGF$$bKey Technologies$$lFuture Information Technology - Fundamentals, Novel Concepts and Energy Efficiency (FIT)$$vControlling Collective States$$x0
000836117 9131_ $$0G:(DE-HGF)POF3-621$$1G:(DE-HGF)POF3-620$$2G:(DE-HGF)POF3-600$$3G:(DE-HGF)POF3$$4G:(DE-HGF)POF$$9G:(DE-HGF)POF3-6212$$aDE-HGF$$bForschungsbereich Materie$$lVon Materie zu Materialien und Leben$$vIn-house research on the structure, dynamics and function of matter$$x1
000836117 9131_ $$0G:(DE-HGF)POF3-6G15$$1G:(DE-HGF)POF3-6G0$$2G:(DE-HGF)POF3-600$$3G:(DE-HGF)POF3$$4G:(DE-HGF)POF$$9G:(DE-HGF)POF3-6G15$$aDE-HGF$$bForschungsbereich Materie$$lGroßgeräte: Materie$$vFRM II / MLZ$$x2
000836117 9131_ $$0G:(DE-HGF)POF3-623$$1G:(DE-HGF)POF3-620$$2G:(DE-HGF)POF3-600$$3G:(DE-HGF)POF3$$4G:(DE-HGF)POF$$9G:(DE-HGF)POF3-6G4$$aDE-HGF$$bForschungsbereich Materie$$lVon Materie zu Materialien und Leben$$vFacility topic: Neutrons for Research on Condensed Matter$$x3
000836117 9141_ $$y2017
000836117 9201_ $$0I:(DE-Juel1)JCNS-FRM-II-20110218$$kJCNS (München) ; Jülich Centre for Neutron Science JCNS (München) ; JCNS-FRM-II$$lJCNS-FRM-II$$x0
000836117 9201_ $$0I:(DE-Juel1)JCNS-2-20110106$$kJCNS-2$$lStreumethoden$$x1
000836117 9201_ $$0I:(DE-Juel1)PGI-4-20110106$$kPGI-4$$lStreumethoden$$x2
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