000851215 001__ 851215
000851215 005__ 20210129234813.0
000851215 037__ $$aFZJ-2018-04915
000851215 041__ $$aEnglish
000851215 1001_ $$0P:(DE-Juel1)168124$$aGutberlet, Thomas$$b0$$eCorresponding author
000851215 1112_ $$aRANS2-HUNS2 Symposium$$cTokyo$$d2018-07-17 - 2018-07-20$$wJapan
000851215 245__ $$aNOVA ERA - A compact neutron source for universities
000851215 260__ $$c2018
000851215 3367_ $$033$$2EndNote$$aConference Paper
000851215 3367_ $$2DataCite$$aOther
000851215 3367_ $$2BibTeX$$aINPROCEEDINGS
000851215 3367_ $$2DRIVER$$aconferenceObject
000851215 3367_ $$2ORCID$$aLECTURE_SPEECH
000851215 3367_ $$0PUB:(DE-HGF)6$$2PUB:(DE-HGF)$$aConference Presentation$$bconf$$mconf$$s1536235186_11580$$xInvited
000851215 502__ $$cRIKEN
000851215 520__ $$aNeutron scattering has proven to be one of the most powerful methods for the investigation of structure and dynamics of condensed matter on atomic length and time scales. A severe drawback in using neutrons is the limited possibilities to access neutrons offered via nuclear research reactors or accelerator driven spallation sources, which are costly to build and to operate. To offer neutrons more easy accessible for science, training and industrial use is a challenge. The concept of a compact accelerator based neutron source is a new approach to tackle this challenge with the aim to bring neutrons to the users on demand and cost effective.Compact accelerator based neutron sources (CANS) produce neutrons by the nuclear reaction between a low energy proton beam and light elements as beryllium or lithium. Depending on the power of the accelerator and the number of target stations and instruments such a source can be equivalent to small and medium flux reactor or spallation based neutron sources. With the aim to design CANS to be operated at universities, research institutes or industry laboratories a conceptual design report has been developed at JCNS for a small neutron source named NOVA ERA (Neutrons Obtained Via Accelerator for Education and Research Activities). Such a neutron source can be built at low cost with low maintenance efforts and without nuclear licencing procedure as small accelerator facility. Main features of this new concept will be presented and discussed.
000851215 536__ $$0G:(DE-HGF)POF3-6G15$$a6G15 - FRM II / MLZ (POF3-6G15)$$cPOF3-6G15$$fPOF III$$x0
000851215 536__ $$0G:(DE-HGF)POF3-6G4$$a6G4 - Jülich Centre for Neutron Research (JCNS) (POF3-623)$$cPOF3-623$$fPOF III$$x1
000851215 65027 $$0V:(DE-MLZ)SciArea-220$$2V:(DE-HGF)$$aInstrument and Method Development$$x0
000851215 65017 $$0V:(DE-MLZ)GC-2002-2016$$2V:(DE-HGF)$$aInstrument and Method Development$$x0
000851215 693__ $$0EXP:(DE-MLZ)NOSPEC-20140101$$5EXP:(DE-MLZ)NOSPEC-20140101$$eNo specific instrument$$x0
000851215 909CO $$ooai:juser.fz-juelich.de:851215$$pVDB$$pVDB:MLZ
000851215 9101_ $$0I:(DE-588b)5008462-8$$6P:(DE-Juel1)168124$$aForschungszentrum Jülich$$b0$$kFZJ
000851215 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$$x0
000851215 9131_ $$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$$vFacility topic: Neutrons for Research on Condensed Matter$$x1
000851215 9141_ $$y2018
000851215 9201_ $$0I:(DE-Juel1)JCNS-FRM-II-20110218$$kJCNS (München) ; Jülich Centre for Neutron Science JCNS (München) ; JCNS-FRM-II$$lJCNS-FRM-II$$x0
000851215 9201_ $$0I:(DE-Juel1)JCNS-1-20110106$$kNeutronenstreuung ; JCNS-1$$lNeutronenstreuung $$x1
000851215 9201_ $$0I:(DE-Juel1)JCNS-2-20110106$$kJCNS-2$$lStreumethoden$$x2
000851215 980__ $$aconf
000851215 980__ $$aVDB
000851215 980__ $$aI:(DE-Juel1)JCNS-FRM-II-20110218
000851215 980__ $$aI:(DE-Juel1)JCNS-1-20110106
000851215 980__ $$aI:(DE-Juel1)JCNS-2-20110106
000851215 980__ $$aUNRESTRICTED