001034061 001__ 1034061 001034061 005__ 20250701125920.0 001034061 037__ $$aFZJ-2024-06882 001034061 1001_ $$aSchweika, Werner$$b0 001034061 1112_ $$aFlipper 2024 as a satellite workshop of the ILL/ESS user meeting$$cInstitut Laue-Langevin (ILL) located on the European Photon and Neutron (EPN) campus$$d2024-12-11 - 2024-12-13$$wFrance 001034061 245__ $$aSpherical neutron polarimetry at MAGiC 001034061 260__ $$c2024 001034061 3367_ $$033$$2EndNote$$aConference Paper 001034061 3367_ $$2BibTeX$$aINPROCEEDINGS 001034061 3367_ $$2DRIVER$$aconferenceObject 001034061 3367_ $$2ORCID$$aCONFERENCE_POSTER 001034061 3367_ $$2DataCite$$aOutput Types/Conference Poster 001034061 3367_ $$0PUB:(DE-HGF)24$$2PUB:(DE-HGF)$$aPoster$$bposter$$mposter$$s1734001941_5471$$xInvited 001034061 520__ $$aSpherical neutron polarimetry has been routinely established using Cryopad [1], measuring in zerofieldthe full polarization tensor for single Bragg peaks. This is a precise tool perfectly suited formonochromatic instruments at reactor sources. How to achieve this goal at ESS and at pulsed sourcesin general with polychromatic beams?There are two feasible solutions. Since such experiments are essentially not limited by flux, a straightforwardsolution for pulsed sources would be to use the Cryopad as a sample environment at instrumentsthat are already equipped for longitudinal polarization analysis.Here we consider an alternative approach based on a precession technique [2,3] that can be fullyadapted to a pulsed, polychromatic neutron beam to cover a large section of the reciprocal space intime-of-flight Laue diffraction. Since this method accepts the non-precessing component for polarizationanalysis, it applies as well to inelastic scattering. In order to make use of the full wavelengthband, the π/2-flipper, which initiates the precession mode, needs to be ramped in time accordingto the neutron’s wavelength and its time-of-flight. A common phase of the precession angle at thesample is not a necessary requirement but can be favorably achieved by an additional spin-echosetup. For an instrument like MAGiC at ESS, spherical polarization analysis can be a straightforwardextension of the existing setup for longitudinal polarization analysis. We are considering thispotential upgrade for the MAGiC instrument and present a relatively simple scheme how to modifythe magnetic field setup for the incoming beam to enable spherical polarimetry. Full simulationsof the polarized neutron transport not only demonstrate the feasibility of spherical polarimetry butalso its excellent performance.[1] Tasset, F. (1989). “Zero field neutron polarimetry”. Physica B: Condensed Matter, 156, 627-630.[2] Schweika, W. (2003). “Time-of-flight and vector polarization analysis for diffuse neutron scattering.”Physica B: Condensed Matter 335 (1 - 4), 157 -163. https://doi.org/10.1016/S0921-4526(03)00229-1[3] Schweika, W., Easton, S., & Neumann, K. U. (2005). “Vector Polarization Analysis on DNS”. NeutronNews, 16(2), 14-17. https://doi.org/10.1080/10448630500454262 001034061 536__ $$0G:(DE-HGF)POF4-632$$a632 - Materials – Quantum, Complex and Functional Materials (POF4-632)$$cPOF4-632$$fPOF IV$$x0 001034061 536__ $$0G:(DE-HGF)POF4-6G4$$a6G4 - Jülich Centre for Neutron Research (JCNS) (FZJ) (POF4-6G4)$$cPOF4-6G4$$fPOF IV$$x1 001034061 7001_ $$aVasiukov, Denis$$b1 001034061 7001_ $$aFabrèges, Xavier$$b2 001034061 7001_ $$aKlimk, Sergey$$b3 001034061 7001_ $$aSoltner, Helmut$$b4 001034061 7001_ $$aKlauser, Christine$$b5 001034061 7001_ $$aLee, Wai Tung$$b6 001034061 7001_ $$aFeygenson, Mikhail$$b7 001034061 909CO $$ooai:juser.fz-juelich.de:1034061$$pVDB 001034061 9131_ $$0G:(DE-HGF)POF4-632$$1G:(DE-HGF)POF4-630$$2G:(DE-HGF)POF4-600$$3G:(DE-HGF)POF4$$4G:(DE-HGF)POF$$aDE-HGF$$bForschungsbereich Materie$$lVon Materie zu Materialien und Leben$$vMaterials – Quantum, Complex and Functional Materials$$x0 001034061 9131_ $$0G:(DE-HGF)POF4-6G4$$1G:(DE-HGF)POF4-6G0$$2G:(DE-HGF)POF4-600$$3G:(DE-HGF)POF4$$4G:(DE-HGF)POF$$aDE-HGF$$bForschungsbereich Materie$$lGroßgeräte: Materie$$vJülich Centre for Neutron Research (JCNS) (FZJ)$$x1 001034061 9141_ $$y2024 001034061 9201_ $$0I:(DE-Juel1)JCNS-2-20110106$$kJCNS-2$$lStreumethoden$$x0 001034061 9201_ $$0I:(DE-82)080009_20140620$$kJARA-FIT$$lJARA-FIT$$x1 001034061 9201_ $$0I:(DE-Juel1)ZEA-1-20090406$$kZEA-1$$lZentralinstitut für Technologie$$x2 001034061 9201_ $$0I:(DE-Juel1)JCNS-ESS-20170404$$kJCNS-ESS$$lJCNS-ESS$$x3 001034061 980__ $$aposter 001034061 980__ $$aVDB 001034061 980__ $$aI:(DE-Juel1)JCNS-2-20110106 001034061 980__ $$aI:(DE-82)080009_20140620 001034061 980__ $$aI:(DE-Juel1)ZEA-1-20090406 001034061 980__ $$aI:(DE-Juel1)JCNS-ESS-20170404 001034061 980__ $$aUNRESTRICTED 001034061 981__ $$aI:(DE-Juel1)ITE-20250108