001 | 1034064 | ||
005 | 20241213210713.0 | ||
037 | _ | _ | |a FZJ-2024-06885 |
100 | 1 | _ | |a Stellhorn, Annika |b 0 |
111 | 2 | _ | |a Flipper 2024 as a satellite workshop of the ILL/ESS user meeting |c Institut Laue-Langevin (ILL) located on the European Photon and Neutron (EPN) campus |d 2024-12-11 - 2024-12-13 |w France |
245 | _ | _ | |a Chiral magnetic structures probed by SANS & GISANS |
260 | _ | _ | |c 2024 |
336 | 7 | _ | |a Conference Paper |0 33 |2 EndNote |
336 | 7 | _ | |a Other |2 DataCite |
336 | 7 | _ | |a INPROCEEDINGS |2 BibTeX |
336 | 7 | _ | |a conferenceObject |2 DRIVER |
336 | 7 | _ | |a LECTURE_SPEECH |2 ORCID |
336 | 7 | _ | |a Conference Presentation |b conf |m conf |0 PUB:(DE-HGF)6 |s 1734081867_7856 |2 PUB:(DE-HGF) |x Invited |
520 | _ | _ | |a Chiral magnetic structures in single crystals and thin film structures probed by polarization-analyzedSmall Angle Neutron Scattering (SANS) & Grazing-Incidence-SANS are often connected to complexanalysis procedures and require the development of individual magnetic models. Additionally, precisedata-reduction protocols are needed to distinguish sample scattering from instrumentationaleffects. The more involved the different interactions in one sample system, the more care has tobe taken for a comprehensive understanding as function of, e.g., magnetic field, electric field, temperature,and further parameter sets. The key to a broad understanding then can be given by thecomparison of various analysis methods.Here, I will provide two examples on the complexity of magnetic (GI-)SANS data analysis on differentmaterials: (i) a ferromagnetic/superconducting thin film with temperature dependent chiralmagnetic domain walls, and (ii) a magnetoelectric single crystal with chiral magnetic phases dependingon temperature, magnetic, and electric field. For study (i) we will compare polarization-analyzedGISANS data on Nb/FePd thin films with perpendicular magnetic anisotropy with results from CDXRMS,and evaluate our conclusions together with information gained by Density Functional Theory(DFT) [1]. In study (ii), we present the dependence of magnetic chiral phases occurring in the magnetoelectricsingle crystal Ba2−xSrxMg2Fe12O22 [2] as function of temperature and magnetic field.[1] P. C. Carvalho et al., Nano Lett. 23, 4854−4861 (2023).[2] K. Zhai et al., Nature Communications 8, 519 (2017). |
536 | _ | _ | |a 632 - Materials – Quantum, Complex and Functional Materials (POF4-632) |0 G:(DE-HGF)POF4-632 |c POF4-632 |f POF IV |x 0 |
536 | _ | _ | |a 6G4 - Jülich Centre for Neutron Research (JCNS) (FZJ) (POF4-6G4) |0 G:(DE-HGF)POF4-6G4 |c POF4-6G4 |f POF IV |x 1 |
700 | 1 | _ | |a Backs, Alicia |b 1 |
700 | 1 | _ | |a Klautau, Angela |b 2 |
700 | 1 | _ | |a Blackburn, Elizabeth |b 3 |
700 | 1 | _ | |a Kentzinger, Emmanuel |b 4 |
700 | 1 | _ | |a Miranda, Ivan |b 5 |
700 | 1 | _ | |a Palm, Juan German Cornelio |b 6 |
700 | 1 | _ | |a Shen, Lingjia |b 7 |
700 | 1 | _ | |a Stepancic, Oskar |b 8 |
700 | 1 | _ | |a Lee, Wai Tung |b 9 |
909 | C | O | |o oai:juser.fz-juelich.de:1034064 |p VDB |
913 | 1 | _ | |a DE-HGF |b Forschungsbereich Materie |l Von Materie zu Materialien und Leben |1 G:(DE-HGF)POF4-630 |0 G:(DE-HGF)POF4-632 |3 G:(DE-HGF)POF4 |2 G:(DE-HGF)POF4-600 |4 G:(DE-HGF)POF |v Materials – Quantum, Complex and Functional Materials |x 0 |
913 | 1 | _ | |a DE-HGF |b Forschungsbereich Materie |l Großgeräte: Materie |1 G:(DE-HGF)POF4-6G0 |0 G:(DE-HGF)POF4-6G4 |3 G:(DE-HGF)POF4 |2 G:(DE-HGF)POF4-600 |4 G:(DE-HGF)POF |v Jülich Centre for Neutron Research (JCNS) (FZJ) |x 1 |
914 | 1 | _ | |y 2024 |
920 | 1 | _ | |0 I:(DE-Juel1)JCNS-2-20110106 |k JCNS-2 |l Streumethoden |x 0 |
920 | 1 | _ | |0 I:(DE-82)080009_20140620 |k JARA-FIT |l JARA-FIT |x 1 |
980 | _ | _ | |a conf |
980 | _ | _ | |a VDB |
980 | _ | _ | |a I:(DE-Juel1)JCNS-2-20110106 |
980 | _ | _ | |a I:(DE-82)080009_20140620 |
980 | _ | _ | |a UNRESTRICTED |
Library | Collection | CLSMajor | CLSMinor | Language | Author |
---|