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In this ๐—ฎ๐—ฝ๐—ฝ๐—น๐—ถ๐—ฐ๐—ฎ๐˜๐—ถ๐—ผ๐—ป ๐—ป๐—ผ๐˜๐—ฒ, you will learn about ๐—ณ๐—ถ๐—ฒ๐—น๐—ฑ-๐˜€๐˜„๐—ถ๐˜๐—ฐ๐—ต๐—ฎ๐—ฏ๐—น๐—ฒ ๐— ๐—ฎ๐—ด๐—ป๐—ฒ๐˜๐—ถ๐—ฐ ๐—™๐—ถ๐—ฒ๐—น๐—ฑ ๐—š๐—ฒ๐—ป๐—ฒ๐—ฟ๐—ฎ๐˜๐—ผ๐—ฟ (๐—™-๐˜€ ๐— ๐—™๐—š) that enables precise in-plane and out-of-plane magnetic fields during in-situ MFM imaging. It allows real-time observation of magnetization switching in thin films and artificial spin ice lattices, with controlled fields up to ~205 G. Available on ๐—ก๐—ซ ๐—ฎ๐—ป๐—ฑ ๐—™๐—ซ ๐—”๐—™๐—  ๐—ฝ๐—น๐—ฎ๐˜๐—ณ๐—ผ๐—ฟ๐—บ๐˜€, the MFG (developed by Caylar SAS) is a precise and flexible solution that ๐—ฝ๐—ฟ๐—ผ๐˜ƒ๐—ถ๐—ฑ๐—ฒ๐˜€ ๐—ฑ๐—ถ๐—ฟ๐—ฒ๐—ฐ๐˜ ๐—ฐ๐—ผ๐—ฟ๐—ฟ๐—ฒ๐—น๐—ฎ๐˜๐—ถ๐—ผ๐—ป ๐—ฏ๐—ฒ๐˜๐˜„๐—ฒ๐—ฒ๐—ป ๐—ฎ๐—ฝ๐—ฝ๐—น๐—ถ๐—ฒ๐—ฑ ๐—ณ๐—ถ๐—ฒ๐—น๐—ฑ๐˜€ ๐—ฎ๐—ป๐—ฑ ๐—ป๐—ฎ๐—ป๐—ผ๐˜€๐—ฐ๐—ฎ๐—น๐—ฒ ๐—บ๐—ฎ๐—ด๐—ป๐—ฒ๐˜๐—ถ๐—ฐ ๐˜€๐˜๐—ฎ๐˜๐—ฒ๐˜€, advancing thin-film material characterization. ๐Ÿ“œ๐—ฅ๐—ฒ๐—ฎ๐—ฑ ๐˜๐—ต๐—ฒ ๐—ฎ๐—ฝ๐—ฝ๐—น๐—ถ๐—ฐ๐—ฎ๐˜๐—ถ๐—ผ๐—ป ๐—ป๐—ผ๐˜๐—ฒ: https://okt.to/FAV8c1 Image captions: 1: MFM phase data collected at various in-plane magnetic field strengths. A: 155 G, all pairs in the initial state. B: 170 G, most pairs in a disordered partially switched state. C: 205 G, all pairs in fully switched state. The red box outlines the same pair in each image to more easily observe the changes. D. MFG mounted on the Park AFM 2: Representative lattice interface state configurations #ParkSystems #AFM #MFM #ThinFilms #Magnetics #Nanotechnology #MaterialsScience

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