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Sss mfmr

Manufactured by Nanosensors

The SSS-MFMR is a high-precision laboratory instrument designed for the measurement and analysis of magnetic fields. The device utilizes a state-of-the-art sensor technology to accurately detect and record magnetic field fluctuations. Its core function is to provide researchers and scientists with detailed data on the magnetic properties of various materials and systems under investigation.

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2 protocols using sss mfmr

1

Magnetic Skyrmions in Pt/Co/Gd Multilayers

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Films were grown by magnetron sputtering at a base pressure below 1 × 10−8 Torr. The sample structure was substrate/Ta(2)/Pt(3)/[Co(1.95)/Gd(1.2)/Pt(3)]7 (with thicknesses given in parentheses in nanometres). The hysteresis loop measured by Polar MOKE at room temperature is shown in supplementary Fig. 2a.
L-TEM measurements with a tilting angle of 10° were conducted to observe the magnetic structures and confirm the skyrmion type in the multilayer structure at room temperature. The sample deposited on a 50-nm-thick silicon nitride membrane (CleanSiN) was used for L-TEM measurements. As shown in supplementary Fig. 2b, the magnetization reversal process, and Néel-type skyrmions in the Pt/Co/Gd multilayers are confirmed35 (link),46 (link).
MFM measurements were conducted with the MFP-3D Infinity atomic force microscope, using the high-resolution and low-moment magnetic probe, SSS-MFMR (Nanosensors), with a lifted height of 30 nm.
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2

Cryogenic Magnetic Force Microscopy

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Room temperature MFM experiments were carried out using a Veeco Dimension 3100 Scanning Probe Microscope. The MFM tips used (Nanosensors SSS-MFMR) were ≈30 nm in diameter, with low coercivity (≈12 mT) and ultralow magnetic moment (≈80 emu/cc). Samples were initially saturated in the out of plane (OP) direction using fields up to H = −0.5 T. The measurements were performed in OP fields starting from H = 0 and incrementally approaching H = +HS, with a typical tip height of 20 nm. The field evolution of the spin textures is presented in Section 1 of the Supplementary Information. Low T (5–200 K) MFM imaging is carried out using a cryogenic frequency-modulated MFM system9 (link). We used two commercial probes by Team Nanotec, model ML3 (35–40 nm Co alloy coating), with f0 ≈ 75 kHz and k0 ≈ 1 N/m. The sample was first stabilized at a given temperature and then magnetized in the OP direction by applying H > HS. After saturation, MFM images were acquired at various field values as H was swept from −HS to +HS. The details of the MFM image analysis are reported in our earlier reports5 (link),9 (link),30 (link).
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