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Abstract
In chiral cubic helimagnets, phases of magnetic skyrmions—topologically protected spin whirls—are stabilized by thermal fluctuations over a narrow region directly below the magnetic ordering temperature Tc. Due to often being touted for use in applications, there is a high demand to identify new ways to stabilize equilibrium skyrmion phases far below Tc where they may display an enhanced robustness against external perturbation due to a larger magnetic order parameter. Here, from quantum beam experiments on the chiral magnet Co7Zn7Mn6, we unveil a direct correlation between the stability of its second skyrmion phase-stable far from Tc, and a concomitant enhancement of an underlying magnetic fluctuation rate that is driven by geometric magnetic frustration. The influences of other leading skyrmion stability mechanisms, such as those derived from thermal fluctuations and low T cubic anisotropies, are shown to be weak in this system. We therefore advance the existence of a fundamental mechanism for stabilizing topological skyrmions in Co7Zn7Mn6 chiral magnet that draws upon magnetic frustration as the key ingredient.
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1 Paul Scherrer Institute (PSI), Laboratory for Neutron Scattering and Imaging (LNS), Villigen, Switzerland (GRID:grid.5991.4) (ISNI:0000 0001 1090 7501)
2 RIKEN Center for Emergent Matter Science (CEMS), Wako, Japan (GRID:grid.474689.0)
3 Condensed Matter Theory Group, Paul Scherrer Institute (PSI), Villigen, Switzerland (GRID:grid.5991.4) (ISNI:0000 0001 1090 7501)
4 Paul Scherrer Institute (PSI), Laboratory for Muon Spin Spectroscopy (LMU), Villigen, Switzerland (GRID:grid.5991.4) (ISNI:0000 0001 1090 7501)
5 Institut Laue-Langevin, Grenoble, France (GRID:grid.156520.5) (ISNI:0000 0004 0647 2236)
6 National Institute for Materials Science (NIMS), Research and Services Division of Materials Data and Integrated System (MaDIS), Tsukuba, Japan (GRID:grid.21941.3f) (ISNI:0000 0001 0789 6880); PRESTO, Japan Science and Technology Agency (JST), Kawaguchi, Japan (GRID:grid.419082.6) (ISNI:0000 0004 1754 9200)
7 National Institute for Materials Science (NIMS), Research and Services Division of Materials Data and Integrated System (MaDIS), Tsukuba, Japan (GRID:grid.21941.3f) (ISNI:0000 0001 0789 6880)
8 Paul Scherrer Institute (PSI), Laboratory for Neutron Scattering and Imaging (LNS), Villigen, Switzerland (GRID:grid.5991.4) (ISNI:0000 0001 1090 7501); Institute of Physics, École Polytechnique Fédérale de Lausanne (EPFL), Laboratory for Ultrafast Microscopy and Electron Scattering (LUMES), Lausanne, Switzerland (GRID:grid.5333.6) (ISNI:0000000121839049); Institute of Materials, École Polytechnique Fédérale de Lausanne (EPFL), Laboratory of Nanoscale Magnetic Materials and Magnonics (LMGN), Lausanne, Switzerland (GRID:grid.5333.6) (ISNI:0000000121839049)
9 Swiss Light Source, Paul Scherrer Institute (PSI), Villigen, Switzerland (GRID:grid.5991.4) (ISNI:0000 0001 1090 7501)
10 Synchrotron SOLEIL, Gif-sur-Yvette Cedex, France (GRID:grid.426328.9)
11 University of Tokyo, Department of Advanced Materials Science, Kashiwa, Japan (GRID:grid.26999.3d) (ISNI:0000 0001 2151 536X)
12 École Polytechnique Fédérale de Lausanne (EPFL), Laboratory for Quantum Magnetism (LQM), Institute of Physics, Lausanne, Switzerland (GRID:grid.5333.6) (ISNI:0000000121839049)
13 RIKEN Center for Emergent Matter Science (CEMS), Wako, Japan (GRID:grid.474689.0); University of Tokyo, Department of Advanced Materials Science, Kashiwa, Japan (GRID:grid.26999.3d) (ISNI:0000 0001 2151 536X)
14 RIKEN Center for Emergent Matter Science (CEMS), Wako, Japan (GRID:grid.474689.0); University of Tokyo, Department of Applied Physics, Tokyo, Japan (GRID:grid.26999.3d) (ISNI:0000 0001 2151 536X); University of Tokyo, Tokyo College, Tokyo, Japan (GRID:grid.26999.3d) (ISNI:0000 0001 2151 536X)