Ukleev, VKarube, K.Derlet, P. M.Wang, C. N.Luetkens, H.Morikawa, D.Kikkawa, A.Mangin-Thro, L.Wildes, A. R.Yamasaki, Y.Yokoyama, Y.Yu, L.Piamonteze, C.Jaouen, N.Tokunaga, Y.Ronnow, H. M.Arima, T.Tokura, Y.Taguchi, Y.White, J. S.2021-05-222021-05-222021-05-222021-04-2310.1038/s41535-021-00342-5https://infoscience.epfl.ch/handle/20.500.14299/178328WOS:000642904200002In 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 T-c. 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 T-c 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 T-c, 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.Materials Science, MultidisciplinaryQuantum Science & TechnologyPhysics, AppliedPhysics, Condensed MatterMaterials SciencePhysicsbeta-mnmu-srcircular-dichroismspin fluctuationschiral magnettransitionlatticestatescatteringdisordertext::journal::journal article::research article