Traditional metallic alloys are mixtures of elements in which the atoms of minority species tend to be distributed randomly if they are below their solubility limit, or to form secondary phases if they are above it. The concept of multiple-principal-element alloys has recently expanded this view, as these materials are single-phase solid solutions of generally equiatomic mixtures of metallic elements. This group of materials has received much interest owing to their enhanced mechanical properties 1-5. They are usually called medium-entropy alloys in ternary systems and high-entropy alloys in quaternary or quinary systems, alluding to their high degree of configurational entropy. However, the question has remained as to how random these solid solutions actually are, with the influence of short-range order being suggested in computational simulations but not seen experimentally 6,7. Here we report the observation, using energy-filtered transmission electron microscopy, of structural features attributable to short-range order in the CrCoNi medium-entropy alloy. Increasing amounts of such order give rise to both higher stacking-fault energy and hardness. These findings suggest that the degree of local ordering at the nanometre scale can be tailored through thermomechanical processing, providing a new avenue for tuning the mechanical properties of medium-and high-entropy alloys. Among the increasing number of medium-to high-entropy alloy systems reported in the literature 8-12 , the CrCoNi-based, face-centred-cubic (fcc) single-phase alloys exhibit an exceptional combination of mechanical properties, including high strength, tensile ductility, fracture toughness and impact resistance 13. Extensive studies have documented the deformation mechanisms in these alloys. Gludovatz et al. reported the outstanding fracture toughness of CrCoNi at cryogenic temperatures 14 , and attributed this to a synergy of deformation mechanisms, including a propensity for mechanical twinning 15. Interestingly, computational work has suggested that the CrCoNi-based fcc single-phase alloys should have near-zero or negative stacking-fault energies (SFEs; γ SF) 15-19. However, these computational predictions do not agree with measured values 20,21 (γ SF_CrCoNi ≈ 22 mJ m −2 and γ SF_CrMnFeCoNi ≈ 30 mJ m −2). Experimentally, the measured SFEs in medium-entropy alloys (MEAs) and high-entropy alloys (HEAs) exhibit a wide distribution 22 , indicating a strong dependence of γ SF on local atomic configuration. Ding et al. 6 showed that the SFE of CrCoNi MEA can be tailored over a wide range by tuning its local chemical order. The work highlights the potentially strong impact of chemical short-range order (SRO) on the mechanical properties of the MEA/HEAs. Later, Li et al. 7 , using molecular dynamics simulations, demonstrated the ruggedness of the local energy landscape and how it raises activation barriers governing dislocation activities. Experimental evidence for the existence of such SRO has so far been limited to X-ray adsorption measurements 23 that are averaged over a relatively large volume of material. Indeed, further efforts are needed to characterize the degree and the spatial extent of the ordering , as well as how both would be affected by thermal history and any associated effects on mechanical behaviour. Here we provide quantitative visualization of the SRO structure, by which we establish a direct effect of this SRO on the mechanical behaviour of MEA/HEA materials. To investigate the presence of chemical SRO, samples of equiatomic CrCoNi alloys were subjected to different thermal treatments after homogenization at 1,200 °C: (1) water-quenched to room temperature to suppress SRO formation; or (2) aged at 1,000 °C for 120 h followed by slow furnace cooling to promote SRO formation. The microstructure and the degree of SRO were characterized with a variety of transmission electron microscope (TEM) imaging techniques. Diffraction contrast from SRO is inherently faint as compared to the fcc matrix lattice dif-fraction signal because the former arises from relatively minor differences in lattice distortion. As a result, measurement of the faint SRO diffraction signal has proven to be challenging. In order to enhance the signal-to-noise ratio of the diffraction contrast from SRO, we minimized the background noise from inelastic scattering by using a Zeiss TEM (LIBRA 200MC) equipped with an in-column Ω energy filter and a camera with 16-bit dynamic range. Energy-filtered diffraction patterns and dark-field images for the two heat treatment conditions are shown in Fig. 1. In the diffraction patterns (Fig. 1a, b), streaks along {111} directions between fcc Bragg spots are clearly observed in the aged sample. Dark-field imaging taken with the objective aperture positioned in the centre of the streaked region shown in Fig. 1b was used to image the https://doi.