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Xiao et al. Microstructures 2023;3:2023006  https://dx.doi.org/10.20517/microstructures.2022.26  Page 3 of 17

               Table 1. Summary of different categories of HEAs (at.%)
                EE issues   HE                    ITE
                HEA systems  Equiatomic CoCrNi    39.9Ni-20Co-30Fe-6Al-4Ti-0.1B
                            Equiatomic CoNiV      29.9Ni-30Co-13Fe-15Cr-6Al-6Ti-0.1B
                            Equiatomic FeCoCrNiMn  46.23Ni-23Co-10Cr-5Fe-8.5Al-4Ti-2W-1Mo-0.15C-0.1B-0.02Zr
                            97(CoCrNi)-3Mo        100-x(NbMoTaW)-xB
                            Equiatomic FeCoCrNi
                            45Fe-35Mn-10Co-10Cr
                            50Fe-30Mn-10Cr-10Co

               HEAs: High entropy alloys; EE: environmental embrittlement; HE: hydrogen embrittlement; ITE: intermediate-temperature embrittlement.





















                      Figure 1. Schematic showing EE phenomena and associated microstructural factors. EE: Environmental embrittlement.

               equiatomic CoCrNi medium entropy alloy (MEA) with ultimate tensile strength as high as ~1 GPa, as
               shown in Figure 2A . The authors argued that the superior HE resistance is primarily attributed to the
                                [51]
               enhanced dynamic strain hardening caused by hydrogen-promoted mechanical nanotwinning [Figure 2B].
               However, an inconsistent observation of this equiatomic CoCrNi MEA can be found under gas hydrogen
               charging, where the CoCrNi MEA displayed a pronounced ductility reduction (~70.9%) compared to the
               uncharged sample. Interestingly, it was further shown that boron doping (400 at. ppm) can obviously
               decrease the hydrogen-induced ductility loss (~45.8%) in this MEA, which is basically ascribed to the GB
               decoration of boron [Figure 2C-E]. The boron segregation not only significantly increases the cohesive
               strength of GBs but also reduces the hydrogen diffusivity along GBs, resulting in improved HE resistance .
                                                                                                       [49]
               Therefore, it should be noted that different hydrogen charging approaches can create distinctive mechanical
               responses in the same HEA. This is because hydrogen atoms are largely concentrated on the surface region
               of the samples via electrochemical charging, whereas hydrogen is more homogeneously distributed in the
               gas hydrogen-charged samples . In addition to the effect of boron on the resistance to HE, it was also
                                          [53]
               reported that a small addition of boron (0.2-1.6 at.%) can improve the malleability of brittle eutectic HEAs,
               which is primarily attributed to the transition in eutectic morphology from lamellar eutectic to dendrite
               eutectic. Such a transition is believed to result from the increased constitutional undercooling caused by
               boron additions .
                             [54]
               Additionally, the HE resistance of the equiatomic CoCrNi MEA can be further enhanced via Mo doping
               (~3 at.%). As shown in Figure 3, Mo can promote the formation of nanotwins (NTs) in the hydrogen-
                                                          [55]
               charged specimen during the deformation process . It was claimed that the existence of NTs can impede
               the local accumulation of hydrogen and disturb the continuous motion of dislocation interacting GBs,
               thereby inhibiting the intergranular decohesion and improving the HE resistance. Nevertheless, it is
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