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Page 10 of 21                         Zhou et al. J Mater Inf 2022;2:18  https://dx.doi.org/10.20517/jmi.2022.27























                Figure 9. (A) Tensile stress-strain curve of as-printed CoCrFeMnNi HEA in different atmospheres with work hardening rate curve
                inserted. (B) Schematic diagram showing the in situ doping of nitrogen through the L-PBF process under a reactive N  atmosphere and
                                                             [92]                             2
                the inset showing the annular bright-field STEM image of N-50 HEA  .






















                                                                                                       [83]
                Figure 10. Microstructure and tensile properties of ODS HEA by L-PBF and schematic diagram showing oxide formation mechanism  .
                ODS: oxide-dispersion-strengthened; HEA: high-entropy alloys.
                                                               [96,97]
               resistance of the FeCoCrNiMn HEA fabricated by L-PBF  .

               An incoherent interface is prone to cause stress concentration during deformation. Thus, the contents of the
               incoherent precipitations are usually controlled to a low level, which in turn limits their strengthening
               effects on the matrix. As discussed above, the L1  precipitation coherent with the FCC HEA matrix can
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               maintain a high content, significantly improving the tensile strength without sacrificing ductility. Mu et al.
               broke the strength-ductility trade-off by introducing high-density dislocation networks and disordered L1
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               precipitates to the FCC HEA matrix (Fe Co Ni Al Ti , at. %) through the L-PBF and the subsequent
                            [89]                  28  29.5  27.5  8.5  6.5
               heat treatment . Compared with the conventional L1 -strengthened HEA, the pre-existing high-density
                                                              2
               dislocation networks of the as-printed sample provided a fast diffusion channel for the solute atoms.
               Therefore, the L1  precipitation was preferentially formed near the high-density dislocation networks during
                              2
               the aging process. Thus, an ultrahigh strength of ~1.8 GPa and a maximum elongation of ~16% were
               achieved for the as-printed FeCoNiAlTi HEA after aging at 780 °C for 4 h [Figure 11A]. The large ductility
               mainly came from the evolution of multiple stacking faults (SFs) [Figure 11B], while the ultrahigh strength
               was mainly derived from dislocation-precipitation synergistic strengthening [Figure 11C and D]. This work
               provided an efficient method to develop high-performance HEAs by simultaneously introducing
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