[1] De Cooman, B. C., Estrin, Y., Kim, S. K. Twinning-induced plasticity (TWIP) steels. Acta Mater. 142, 283-362 (2018).
[2] Bouaziz, O., Allain, S., Scott, C. P., Cugy, P., Barbier, D. High manganese austenitic twinning induced plasticity steels: A review of the microstructure properties relationships. Curr. Opin. Solid State Mat. Sci. 15, 141-168 (2011).
[3] Liang, Z. Y., Li, Y. Z., Huang, M. X. The respective hardening contributions of dislocations and twins to the flow stress of a twinning-induced plasticity steel. Scr. Mater. 112, 28-31 (2016).
[4] Fu, X., Wu, X., Yu, Q. Dislocation plasticity reigns in a traditional twinning-induced plasticity (TWIP) steel by in situ observation. Mater. Today Nano 3, 48-53 (2018).
[5] Grässel, O., Krüger, L., Frommeyer, G., Meyer, L. W. High strength Fe-Mn-(Al, Si) TRIP/TWIP steels development - properties - application. Int. J. Plast. 16, 1391-1409 (2000).
[6] Frommeyer, G., Brüx, U., Neumann, P. Supra-ductile and high-strength manganese-TRIP/TWIP Steels for high energy absorption purposes. ISIJ Int. 43, 438-446 (2003).
[7] Deng, Y. et al. Design of a twinning-induced plasticity high entropy alloy. Acta Mater. 94, 124-133 (2015).
[8] Karaman, I. et al. Modeling the deformation behavior of Hadfield steel single and polycrystals due to twinning and slip. Acta Mater. 48, 2031-2047 (2000).
[9] Lu, K., Lu, L., Suresh, S. Strengthening materials by engineering coherent internal boundaries at the nanoscale. Science 324, 349-352 (2009).
[10] Venables, J. A. Deformation twinning in face-centred cubic metals. Philos. Mag. 6, 379-396 (1961).
[11] Mahajan, S., Chin, G. Y. Formation of deformation twins in f.c.c. crystals. Acta Metall. 21, 1353-1363 (1973).
[12] Christian, J. W., Mahajan, S. Deformation twinning. Prog. Mater. Sci. 39, 1-157 (1995).
[13] Husser, E., Bargmann, S. Modeling twinning-induced lattice reorientation and slip-in-twin deformation. J. Mech. Phys. Solids 122, 315-339 (2019).
[14] Asgari, S., El-Danaf, E., Kalidindi, S. R., Doherty, R. D. Strain hardening regimes and microstructural evolution during large strain compression of low stacking fault energy fcc alloys that form deformation twins. Metall. Mater. Trans. A, 28, 1781-1795 (1997).
[15] Lu, L., Chen, X., Huang, X., Lu, K. Revealing the maximum strength in nanotwinned copper. Science 323, 607-610 (2009).
[16] Beladi, H. et al. Orientation dependence of twinning and strain hardening behaviour of a high manganese twinning induced plasticity steel with polycrystalline structure. Acta Mater. 59, 7787-7799 (2011).
[17] Rémy, L. Twin-slip interaction in f.c.c. crystals. Acta Metall. 25, 711-714 (1977).
[18] Li, X., Wei, Y., Lu, L., Lu, K., Gao, H. Dislocation nucleation governed softening and maximum strength in nano-twinned metals. Nature 464, 877-880 (2010).
[19] Taheri Mousavi, S. M., Zhou, H., Zou, G., Gao, H. Transition from source- to stress-controlled plasticity in nanotwinned materials below a softening temperature. npj Comput. Mater. 5, 2 (2019).
[20] Wang, Y. B., Sui, M. L., Ma, E. In situ observation of twin boundary migration in copper with nanoscale twins during tensile deformation. Philos. Mag. Lett. 87, 935-942 (2007).
[21] Chen, S. et al. Real-time observations of TRIP-induced ultrahigh strain hardening in a dual-phase CrMnFeCoNi high-entropy alloy. Nat. Commun. 11, 826 (2020).
[22] Ranganathan, S. On the geometry of coincidence-site lattice. Acta Crystallogr. 21, 197-199 (1966).
[23] Randle, V. Twinning-related grain boundary engineering. Acta Mater. 52, 4067-4081 (2004).
[24] Randle, V., Coleman, M., Waterton, M. The Role of Σ9 Boundaries in Grain Boundary Engineering. Metall. Mater. Trans. A 42, 582-586 (2011).
[25] Liu, L., Wang, J., Gong, S. K., Mao, S. X. High resolution transmission electron microscope observation of zero-strain deformation twinning mechanisms in Ag. Phys. Rev. Lett. 106, 175504 (2011).
[26] Wang, J., Anderoglu, O., Hirth, J. P., Misra, A., Zhang, X. Dislocation structures of Σ3 {112} twin boundaries in face centered cubic metals. Appl. Phys. Lett. 95, 021908 (2009).
[27] Lucadamo, G., Medlin, D. L. Geometric Origin of Hexagonal Close Packing at a Grain Boundary in Gold. Science 300, 1272-1275 (2003).
[28] Ernst, F. et al. Theoretical prediction and direct observation of the 9R structure in Ag. Phys. Rev. Lett. 69, 620-623 (1992).
[29] Wolf, U., Ernst, F., Muschik, T., Finnis, M. W., Fischmeister, H. F. The influence of grain boundary inclination on the structure and energy of σ = 3 grain boundaries in copper. Philos. Mag. A 66, 991-1016 (1992).
[30] Zhang, Z. et al. Nanoscale origins of the damage tolerance of the high-entropy alloy CrMnFeCoNi. Nat. Commun. 6, 10143 (2015).
[31] Zhang, Z. et al. Dislocation mechanisms and 3D twin architectures generate exceptional strength-ductility-toughness combination in CrCoNi medium-entropy alloy. Nat. Commun. 8, 14390 (2017).
[32] Priester, L., Khalfallah, O. Image force on a lattice dislocation due to a grain boundary in anisotropic f.c.c. materials. Philos. Mag. A 69, 471-484 (1994).
[33] Plimpton, S. Fast parallel algorithms for short range molecular dynamicas. J. Comput. Phys. 117, 1–19 (1995).
[34] Choi, W. M., Jo, Y. H., Sohn, S. S., Lee, S., Lee, B.-J. Understanding the physical metallurgy of the CoCrFeMnNi high-entropy alloy: an atomistic simulation study. npj Comput. Mater. 4, 1 (2018).
[35] Li, Q. J., Sheng, H., Ma, E. Strengthening in multi-principal element alloys with local-chemical-order roughened dislocation pathways. Nat. Commun. 10, 3563 (2019).
[36] Sheng, H. W., Kramer, M. J., Cadien, A., Fujita, T., Chen, M. W. Highly optimized embedded-atom-method potentials for fourteen fcc metals. Phys. Rev. B 83, 134118 (2011).