“…[10] The sequence of invariant reactions in the Fe-N-C system possibly met upon cooling at T 1000 K (727°C) can be visualized in a Scheil reaction scheme [39][40][41] as shown in Figure 1. From the binary systems, the congruent transition c [Fe-N, e Ð c 0 , 953 K (677°C) [8] ] as well as the well-established eutectoid reactions e 1 [Fe-C, c Ð a þ h, 1000 K (727°C) [9] ], e 2 [Fe-N, e Ð c þ c 0 , 923 K (650 C) [8] ], and e 3 [Fe-N, c Ð a þ c 0 , 865 K (592°C) [8] ] are inherited, giving rise to two-phase (c 0 þ e) and three-phase (a þ c þ h; c þ c 0 þ e; a þ c þ c 0 ; in that order upon decreasing temperature) fields in the ternary system. In the ternary system, at high temperatures, an equilibrium between c and h exists, vanishing upon cooling and being replaced by the a þ e equilibrium via the U 1 invariant reaction, c þ h Ð a þ e. Upon further cooling, the c phase vanishes via the ternary eutectoid reaction E 1 , c Ð a þ c 0 þ e. Both reactions (U 1 and E 1 ) involving the c phase have been investigated recently in an experimental study of the Fe-N-C system [32] *; the temperature of the invariant reaction U 1 , as first determined in Reference 32 to occur between 868 K and 873 K (595°C to 600°C), was confirmed in Reference 42. in the system Fe-N-C leading to the replacement of the a þ e equilibrium by the c 0 þ h equilibrium upon cooling.…”