“…In state B, the recrystallisation that occurs during ␥ growth destroys the habitual N-W and K-S orientation relationships between the ␥ and ␣ phases and leads to a more random misorientation between these phases. This means that the main difference between the two states results in special IBs structure that is characterized by low energy in state A (where the IBs fulfill special ORs) and is random in state B (for which the IBs deviate from special ORs) [6]. Samples in the form of bars (8 mm in diameter) were machined to reduce their diameter to 3 mm and next sliced to 0.2 mm thick discs using a wire saw.…”