. 2020 Mar 27;6(13):eaay5986. doi: 10.1126/sciadv.aay5986

Table 2. Modeled and measured strain components of the BPI₍₁₁₀₎ lattices after the martensitic transformation from BPII₍₁₀₀₎.

ϵ_b and ϵ_c are the normal strain components in their lattice coordination, and ϵ_x, ϵ_y, and γ_xy are the strain components in the xy global coordination.

Lattice		θ (°)	ϵ_b	ϵ_c	ϵ_x	ϵ_y	γ_xy
Modeled	BPI_{(110), −9.75°}	−9.75	−0.172	0.172	−0.162	0.162	−0.115
	BPI_{(110), −80.25°}	−80.25	−0.172	0.172	0.162	−0.162	−0.115
	BPI_{(110), 9.75°}	9.75	−0.172	0.172	−0.162	0.162	0.115
	BPI_{(110), 80.25°}	80.25	−0.172	0.172	0.162	−0.162	0.115
Measured	BPI_{(110), −9.75°}	−9.52	−0.171	0.163	−0.162	0.154	−0.109
	BPI_{(110), −80.25°}	−80.77	−0.170	0.157	0.149	−0.162	−0.104
	BPI_{(110), 9.75°}	10.55	−0.166	0.179	−0.154	0.168	0.124
	BPI_{(110), 80.25°}	81.3	−0.161	0.166	0.159	−0.153	0.098

Table 2. Modeled and measured strain components of the BPI(110) lattices after the martensitic transformation from BPII(100).

Table 2. Modeled and measured strain components of the BPI₍₁₁₀₎ lattices after the martensitic transformation from BPII₍₁₀₀₎.