“…This mosaic block model is commonly applied to relaxed heteroepitaxial layers [11,12] including Ge/Si (0 0 1) [13], InAs/GaAs (0 0 1) and GaAs/InAs (0 0 1) [14], InAsP/InP (0 0 1) [15], InAs x Sb 1 À x /GaAs (0 0 1) [16], GaN/sapphire (0 0 0 1) [17], GaN/SiC (0 0 0 1) [18], ZnTe/GaAs (0 0 1) [19], ZnSe/GaAs (0 0 1) [20], and PbSe/BaF 2 (0 1 1) [21]. According to this model the dislocations broaden the X-ray rocking curve for a semiconductor crystal in two ways: (i) dislocations introduce rotations of the crystal lattice (''angular broadening''); and (ii) dislocations are surrounded by strained regions of the crystal, in which the Bragg angle is nonuniform (''strain broadening'').…”