“…1 and identified as R 2 →Y 3 in Fig. 2, have been measured at ten different temperatures ranging from 10 to 300 K. Figure 3 portrays the R 1 →X 5 and R 2 →Y 3 inter-Stark transitions within the 4 F 3/2 , 4 I 9/2 , and 4 I 11/2 intermanifolds of Nd 3ϩ ions in BAMGAR at 300 K. 6 According to the ion-phonon interaction theory, 8-10,12-16 the linewidths of the R 1 →X 5 and R 2 →Y 3 inter-Stark transitions arise from the crystal strain inhomogeneity, direct onephonon processes, multiphonon processes, and Raman phonon scattering processes. As the crystal temperature increases, the spectral line widths increase.…”