By N. Yamamoto

ISBN-10: 9535103628

ISBN-13: 9789535103622

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93, 693 (1954). [44] S. Dhar and S. Ghosh, Appl. Phys. , 80, 4519 (2002). [45] V. Ursaki, I. M. Tiginyanu, P. C. Ricci, A. Anedda, S. Hubbard and D. Pavlidis, J. Appl. , 94, 3875 (2003). [46] J. Ryan, D. P. Lowney, M. O. Henry, P. J. McNally, E. McGlynn, K. Jacobs and L. Considine, Thin Solid Films, 473, 308 (2005). [47] L. Chernyak, G Nootz and A. Osinsky, Electron. , 37, 922 (2001). [48] C. Look and B. Claftin, Phys. , 241, 624 (2004). [49] O. 241-265, Edited by C. Jagadish and S. Pearton, Elsevier Ltd.

1982], are shown in brackets. A conspicuous difference appears in PCL spectra of neodymium ions in yttrium aluminates in case of different crystal structure. The spectrum of orthorhombic Nd3+:YAlO3 single crystal together with the spectrum of cubic Nd3+:Y3Al5O12 are presented in Fig. 3 as an illustration of this difference. 37 What is the Pulsed Cathodoluminescence? Nd3+:Y3Al5O12 , nm 399,2 401,6 Identification of optical trasfer 2F25/2 2F25/2 429,9 435,6 2F25/2 450,4 455,4 458,8 461,0 479,3 487,5 494,4 525,2 2F25/2 2F25/2 (0)2H9/2 (2), (397,5) (0)2H9/2 (4), (401,4) (1)4F9/2 (0), (430,2) (0)4F9/2 (2), (435,1) (2)2H11/2 (3), (450,5) (0)2H11/2 (1), (455,9) 2F25/2 (0)2H11/2 (3), (458,3) 2F25/2 (0)2H11/2 (4), (461,4) 2F25/2 (1)4G5/2 (1), (479,0) 2F25/2 (0)2G7/2 (0), (487,1) 4G11/2 (2)4I9/2 (4) (494,2) 2F25/2 (0)4G7/2 (0), (524,9) 2F25/2 540,6 2F25/2 (0)2K13/2+2G9/2 (2), (541,0) 549,1 2F25/2 (0)2K13/2+2G9/2 (7), (549,4) 557,4 562,9 2F25/2 576,4 587,4 596,2 600,6 620,1 (0)2K13/2+2G9/2 (10),(557,0) (3)4I13/2 (0), (562,6) Superposition 2G7/2 (2,3)4I9/2 (0,2), (576,3) 2K15/2 Nd3+:YAlO3 , nm 389,9 394,6 398,1 Identification of optical trasfer 2F25/2 (2)2H9/2 (0), (390,0) (0)4F5/2 (2), (394,6) 2F25/2 (0)2H9/2 (3), (398,3) 2F25/2 422,5 426,9 429,9 435,2 439,0 440,7 450,4 456,0 2D5/2 480,7 487,8 2F25/2 525,4 527,8 538,0 539,5 541,6 545,7 547,5 549,2 554,5 556,3 2F25/2 563,6 2K13/2 (4)4I11/2(1), (563,5) 585,4 2F25/2 (2)4G9/2 (4), (585,2) 602,1 610,4 612,1 615,4 620,1 622,1 625,4 638,3 639,5 646,2 652,4 660,9 665,3 668,6 2F25/2(2)4G11/2+2K15/2+2D3/2(6),(601,8) (2)4I9/2 (1), (423,0) (2)4F9/2 (3), (427,3) 2F25/2 (1)4F9/2 (0), (429,9) 2F25/2 (1)4F9/2 (1), (434,8) 2D5/2 (0)4I9/2 (4), (438,8) 2P1/2 (0) 4I9/2 (3), (441,2) 2F25/2 (2)2H11/2 (3), (450,4) 2F25/2 (1)2H11/2 (3), (456,0) 2F25/2 2F25/2 (1)4G5/2 (2), (480,5) (0)2G7/2 (2) (488,1) (1)4G7/2 (1), (525,4) (1)4G7/2 (2), (527,8) 2F25/2 (1)4G9/2 (2), (538,3) 2F25/2 (0)4G9/2 (0), (539,3) 2F25/2 (2)2K13/2 (2), (542,0) 2F25/2 (2)2K13/2 (4), (545,7) 2F25/2 (2)2K13/2 (5), (547,5) 2F25/2 (0)2K13/2 (0), (549,0) 2F25/2 (0)2K13/2 (3), (554,2) 2F25/2 (0)2K13/2 (4), (556,2) 2F25/2 2F25/2 (0)4G9/2 (0), (586,8) Superposition 2F25/2 (0)4G11/2 (0,1), (596,2) 2F25/2 (0)4G11/2 (3), (600,1) 2F25/2 (0)2K15/2 (2), (620,8) 2F25/2(0)4G11/2+2K15/2+2D3/2(4),(610,2) 2F25/2(1)4G11/2+2K15/2+2D3/2(6),(611,8) 2F25/2(2)4G11/2+2K15/2+2D3/2(13),(614,7) 2F25/2(0)4G11/2+2K15/2+2D3/2(9),(619,8) 2F25/2(1)4G11/2+2K15/2+2D3/2(11),(621,4) 2F25/2(1)4G11/2+2K15/2+2D3/2(13),(625,2) 2H11/2 (1)4I9/2 (2) (637,7) (0)4I9/2 (2) (639,1) 2H11/2 (3)4I9/2 (3) (645,4) 2H11/2 (3)4I9/2 (4) (652,6) 2G7/2 (3)4I11/2 (4) (660,8) 2G7/2 (0)4I11/2 (3) (665,3) 2G7/2 (0)4I11/2 (4) (667,9) 2H11/2 Table 1.

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