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Pb 2+ doped NaSr 4 (BO 3 ) 3 materials were prepared by a solution combustion synthesis method. The phase analysis of all synthesized materials was carried out using the powder XRD. The synthesized materials were investigated using spectrofluorometer at room temperature. The excitation and emission bands of NaSr 4 (BO 3 ) 3 : Pb 2+ were observed at 291 and 368 nm, respectively. The dependence of the emission intensity on the Pb 2+ concentration for the NaSr 4 (BO 3 ) 3 was studied in detail. It was observed that the concentration quenching of Pb 2+ in NaSr 4 (BO 3 ) 3 is 0.01 mol. The Stokes shifts of NaSr 4 (BO 3 ) 3 : Pb 2+ phosphor were calculated to be 7190 cm −1 . [ABSTRACT FROM AUTHOR]

Pure and Pb 2+ doped Ba 2 Be 2 B 2 O 7 materials were prepared by a solution combustion synthesis method. The phase analysis of all synthesized materials was carried out using the powder XRD. The synthesized phosphors were investigated using spectrofluorometer at room temperature. The excitation and emission bands of Ba 2 Be 2 B 2 O 7 :Pb 2+ were observed at 284 and 396 nm, respectively. The dependence of the emission intensity on the Pb 2+ concentration for the Ba 2 Be 2 B 2 O 7 was studied in detail. It was observed that the concentration quenching of Pb 2+ in Ba 2 Be 2 B 2 O 7 is 0.04 mol. The Stokes shifts of Ba 2 Be 2 B 2 O 7 :Pb 2+ phosphor were calculated to be 9959 cm −1 . [ABSTRACT FROM AUTHOR]

Abstract: Pure and Pb2+ doped LiSr4(BO3)3 materials were prepared by a solution combustion synthesis method. The phase analysis of all synthesized materials were determined using the powder XRD. The synthesized materials were investigated using spectrofluorometer at room temperature. The excitation and emission bands of LiSr4(BO3)3: Pb2+ were observed at 284 and 328nm, respectively. The dependence of the emission intensity on the Pb2+ concentration for the LiSr4(BO3)3 were studied in detail. It was observed that the concentration quenching of Pb2+ in LiSr4(BO3)3 is 0.005mol. The Stokes shifts of LiSr4(BO3)3: Pb2+ phosphor was calculated to be 4723cm–1. [Copyright &y& Elsevier]