TY - JOUR
T1 - Energy transfer between managanese(II) and erbium(III) in various fluoride glasses
AU - Reisfeld, R.
AU - Greenberg, E.
AU - Jacoboni, C.
AU - De Pape, R.
AU - Jørgensen, C. K.
PY - 1984/7/1
Y1 - 1984/7/1
N2 - The fluorescence spectra and lifetimes of fluoride glasses of molar composition 36PbF2, 24MnF2 (or ZnF2), 35GaF3, 5 (or 7) Al(PO3)3, doped by ErF3 were investigated. The emission of Mn(II) in absence of Er(III) consists of a broad band centered around 630 nm and an integrated lifetime of 1.4 msec. In the presence of Er(III) the intensity and lifetimes are decreased as a result of energy transfer to the 4F 9 2 level of Er(III). The fluorescence of Er(III) arising from 4S 3 2 at 543 nm has an integrated lifetime of 0.06 ms in the absence of Mn(II) and is decreased to 0.01 ms in the presence of Mn(II) as a result of energy transfer to Mn(II). The 666-nm luminescence of Er(III) due to 4F 9 2 emission under excitation at 370 nm (4G 11 2) is about 20 times weaker than the 543-nm emission when Mn(II) is absent. However, in the presence of Mn(II) this emission becomes 5 times stronger than the 543-nm emission. This intensified emission has a non-exponential time dependence. The longer component corresponds to the transfer of stored energy in Mn(II) to Er(III) while the short-lived component is probably due to cascading down Er(III) → Mn(II) → Er(III) through states above the Stokes threshold of Mn(II). This interpretation is backed up by weaker 543-nm emission and stronger 630-nm broad-band emission when the mixed system is excited in one of the upper excited states, of Mn(II) at 395 nm, or of Er(III).
AB - The fluorescence spectra and lifetimes of fluoride glasses of molar composition 36PbF2, 24MnF2 (or ZnF2), 35GaF3, 5 (or 7) Al(PO3)3, doped by ErF3 were investigated. The emission of Mn(II) in absence of Er(III) consists of a broad band centered around 630 nm and an integrated lifetime of 1.4 msec. In the presence of Er(III) the intensity and lifetimes are decreased as a result of energy transfer to the 4F 9 2 level of Er(III). The fluorescence of Er(III) arising from 4S 3 2 at 543 nm has an integrated lifetime of 0.06 ms in the absence of Mn(II) and is decreased to 0.01 ms in the presence of Mn(II) as a result of energy transfer to Mn(II). The 666-nm luminescence of Er(III) due to 4F 9 2 emission under excitation at 370 nm (4G 11 2) is about 20 times weaker than the 543-nm emission when Mn(II) is absent. However, in the presence of Mn(II) this emission becomes 5 times stronger than the 543-nm emission. This intensified emission has a non-exponential time dependence. The longer component corresponds to the transfer of stored energy in Mn(II) to Er(III) while the short-lived component is probably due to cascading down Er(III) → Mn(II) → Er(III) through states above the Stokes threshold of Mn(II). This interpretation is backed up by weaker 543-nm emission and stronger 630-nm broad-band emission when the mixed system is excited in one of the upper excited states, of Mn(II) at 395 nm, or of Er(III).
UR - http://www.scopus.com/inward/record.url?scp=0021468615&partnerID=8YFLogxK
U2 - 10.1016/0022-4596(84)90097-5
DO - 10.1016/0022-4596(84)90097-5
M3 - ???researchoutput.researchoutputtypes.contributiontojournal.article???
AN - SCOPUS:0021468615
SN - 0022-4596
VL - 53
SP - 236
EP - 245
JO - Journal of Solid State Chemistry
JF - Journal of Solid State Chemistry
IS - 2
ER -