Photoexcitation of Yb-doped aluminosilicate fibers at 250 nm: evidence for excitation transfer from oxygen deficiency centers to Yb 3+

Emission spectra in the ~240–1100 nm wavelength region as well as the temporally resolved decay of Yb3+ and point defect spontaneous emission have been recorded when aluminosilicate optical fibers doped with Yb are irradiated with ~160 fs laser pulses having a central wavelength of ~250 nm(ℏω=5 eV). Photoexcitation of the fibers in this region of the deep ultraviolet (UV) provides access simultaneously to the Type II Si oxygen deficiency center (ODC), the non-bridging oxygen hole center (NBOHC: an oxygen-excess defect), and the Ge ODC. Emission from all of these defects in the ultraviolet and/or visible is observed, as is intense fluorescence at 976 nm from Yb3+. Absorption measurements conducted in the ~230–265 nm region with a sequence of UV light-emitting diodes reveal a continuum peaking at ~248 nm and having a spectral width of ~18 nm (FWHM), confirming that the 250 nm laser pump is photoexciting predominantly the ODC. The temporal histories of the optically active defect and rare earth ion emission waveforms, in combination with time-integrated spectra, suggest that the Si ODC(II) triplet state directly excites Yb3+ as well as at least one other intrinsic defect in the silica network. Prolonged exposure of the Yb-doped fibers to 250 nm radiation yields increased Yb3+, NBOHC, and Si ODC(II) singlet emission which is accompanied by a decline in Si ODC(II) triplet fluorescence, thus reinforcing the conclusion—drawn on the basis of luminescence decay constants—that the triplet state of Si ODC(II) is the immediate precursor to the NBOHC and is partially responsible for Yb ion emission at 976 nm. This conclusion is consistent with the observation that exposure of fiber to 5 eV radiation slightly suppresses ODC absorption in the ~240–255 nm region while simultaneously introducing an absorption continuum extending from 260 nm to below 235 nm (ℏω≈5.28 eV). These results suggest that ODC→E′ center conversion assumes a role in excitation transfer to Yb3+.

[1]  André Croteau,et al.  Characterization of defect luminescence in Yb doped silica fibers: part I NBOHC. , 2008, Optics express.

[2]  Nakamura,et al.  Enhanced photogeneration of E' centers from neutral oxygen vacancies in the presence of hydrogen in high-purity silica glass. , 1993, Physical review. B, Condensed matter.

[3]  H. Imai,et al.  Generation of E' centers and oxygen hole centers in synthetic silica glasses by γ irradiation , 1993 .

[4]  George H. Sigel,et al.  Processing-induced defects in optical waveguide materials , 1998, Bragg Gratings, Photosensitivity, and Poling in Glass Fibers and Waveguides: Applications and Fundamentals.

[5]  J K Sahu,et al.  Photodarkening in Yb-doped aluminosilicate fibers induced by 488 nm irradiation. , 2008, Optics letters.

[6]  Y. Ouerdane,et al.  COOPERATIVE LUMINESCENCE IN AN YTTERBIUM-DOPED SILICA FIBRE , 1994 .

[7]  Kawamura,et al.  Photochemical reactions in GeO2-SiO2 glasses induced by ultraviolet irradiation: Comparison between Hg lamp and excimer laser. , 1995, Physical review. B, Condensed matter.

[8]  M. Söderlund,et al.  Measuring photodarkening from single-mode ytterbium doped silica fibers. , 2006, Optics express.

[9]  C. Burrus,et al.  Neodymium‐doped silica lasers in end‐pumped fiber geometry , 1973 .

[10]  A. Trukhin,et al.  Luminescence of silica glass containing aluminum oxide , 2004 .

[11]  S. Unger,et al.  Photodarkening in Yb doped fibers: experimental evidence of equilibrium states depending on the pump power. , 2007, Optics express.

[12]  A. Amossov,et al.  Oxygen-deficient centers in silica glasses: a review of their properties and structure , 1994 .

[13]  B. Poumellec,et al.  Computed paramagnetic properties for an E′ center produced from the twofold coordinated Si or Ge in silica , 2007 .

[14]  G. M. Zhidomirov,et al.  Two fold coordinated silicon atom: a hole trap in SiO2 , 2002 .

[15]  L. Norin,et al.  Comment on "Photodarkening in Yb-doped aluminosilicate fibers induced by 488 nm irradiation". , 2008, Optics letters.

[16]  L. Norin,et al.  Preventing photodarkening in ytterbium-doped high power fiber lasers; correlation to the UV-transparency of the core glass. , 2008, Optics express.

[17]  A. J. Cohen NEUTRON SPECIFIC COLOR CENTER IN FUSED SILICA AND AN IMPURITY BAND OF IDENTICAL WAVELENGTH , 1957 .

[18]  D. Payne,et al.  Photodarkening in Yb-doped aluminosilicate fibers induced by 488 nm irradiation , 2007 .

[19]  Takashi Handa,et al.  Aluminum or phosphorus co‐doping effects on the fluorescence and structural properties of neodymium‐doped silica glass , 1986 .

[20]  V. B. Neustruev,et al.  Colour centres in germanosilicate glass and optical fibres , 1994 .

[21]  F. Meinardi,et al.  Native and radiation-induced photoluminescent defects in SiO 2 : Role of impurities , 1998 .

[22]  F. Salin,et al.  Photodarkening and Photobleaching of an Ytterbium-doped Silica Double-clad LMA fiber , 2007, 2007 Conference on Lasers and Electro-Optics (CLEO).

[23]  Arai,et al.  Evidence for pair generation of an E' center and a nonbridging oxygen-hole center in gamma -ray-irradiated fluorine-doped low-OH synthetic silica glasses. , 1992, Physical review. B, Condensed matter.

[24]  L. Skuja Optically active oxygen-deficiency-related centers in amorphous silicon dioxide , 1998 .

[25]  D. Åberg,et al.  Strong UV absorption and visible luminescence in ytterbium-doped aluminosilicate glass under UV excitation. , 2007, Optics letters.

[26]  Y. Barmenkov,et al.  Cooperative luminescence and absorption in Ytterbium-doped silica fiber and the fiber nonlinear transmission coefficient at lambda = 980 nm with a regard to the Ytterbium ion-pairs' effect: Reply. , 2006, Optics express.