Page 8 - PR 2014 2016 02 Lasers Technology
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22   Lasers Technology | Progress Report





               Crystal growth activities


               Recently, rare earth doped nanocrystals re-    with spectral and temporal discrimination
               ceived great attention due to their application   that uses a Box-car technique and tuneable
               in high-resolution panels, integrated optical   laser excitations of 4 ns (10 Hz) in the range of
               systems and biological labeling. The controlled   420 to 2000 nm (10mJ) was used for lifetime
               synthesis of nanoparticles with uniform size,   measurements of rare earth ions in glasses
               shape, structure and rare earth doping be-     and fluorides crystals. These measurements
               came of fundamental importance once the        allowed determining the rate constant of the
               final properties are directly related to these   non-radiative energy transfer that happens
               parameters.                                    due to multipolar interactions between donor
                                                              and acceptor ions in solids. Energy transfer
               The NaYF  is a very efficient host matrix for   mechanism involving two interacting erbium
                         4
               trivalent rare earth ions such as Yb/Er and    (and holmium) ions in the first (and second)
               Yb/Tm for up-conversion systems. There are     excited state, energy-transfer up-conversion
               several synthetic processes already reported   have (has) been observed and the rate constant
               in the literature for production of this mate-  determined. The aim of this study is the devel-
               rial, involving different chemical routes and   opment of solid laser medium emitting in the
               processing from organic and inorganic com-     mid-infrared (2700 - 3600 nm) and to improve
               pounds, however, the reproducibility of these   the small signal gain laser emission of Er  and
                                                                                                    3+
                                                                 3+
               processes are not always achieved. We are      Ho -doped materials. A detailed investigation
               studying the production of NaYF  co-doped      of the energy transfer processes involving one
                                                4
                                                                                3+
                                                                                             3+
                       3+
               with Yb /Er  by micro-flow reaction using a    or two excited Ho  ions in Ho -doped InF
                           3+
                                                                                                         3
               microchannel system. A microfluidic circuit    glass has been performed to examine all the
               was designed and fabricated at the Center      energy transfer rates relevant to the  I  →  I
                                                                                                        5
                                                                                                   5
                                                                                                    5    6
               for Lasers and Applications at IPEN.  It is a   transition at 3930 nm as a function of the Ho
                                                                                                         3+
               two-stage microfluidic reactor - in the first   concentration (2, 4 and 10 mol %).  The decay
               stage, the product stream (NaF solution) is    times, branching ratios and rate parameters for
               combined with the second precursor stream      the energy transfer, were measured and they
               (RECl  solution, were RE = rare earth). In the   were used as the input parameters for a rate
                    3
               second stage, the compounds flow through a     equations analysis. Excited state absorption
               heated zone (temperature range of 70 - 100°C).    (ESA) initiating from the lower laser level of
                                                                 3+
               The main compounds are guided through the      Ho  was determined in this study. Numerical
               system with two syringes, with flow controlled   simulation of CW laser emission at 3930 nm
               by the applied pressure (electronic controlled).   was performed using two pump wavelength,
               Experiments are under way to analyze injec-    one for the upper laser level excitation (i.e.
               tion flow rates of the components, aiming to   5 I  →  I   = λ ) and the other for lower laser level
                                                                  5
                                                                8   5   P1
                                                                                      5
               define the residence rate and temperature for   de-excitation (i.e.  I6 →  S  = λ ). The pump
                                                                                5
                                                                                        2   P2
               desired nanoparticles production.              wavelength λ  = 889 nm was chosen to match
                                                                           P1
                                                              the fundamental absorption of the  I  →  I  Ho
                                                                                                   5
                                                                                                         3+
                                                                                               5
                                                                                                 8   5
               The next step before laser development is      transition and the pump wavelength λ  = 962
                                                                                                   P2
               the characterization, modeling and optical     nm was determined based on the measure-
               spectroscopy of rare-earth doped solid laser   ments of ESA and the application of the Mc-
               media. A luminescence spectroscopic system     Cumber method. Critically, the estimated ESA
                         Instituto de Pesquisas Energéticas e Nucleares
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