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