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CPM Seminar
Crafting Light at the Nanoscale: Disruptive Optical
and Optoelectronic Applications Harnessing the Power of Reverse Micelles
Ayse Turak
Departments of Physics Concordia University
Over the past two decades, nanometer-sized materials and devices have
attracted much interest from scientists and the general public, due to the
broad range of current and prospective applications of nanomaterials in
electronics, high-density data storage, chemical sensing, drug delivery,
medical diagnostic systems, and nanocatalysis. The explosive growth in
solution processed semiconductors has driven new emerging technologies for
photonic sources and adaptive optics: organic, hybrid, perovskite and all
inorganic-nanoparticle systems have developed significantly over the last
four decades due to the promise of cheap, flexible displays and lights
and the sources to power them. Though they have impacted the consumer
landscape, such devices have not dominated the market as has been long
predicted, as a roadblock in effective nanoparticle device development is
homogeneity, uniformity and effective size control, in the materials and at
various interfaces. Self-assembly of amphiphilic block copolymers is a model
example of a “bottom-up” approach to the construction of
nano-objects on large??areas. Di-block copolymers, due to their amphiphilic
nature, spontaneously form core-corona micelles in selective solvents. Using
the micelles as “nanoreactors” allows the formation
of highly controllable nanoparticles. The hydrophilic block typically has
high affinity to coordinate with metal reactants allowing control of the
nanoscale chemical reaction and nanoparticle growth. Reverse micelles are used
as carriers for the metal precursor and upon removal form highly organized
monodispersed nanoparticles. Particles are possible with a very narrow size
distribution, less than 2% variation in the particle diameters, which can
be deposited on any surface at room temperature with highly controlled
spacing and spatial organization. In the Turak Functional Nanomaterials
Group, we have used the same basic micellar diblock copolymer nanoreactor
to produce monodisperse oxide, dielectric, perovskite, core-shell, and metal
nanoparticles[1-10] for a variety of applications. This talk
will cover our work on polystyrene-block-poly-2-vinylpyridine (PS-b-P2VP)
reverse micelles as nearly universal nanoreactors systems for functional
nanoparticles. With a complete picture of the synthesis process coming out
of our research -- from an understanding of the basic loading behaviour, the
stability and the organizational structure of the micelles, to the properties
of the nanoparticles and their impact in devices -- it is possible to tailor
nanoparticle properties for widespread applications.
References
[1] S.I. Lee, M. Munir, R. Arbi, P. Oliveira, S.J. Lee, J.H.
Lim, W.Y. Kim, and A. Turak, J Mater Sci: Mater Electron 34, 1101
(2023).
[2] R. Arbi, M. Munir, D. Hoyle, S. Dogel, and A. Turak, Materials Today
Chemistry 34, 101732 (2023).
[3] Lewis, R. Arbi, A. Ibrahim, E. Smith, P. Olivera, F. Garza, and A. Turak,
J Mater Sci: Mater Electron 34, 750 (2023).
[4] F.J. Garza, R. Arbi, M. Munir, J.-H. Lim, and A. Turak, J. Phys. Chem. C
127, 4594 (2023).
[5] M. Munir, J. Tan, R. Arbi, P. Oliveira, E. Leeb, Y. Salinas, M.C.
Scharber, N.S. Sariciftci, and A. Turak, Adv. Photonics Res. 3(11),
2100372 (2022).
[6] A. Turak, Vid. Proc. Adv. Mater. 2, 2103166 (2021).
[7] T. Tokubuchi, R.I. Arbi, P. Zhenhua, K. Katayama, A. Turak, and W.Y. Sohn,
J. Photochem. Photobiol. A 410, 113179 (2021).
[8] S.I. Lee, K. Liang, L.S. Hui, R. Arbi, M. Munir, S.J. Lee, J.W. Kim, K.J.
Kim, W.Y. Kim, and A. Turak J Mater Sci: Mater Electron 32, 1161 (2021).
[9] R. Arbi, A. Ibrahim, L. Goldring-Vandergeest, K. Liang, G. Hanta, L.S.
Hui, and A. Turak, Nano Select 2, 2419 (2021).
[10] L.S. Hui, C. Beswick, A. Getachew, H. Heilbrunner, K. Liang, G. Hanta, R.
Arbi, M. Munir, H. Dawood, N. Isik Goktas, R.R. LaPierre, M.C. Scharber,
N.S. Sariciftci, and A. Turak, ACS Appl. Nano Mater. 2, 4121 (2019).
Thursday, October 19th 2023, 10:30
Ernest Rutherford Physics Building, Boardroom (room 104)
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