3 research outputs found
Ultrathin Polypyrrole Nanosheets via Space-Confined Synthesis for Efficient Photothermal Therapy in the Second Near-Infrared Window
Extensive
efforts have been devoted to synthesizing photothermal
agents (PTAs) that are active in the first near-infrared (NIR) region
(650–950 nm). However, PTAs for photothermal therapy in the
second NIR window (1000–1350 nm) are still rare. Here, it is
shown that two-dimensional ultrathin polypyrrole (PPy) nanosheets
prepared via a novel space-confined synthesis method could exhibit
unique broadband absorption with a large extinction coefficient of
27.8 L g<sup>–1</sup> cm<sup>–1</sup> at 1064 nm and
can be used as an efficient PTA in the second NIR window. This unique
optical property is attributed to the formation of bipolaron bands
in highly doped PPy nanosheets. The measured prominent photothermal
conversion efficiency could achieve 64.6%, surpassing previous PTAs
that are active in the second NIR window. Both in vitro and in vivo
studies reveal that these ultrathin PPy nanosheets possess good biocompatibility
and notable tumor ablation ability in the second NIR window. Our study
highlights the potential of ultrathin two-dimensional polymers with
unique optical properties in biomedical applications
Nonimaging Optical Gain in Luminescent Concentration through Photonic Control of Emission Étendue
Luminescent and nonimaging optical
concentration constitute two
fundamentally different ways of collecting and intensifying light.
Whereas nonimaging concentrators based on reflective, refractive,
or diffractive optics operate most effectively for collimated light,
luminescent concentrators (LCs) rely on absorption, re-emission, and
waveguiding to concentrate diffuse light incident from any direction.
LCs have been explored in many different shapes and sizes but have
so far been unable to exploit the power of nonimaging optics to further
increase their concentration ratio because their emission is angularly
isotropic. Here, we use a luminescent thin film bilayer to create
sharply directed conical emission in an LC and derive a nonimaging
optical solution to leverage this directionality for secondary geometric
gain ranging up to an order of magnitude or higher. We demonstrate
this concept experimentally using a custom compound parabolic optical
element index-matched to the LC surface and show that it delivers
three times more luminescent power to an opposing GaAs photovoltaic
cell when the emission profile is conically directed than when it
is isotropic or the nonimaging optic is absent. These results open
up a significant and general opportunity to improve LC performance
for a variety of applications including photovoltaics, photobioreactors,
and scintillator-based radiation detection
Transfer-Printing of Tunable Porous Silicon Microcavities with Embedded Emitters
Here
we demonstrate, via a modified transfer-printing technique,
that electrochemically fabricated porous silicon (PSi) distributed
Bragg reflectors (DBRs) can serve as the basis of high-quality hybrid
microcavities compatible with most forms of photoemitters. Vertical
microcavities consisting of an emitter layer sandwiched between 11-
and 15-period PSi DBRs were constructed. The emitter layer included
a polymer doped with PbS quantum dots, as well as a heterogeneous
GaAs thin film. In this structure, the PbS emission was significantly
redistributed to a 2.1 nm full-width at half-maximum around 1198 nm,
while the PSi/GaAs hybrid microcavity emitted at 902 nm with a sub-nanometer
full-width at half-maximum and quality-factor of 1058. Modification
of PSi DBRs to include a PSi cavity coupling layer enabled tuning
of the total cavity optical thickness. Infiltration of the PSi with
Al<sub>2</sub>O<sub>3</sub> by atomic layer deposition globally red-shifted
the emission peak of PbS quantum dots up to ∼18 nm (∼0.9
nm per cycle), while introducing a cavity coupling layer with a gradient
optical thickness spatially modulated the cavity resonance of the
PSi/GaAs hybrid such that there was an ∼30 nm spectral variation
in the emission of separate GaAs modules printed ∼3 mm apart