3 research outputs found
Directional Negative Thermal Expansion and Large Poisson Ratio in CH<sub>3</sub>NH<sub>3</sub>PbI<sub>3</sub> Perovskite Revealed by Strong Coherent Shear Phonon Generation
Despite
the enormous amount of attention CH<sub>3</sub>NH<sub>3</sub>PbI<sub>3</sub> has received, we are still lacking an in-depth understanding
of its basic properties. In particular, the directional mechanical
and structural characteristics of this material have remained elusive.
Here, we investigate these properties by monitoring the propagation
of longitudinal and shear phonons following the absorption of a femtosecond
pulse along various crystalline directions of a CH<sub>3</sub>NH<sub>3</sub>PbI<sub>3</sub> single crystal. We first extract the sound
velocities of longitudinal and transverse phonons along these directions
of the crystal. Our study then reveals the negative directional thermal
expansion of CH<sub>3</sub>NH<sub>3</sub>PbI<sub>3</sub>, which is
responsible for strong coherent shear phonon generation. Finally,
from these observations, we perform elastic characterization of this
material, revealing a large directional Poisson’s ratio, which
reaches 0.7 and that we associate with the weak mechanical stability
of this material. Our results also provide guidelines to fabricate
a transducer of high-frequency transverse phonons
Carrier Recombination Processes in Gallium Indium Phosphide Nanowires
Understanding
of recombination and photoconductivity dynamics of photogenerated
charge carriers in Ga<sub><i>x</i></sub>In<sub>1–x</sub>P NWs is essential for their optoelectronic applications. In this
letter, we have studied a series of Ga<sub><i>x</i></sub>In<sub>1–x</sub>P NWs with varied Ga composition. Time-resolved
photoinduced luminescence, femtosecond transient absorption, and time-resolved
THz transmission measurements were performed to assess radiative and
nonradiative recombination and photoconductivity dynamics of photogenerated
charges in the NWs. We conclude that radiative recombination dynamics
is limited by hole trapping, whereas electrons are highly mobile until
they recombine nonradiatively. We also resolve gradual decrease of
mobility of photogenerated electrons assigned to electron trapping
and detrapping in a distribution of trap states. We identify that
the nonradiative recombination of charges is much slower than the
decay of the photoluminescence signal. Further, we conclude that trapping
of both electrons and holes as well as nonradiative recombination
become faster with increasing Ga composition in Ga<sub><i>x</i></sub>In<sub>1–x</sub>P NWs. We have estimated early time
electron mobility in Ga<sub><i>x</i></sub>In<sub>1–x</sub>P NWs and found it to be strongly dependent on Ga composition due
to the contribution of electrons in the X-valley
Graphene-to-Substrate Energy Transfer through Out-of-Plane Longitudinal Acoustic Phonons
Practically, graphene is often deposited
on substrates. Given the
major substrate-induced modification of properties and considerable
energy transfer at the interface, the graphene–substrate interaction
has been widely discussed. However, the proposed mechanisms were restricted
to the two-dimensional (2D) plane and interface, while the energy
conduction in the third dimension is hardly considered. Herein, we
disclose the transfer of energy perpendicular to the interface of
the combined system of the 2D graphene and the 3D base. More precisely,
our observation of the energy dissipation of optically excited graphene
via emitting out-of-plane longitudinal acoustic phonon into the substrate
is presented. By applying nanoultrasonic spectroscopy with a piezoelectric
nanolayer embedded in the substrate, we found that under photoexcitation
by a femtosecond laser pulse graphene can emit longitudinal coherent
acoustic phonons (CAPs) with frequencies over 1 THz into the substrate.
In addition, the waveform of the CAP pulse infers that the photocarriers
and sudden lattice heating in graphene caused modification of graphene–substrate
bond and consequently generated longitudinal acoustic phonons in the
substrate. The direct observation of this unexplored graphene-to-substrate
vertical energy transfer channel can bring new insights into the understanding
of the energy dissipation and limited transport properties of supported
graphene