Nonresonant optical driving of confined
semiconductors can open
up exciting opportunities for experimentally realizing strongly interacting
photon-dressed (Floquet) states through the optical Stark effect (OSE)
for coherent modulation of the exciton state. Here we report the first
room-temperature observation of the Floquet biexciton-mediated anomalous
coherent excitonic OSE in CsPbBr3 quantum dots (QDs). Remarkably,
the strong exciton–biexciton interaction leads to a coherent
red shift and splitting of the exciton resonance as a function of
the drive photon frequency, similar to Autler–Townes splitting
in atomic and molecular systems. The large biexciton binding energy
of ∼71 meV and exciton–biexciton transition dipole moment
of ∼25 D facilitate the hallmark observations, even at large
detuning energies of >300 meV. This is accompanied by an unusual
crossover
from linear to nonlinear fluence dependence of the OSE as a function
of the drive photon frequency. Our findings reveal crucial information
on the unexplored many-body coherent interacting regime, making perovskite
QDs suitable for room temperature quantum devices.
ReS2, a layered transition metal dichalcogenide (TMD)
with reduced crystal symmetry exhibiting unique anisotropic and layer-independent
properties, holds great potential for optoelectronic and photonic
applications. Despite a flurry of research activities in the third-order
nonlinear optical response of TMDs, tuning those properties in a completely
reversible manner in real time is a challenge and remains largely
unexplored. Here, we experimentally demonstrate band edge carrier-induced
sign reversal of the ultrafast third-order nonlinear optical response
in few-layer (4–8) ReS2 nanoflakes. In particular,
saturable absorption observed before hot carrier thermalization (<0.3
ps) is tuned to reverse saturable absorption (RSA) after the carrier
thermalized (>0.6 ps) at the band edge and defects using a single-color
pump–probe intensity scan (I-scan) technique. RSA in our experiment
is due to the two-step two single-photon absorption of the long-lived
(∼1000s of ps from our ultrafast transient absorption) carriers
at the band edges and defects. Motivated by the results, a liquid
cell-based high-performance few-layer ReS2 optical limiter
is fabricated with a remarkable 0.1 GW/cm
2
onset threshold and 0.64 limiting differential transmittance better
than the other optical-limiting materials. These results offer a direction
to manipulate the nonlinear optical response of materials which otherwise
requires a large electric field, high intensity, or efficient charge
transfer between donor and acceptor pairs.
Nanosecond near resonant excitation in As50S50 thin films leads to strong nonlinear optical response, i.e. nonlinear absorption coefficient up to 4 × 10 6 cm/GW and nonlinear refractive index of 8.5 cm 2 /GW, both of which is the strongest ever reported in amorphous semiconductors. We propose a five-level energy model to explain such effect which indicates that nonlinear process is reverse saturable absorption in nature, mediated by excited state absorption from triplet-triplet transition. On the other hand, observation of negative nonlinear refractive index reveals the occurrence of self-defocusing effect. Finally, benefitting from the strong nonlinear response, we demonstrate a promising application of As50S50 thin films as an optical limiter for optoelectronic sensors.
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