Two-photon patterned photostimulation with low-power, high-efficiency and reliable single-cell optogenetic control

Two-photon optogenetics enables selectively stimulating individual cells for manipulating neuronal ensembles. As the general photostimulation strategy, the patterned two-photon excitation has enabled millisecond-timescale activation for single or multiple neurons, but its activation efficiency is suffered from high laser power due to low beam-modulation efficiency. Here, we develop a high-efficiency beam-shaping method based on the Gerchberg-Saxton (GS) algorithm with spherical-distribution initial phase (GSSIP) to reduce the patterned two-photon excitation speckles and intensity. It can well control the phase of shaped beams to attain speckle-free accurate patterned illumination with an improvement of 44.21% in the modulation efficiency compared with that of the traditional GS algorithm. A combination of temporal focusing and the GSSIP algorithm (TF-GSSIP) achieves patterned focusing through 500-μm-thickness mouse brain slices, which is 2.5 times deeper than the penetration depth of TF-GS with the same signal-to-noise ratio (SNR). With our method, the laser power can be reduced to only 55.56% of that with traditional method (the temporal focusing with GS, TF-GS) to reliably evoke GCaMP6s response in C1V1-expressing cultured neurons with single-cell resolution. Besides, the photostimulation efficiency is remarkably increased by 80.19% at the same excitation density of 0.27 mW/μm2. This two-photon stimulation method with low-power, reliable and patterned illumination may pave the way for analyzing neural circuits and neural coding and decoding mechanism.

Drastic transitions of excited state and coupling regime in all-inorganic perovskite microcavities characterized by exciton/plasmon hybrid natures

Lead-halide perovskites are highly promising for various optoelectronic applications, including laser devices. However, fundamental photophysics explaining the coherent-light emission from this material system is so intricate and often the subject of debate. Here, we systematically investigate photoluminescence properties of all-inorganic perovskite microcavity at room temperature and discuss the excited state and the light–matter coupling regime depending on excitation density. Angle-resolved photoluminescence clearly exhibits that the microcavity system shows a transition from weak coupling regime to strong coupling regime, revealing the increase in correlated electron–hole pairs. With pumping fluence above the threshold, the photoluminescence signal shows a lasing behavior with bosonic condensation characteristics, accompanied by long-range phase coherence. The excitation density required for the lasing behavior, however, is found to exceed the Mott density, excluding the exciton as the excited state. These results demonstrate that the polaritonic Bardeen–Cooper–Schrieffer state originates the strong coupling formation and the lasing behavior.

Optical probes of free charge generation in organic photovoltaics

<p>Organic photovoltaics (OPVs) show considerable promise as a source of low cost solar energy. Improving our understanding of the processes governing free charge photogeneration in OPVs may unlock the improvements in efficiency required for their widespread implementation. In particular, how do photogenerated charge pairs overcome their mutual columbic attraction, and what governs the branching between bound and free charge pairs that is observed to occur shortly after their creation? Ultrafast laser techniques such as transient absorption (TA) spectroscopy are the only tools capable of probing the time scales associated with these processes (as short as 10⁻¹⁴ seconds). Challenges include achieving sufficient sensitivity to resolve the tiny signals generated in thin films under solar-equivalent excitation densities, and distinguishing and quantifying overlapping signals due to separate phenomena. We present the development of a versatile and ultra-sensitive broadband TA spectrometer, along with a comprehensive analysis of the noise sources limiting sensitivity. Through the use of referenced shot-to-shot detection and a novel method exploiting highly chirped broadband probe pulses, we are capable of resolving changes in differential transmission < 3 × 10⁻⁶ over pump-probe delays of 10⁻¹³–10⁻⁴ seconds. By comparing the absorption due to photogenerated charges to measurements of open-circuit voltage decay in devices under transient excitation, we show that TA is able to quantify the recombination of freely extractable charge pairs over many decades of pump-probe delay. The dependence of this recombination on excitation density can reveal the relative fraction of bound and free charge pairs. We apply this technique to blends of varying efficiency and find that the measured free charge fraction is correlated with published photocharge yields for these materials. We access a regime at low temperature where thermalized charge pairs are frozen out following the primary charge separation step and recombine monomolecularly via tunneling. The dependence of tunneling rate on distance enabled us to fit recombination dynamics to distributions of recombination rates. We identified populations of charge-transfer states and well-separated charge pairs, the yield of which is strongly correlated with the yield of free charges measured via their intensity dependent recombination. We conclude that populations of free charges are established via long-range charge separation within the thermalization timescale, thus invoking early branching between free and bound charges across an energetic barrier. Subject to assumed values of the electron tunneling attenuation constant, we find critical charge separation distances of ~ 3–4nm in all materials. TA spectroscopy probes the absorption of excited states, with the signal being proportional to the product of population density and absorption cross-section of the absorbing species. We show that the dependence of signal on probe pulse intensity can decouple these parameters, and apply a numerical model to determine the time-dependent absorption cross-section of photogenerated excitons in thin films of semiconducting polymers. Collectively, this thesis presents spectroscopic tools and applications thereof that illuminate the process of free charge generation in organic photovoltaics.</p>

Optical probes of free charge generation in organic photovoltaics

<p>Organic photovoltaics (OPVs) show considerable promise as a source of low cost solar energy. Improving our understanding of the processes governing free charge photogeneration in OPVs may unlock the improvements in efficiency required for their widespread implementation. In particular, how do photogenerated charge pairs overcome their mutual columbic attraction, and what governs the branching between bound and free charge pairs that is observed to occur shortly after their creation? Ultrafast laser techniques such as transient absorption (TA) spectroscopy are the only tools capable of probing the time scales associated with these processes (as short as 10⁻¹⁴ seconds). Challenges include achieving sufficient sensitivity to resolve the tiny signals generated in thin films under solar-equivalent excitation densities, and distinguishing and quantifying overlapping signals due to separate phenomena. We present the development of a versatile and ultra-sensitive broadband TA spectrometer, along with a comprehensive analysis of the noise sources limiting sensitivity. Through the use of referenced shot-to-shot detection and a novel method exploiting highly chirped broadband probe pulses, we are capable of resolving changes in differential transmission < 3 × 10⁻⁶ over pump-probe delays of 10⁻¹³–10⁻⁴ seconds. By comparing the absorption due to photogenerated charges to measurements of open-circuit voltage decay in devices under transient excitation, we show that TA is able to quantify the recombination of freely extractable charge pairs over many decades of pump-probe delay. The dependence of this recombination on excitation density can reveal the relative fraction of bound and free charge pairs. We apply this technique to blends of varying efficiency and find that the measured free charge fraction is correlated with published photocharge yields for these materials. We access a regime at low temperature where thermalized charge pairs are frozen out following the primary charge separation step and recombine monomolecularly via tunneling. The dependence of tunneling rate on distance enabled us to fit recombination dynamics to distributions of recombination rates. We identified populations of charge-transfer states and well-separated charge pairs, the yield of which is strongly correlated with the yield of free charges measured via their intensity dependent recombination. We conclude that populations of free charges are established via long-range charge separation within the thermalization timescale, thus invoking early branching between free and bound charges across an energetic barrier. Subject to assumed values of the electron tunneling attenuation constant, we find critical charge separation distances of ~ 3–4nm in all materials. TA spectroscopy probes the absorption of excited states, with the signal being proportional to the product of population density and absorption cross-section of the absorbing species. We show that the dependence of signal on probe pulse intensity can decouple these parameters, and apply a numerical model to determine the time-dependent absorption cross-section of photogenerated excitons in thin films of semiconducting polymers. Collectively, this thesis presents spectroscopic tools and applications thereof that illuminate the process of free charge generation in organic photovoltaics.</p>

Decoherent quench dynamics across quantum phase transitions

We present a formulation for investigating quench dynamics across quantum phase transitions in the presence of decoherence. We formulate decoherent dynamics induced by continuous quantum non-demolition measurements of the instantaneous Hamiltonian. We generalize the well-studied universal Kibble-Zurek behavior for linear temporal drive across the critical point. We identify a strong decoherence regime wherein the decoherence time is shorter than the standard correlation time, which varies as the inverse gap above the groundstate. In this regime, we find that the freeze-out time \bar{t}\sim\tau^{{2\nu z}/({1+2\nu z})}t-∼τ2νz/(1+2νz) for when the system falls out of equilibrium and the associated freeze-out length \bar{\xi}\sim\tau^{\nu/({1+2\nu z})}ξ‾∼τν/(1+2νz) show power-law scaling with respect to the quench rate 1/\tau1/τ, where the exponents depend on the correlation length exponent \nuν and the dynamical exponent zz associated with the transition. The universal exponents differ from those of standard Kibble-Zurek scaling. We explicitly demonstrate this scaling behavior in the instance of a topological transition in a Chern insulator system. We show that the freeze-out time scale can be probed from the relaxation of the Hall conductivity. Furthermore, on introducing disorder to break translational invariance, we demonstrate how quenching results in regions of imbalanced excitation density characterized by an emergent length scale which also shows universal scaling. We perform numerical simulations to confirm our analytical predictions and corroborate the scaling arguments that we postulate as universal to a host of systems.

Nonlinear Photocarrier Dynamics and the Role of Shallow Traps in Mixed-Halide Mixed-Cation Hybrid Perovskites

<p>We examine the role of surface passivation on carrier trapping and nonlinear recombination dynamics in hybrid metal-halide perovskites by means of excitation correlation photoluminescence (ECPL) spectroscopy. We find that carrier trapping occurs on subnanosecond timescales in both control (unpassivated) and passivated samples, which is consistent within a shallow-trap model. However, the impact of passivation has a direct effect on both shallow and deep traps. Our results reveal that the effect of passivation of deep traps is responsible for the increase of the carrier lifetimes, while the passivation of shallow traps reduces the excitation density required for shallow-trap saturation. Our work demonstrates how ECPL provides details about the passivation of shallow traps beyond those available via conventional time-resolved photoluminescence techniques.</p>