Fig. 4 Temporal-mode selective pulse retrieval using ac Stark pulses.

Slides:



Advertisements
Similar presentations
Force limits and layout design.
Advertisements

Three different types of transfer functions with a codomain of [0,1].
Examples of AEGIS autonomous target selection.
Velocity of hygrobots. Velocity of hygrobots. (A) The difference between l and lp corresponds to a distance that a hygrobot advances a period. (B) Velocity.
Visual explanation of the interaction terms.
Visual explanation of the interaction terms.
Fig. 2 Nonlinearities in a cavity-embedded perovskite single crystal.
Fig. 7 Correlation of NHP and human ISGs.
Fig. 1 Biomass over time of C3 grasses and C4 grasses at ambient and elevated CO2. Biomass over time of C3 grasses and C4 grasses at ambient and elevated.
Fig. 6 Avoiding unphysical points in the LZ model.
Fig. 5 Metafluorophores with different photostability.
Fig. 2 2D-IR spectroscopy on liquid ZnPa under dry conditions.
Fig. 4 Ballistic simulation of BP FETs.
Force limits and layout design.
Efficient optical pumping and quantum storage in a Nd:YVO nanocavity
Fig. 1 Schematics of the experiment.
Fig. 1 NP-free Ch-CNC droplets.
Fig. 3 Electron PSD in various regions.
Fig. 4 Morphogenesis in the Ch-CNC host droplets and NP assemblies.
Fig. 4 Resynthesized complex boronic acid derivatives based on different scaffolds on a millimole scale and corresponding yields. Resynthesized complex.
Fig. 2 Ferroelectric domains resolved in WTe2 single crystals.
Fig. 3 TESC spectra with increasing coupling strength and plexciton energy diagram with QD detuning. TESC spectra with increasing coupling strength and.
Fig. 2 Full-frame images recording the violation of a Bell inequality in four images. Full-frame images recording the violation of a Bell inequality in.
Fig. 3 Phase-contrast imaging.
Fig. 2 Time series of ice loss from the Amundsen Sea sector for the cases of unperturbed destabilization (black) and mass deposition (colored). Time series.
Fig. 1 Bioinspired design of AAD for promoting wound contraction.
Fig. 6 External drivers and model response.
Fig. 1 Parameterization and temporal distribution of carbon isotopic events in the database. Parameterization and temporal distribution of carbon isotopic.
Fig. 3 Photon number statistics resulting from Fock state |l, S − l〉 interference. Photon number statistics resulting from Fock state |l, S − l〉 interference.
Fig. 2 2D QWs of different propagation lengths.
Fig. 2 Configuration and composition of urban green space.
Fig. 3 Measurement of SOT efficiency (θDL,m) from ST-FMR.
Fast, noise-free memory for photon synchronization at room temperature
Fig. 2 EUV TG signal. EUV TG signal. Black lines in (A), (B), and (C) are the EUV TG signals from Si3N4 membranes at LTG = 110, 85, and 28 nm, respectively,
Examples of AEGIS autonomous target selection.
Fig. 3 ET dynamics on the control and treatment watersheds during the pretreatment and treatment periods. ET dynamics on the control and treatment watersheds.
Fig. 5 In-plane angle dependence of SOT efficiency (θDL,m) and resonance condition (Hres). In-plane angle dependence of SOT efficiency (θDL,m) and resonance.
Fig. 5 Schematic phase diagrams of Ising spin systems and Mott transition systems. Schematic phase diagrams of Ising spin systems and Mott transition systems.
Fig. 4 Effect of Cu spacer and current direction on SOT efficiency (θDL,m) in L10-IrMn. Effect of Cu spacer and current direction on SOT efficiency (θDL,m)
Fig. 5 Topology structure and strategy for the bottom-up synthesis of structurally uniform carboncones[1,m]. Topology structure and strategy for the bottom-up.
Fig. 4 The mechanical performances of thermally stable click-ionogels.
Fig. 4 Praying Prophet by Lorenzo Monaco: Mapping lake pigments and associated substrate. Praying Prophet by Lorenzo Monaco: Mapping lake pigments and.
Fig. 4 Evolution of fraction of sickled RBCs under hypoxia.
Fig. 4 Demonstration of dynamic scale invariance at long times.
Fig. 3 Characterization of the current-induced effective fields.
Fig. 2 Results of the learning and testing phases.
Fig. 2 Folding motions of the TCO with strain-softening behavior.
Fig. 2 Schematic drawings of Göbekli Tepe skulls.
Fig. 2 NH3, NOx, SO2, and NMVOC emission changes triggered by the JJJ clean air policy. NH3, NOx, SO2, and NMVOC emission changes triggered by the JJJ.
Fig. 2 Asymmetric MR of LMO within the ac plane.
Fig. 5 Predictions of the efficacy of sickling inhibitors with the kinetic model. Predictions of the efficacy of sickling inhibitors with the kinetic model.
Fig. 2 Images of the optical field at transmitter and receiver.
Fig. 1 Experiment description.
Fig. 3 Synaptic weighting and plasticity.
Fig. 1 Study design and antibody pharmacokinetics.
Fig. 4 CO2 emission changes triggered by the JJJ clean air policy.
Kinematic and mechanical advantage trade-off study.
Fig. 3 Comparisons of NDVI trends over the globally vegetated areas from 1982 to Comparisons of NDVI trends over the globally vegetated areas from.
Fig. 1 Schematic depiction of a paradigm for rapid and guided discovery of materials through iterative combination of ML with HiTp experimentation. Schematic.
Fig. 4 Spatial mapping of the distribution and intensity of industrial fishing catch. Spatial mapping of the distribution and intensity of industrial fishing.
Fig. 2 Finite element method (FEM) simulations of the photonic synapse with different structures. Finite element method (FEM) simulations of the photonic.
Fig. 2 Relaxation to a fitness maximum does not generate a logarithmic fitness trajectory. Relaxation to a fitness maximum does not generate a logarithmic.
Fig. 3 Characterization of the zero-point coupling rate and the mechanical dissipation rate. Characterization of the zero-point coupling rate and the mechanical.
Fig. 5 Density plots showing the relationship between growth responses to extreme events and site-level mean precipitation from all sites (N = 1314). Density.
The combined signal spectra of PSD for protons and helium nuclei
Fig. 3 Rubbery strain, pressure, and temperature sensors.
Fig. 1 Completely derived from natural wood, nanowood with hierarchically aligned cellulose nanofibrils can be used as an anisotropic super thermal insulator.
Comparison of children’s behavior between the three conditions.
Fig. 5 Modeling of the ASE threshold using the kinetic equations and experimental parameter inputs. Modeling of the ASE threshold using the kinetic equations.
Fig. 2 Time series of secularization versus GDP per capita, from four illustrative countries, over the 20th century. Time series of secularization versus.
Presentation transcript:

Fig. 4 Temporal-mode selective pulse retrieval using ac Stark pulses. Temporal-mode selective pulse retrieval using ac Stark pulses. (A) Schematic spectral configuration of two Stark pulses with respect to the AFC comb. The symmetric, far-detuned Stark pulses induce uniform compression of the AFC.(B) Stark pulses cause an additional delay in echo retrieval times. (C) Measured AFC echoes with increasing photon number in 16-ns Stark pulses. Here Δst = 1 GHz and Δ = 13.3 MHz. The blue shaded area overlays the echo envelope with no Stark pulses. (D) AFC echo delay against Stark pulse intensity. A linear fit (red dashed line) corresponds to 50 ps per photon. (E) Decrease of AFC echo efficiency with Stark pulse intensity, caused by AFC distortion resulting from inhomogeneous Stark shifts in the nanocavity. Tian Zhong et al. Science 2017;357:1392-1395 Copyright © 2017 The Authors, some rights reserved; exclusive licensee American Association for the Advancement of Science. No claim to original U.S. Government Works