Fig. 2 Rydberg-EIT spectra without control pulse.

Slides:



Advertisements
Similar presentations
Fig. 2 The temperature-dependent evolution of phase structures and surface states for the Ti-MWW– and SiO2-supported Mn2O3-Na2WO4 catalysts in O2 or CH4.
Advertisements

Fig. 5 In vivo MIP imaging of lipid and protein in C. elegans.
Fig. 1 Upward emission functions used to compute the maps.
Fig. 1 Characterization of decellularized zECM.
Fig. 3 Comparison between predicted change in DT since the LIG and observed sea-level highstands. Comparison between predicted change in DT since the LIG.
Fig. 1 Demographic shifts in knowledge producers.
Fig. 3 UV-induced vermilion degradation.
Fig. 3 Critical pressure analysis for reentrant and doubly reentrant geometries. Critical pressure analysis for reentrant and doubly reentrant geometries.
Structural analysis of graphene-embedded FeN4 (FeN4/GN) catalysts
Fig. 1 Examples of experimental stimuli and behavioral performance.
Fig. 6 Different models of assembly of Ch-CNC droplets laden with Fe3O4NPs under magnetic field. Different models of assembly of Ch-CNC droplets laden.
Fig. 2 Exposure effect screening study of CAV against Mtb.
Fig. 3 TESC spectra with increasing coupling strength and plexciton energy diagram with QD detuning. TESC spectra with increasing coupling strength and.
Order parameter θ as a function of time for the five events analyzed
Fig. 4 Response of a swarm model.
Fig. 2 Fluence-dependent emission characteristics of CH3NH3PbI3 recorded at 15 and 300 K. Fluence-dependent emission characteristics of CH3NH3PbI3 recorded.
Fig. 1 CFHT photometry converted into spectral reflectivity obtained on UT (Universal Time) 22 and 25 October 2014, is shown in comparison to the VLT reflectivity.
Fig. 2 Materials and designs for bioresorbable PC microcavity-based pressure and temperature sensors. Materials and designs for bioresorbable PC microcavity-based.
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 Gate voltage dependence of the areal iDMI and PMA.
Fig. 3 Controlled phase shift.
Fig. 2 Four types of MJO propagation patterns along the equator.
Spin diffusion buildup from bound water to amide protons in NaK2K
Fig. 2 Broadband IR s-SNOM of large crystallites.
Fig. 1 Impacts of intensified acidification on stream pH and calcium concentration. Impacts of intensified acidification on stream pH and calcium concentration.
Fast, noise-free memory for photon synchronization at room temperature
Fig. 3 Near-infrared spectrum of EM at 4.5 days after merger.
Fig. 2 Characterization of prepolarized NV NMR.
Fig. 2 Pulsed THz imaging. Pulsed THz imaging. (A) Electric field of our THz pulse recorded in the time domain using electro-optic sampling. The arrow.
HMRS integrated with a microfluidic system for multiple analyses
Fig. 3 Load dependence of friction force and corresponding COF.
Fig. 4 Experimental outputs.
Fig. 2 14C-CH4 data from each station and Keeling plot analysis.
Fig. 3 Collective modes of charge order in LBCO propagate diffusively.
Fig. 1 In vitro calibration plots and pH maps using iopamidol in human blood serum. In vitro calibration plots and pH maps using iopamidol in human blood.
Fig. 1 Time course of growth parameters for acetate-grown cultures of M. acetivorans with and without supplements. Time course of growth parameters for.
Fig. 3 Production of protein and Fe(II) at the end of growth correlated with increasing concentrations of ferrihydrite in the media that contained 0.2.
Fig. 3 Avoidable fraction of heat-related deaths if the current trajectory warming of 3°C is brought down to the 1.5° or 2°C Paris Agreement thresholds.
Fig. 4 Randomized benchmarking measurement.
Superconducting cavity electro-optics: A platform for coherent photon conversion between superconducting and photonic circuits by Linran Fan, Chang-Ling.
Fig. 1 Experiment description.
Fig. 1 Dcr-2 is required for Toll signaling in Drosophila S2 cells.
Fig. 3 Synaptic weighting and plasticity.
Fig. 7 Global change in the collective mass for wild mammals, humans, cattle, and all livestock for the years 1900–2050. Global change in the collective.
Fig. 3 Transition of adiabatic driving from the standard continuous protocol to the jumping protocol. Transition of adiabatic driving from the standard.
Fig. 1 Fractional coverage of the mapping method used in this study.
Fig. 2 XRD spectra and molecular structures of tetragonal and monoclinic crystal phase KDP samples. XRD spectra and molecular structures of tetragonal.
Optical π phase shift created with a single-photon pulse
Fig. 3 Experimental particle patterning actuated by continuous and sub-TOF regime pulsed SAW. Experimental particle patterning actuated by continuous and.
Fig. 2 Number of years that would have been required for the observed vertebrate species extinctions in the last 114 years to occur under a background.
Fig. 1 Light and CRIS of the relationship between magnetite and MMC in the meteorites studied. Light and CRIS of the relationship between magnetite and.
Fig. 6 Stabilization of hippocampal signaling over sleep.
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. 2 Inferring the diffusion equation from a single Brownian motion.
Fig. 3 Efficiency of the GDML predictor versus a model that has been trained on energies. Efficiency of the GDML predictor versus a model that has been.
Fig. 5 Frequency of appearances of immigrant vertebrate taxa or their oldest known descendants in opposing continents as observed in well-dated fossiliferous.
Fig. 2 Proton spectrum from 40 GeV to 100 TeV measured with DAMPE (red filled circles). Proton spectrum from 40 GeV to 100 TeV measured with DAMPE (red.
Fig. 5 Distributions of cell nuclear area values and internuclear distances in the breast tumor specimens (Figs. 3 and 4), where bin interval = 8 and n.
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. 2 Structural information.
The combined signal spectra of PSD for protons and helium nuclei
Fig. 3 Estimating nρ3 from LSPR absorption.
Fig. 4 Matrix for intersections of differentially expressed transcripts between RNAiAFL transgenic and null kernels. Matrix for intersections of differentially.
Fig. 3 The human FABP7 point mutation phenotype is recapitulated in Fabp7 KO mice, which also showed sleep fragmentation. The human FABP7 point mutation.
Fig. 4 Effects of individual picosecond and microsecond pulses.
Fig. 3 TDP1 promotes OXPHOS at basal and high ATP demands.
Fig. 1 TH17 cell differentiation was severely impaired in Cxxc1-deficient mice. TH17 cell differentiation was severely impaired in Cxxc1-deficient mice.
Fig. 4 Color modulation of fungal bioluminescence.
Fig. 1 TA mode in (22¯0) Brillouin zone.
Fig. 3 Spatial distribution of the shoot density (high densities are represented in dark green and low ones in bright yellow) in a simulation of a P. oceanica.
Presentation transcript:

Fig. 2 Rydberg-EIT spectra without control pulse. Rydberg-EIT spectra without control pulse. (A and B) The transmission and phase shift φ0 of the target signal beam are shown as a function of the signal detuning Δs. The line in (A) shows a fit based on Eq. (3). The line in (B) shows the expectation from Eq. (3) for the parameter values obtained in (A). For further experiments, we choose Δs/2π = −10 MHz (arrow), which is near the minimum of φ0. (C and D) For reference, similar spectra are shown in the absence of coupling light. All error bars in this article represent a statistical uncertainty of ±1 SD. Daniel Tiarks et al. Sci Adv 2016;2:e1600036 Copyright © 2016, The Authors