Fig. 1 Simplified sketch of the experimental design.

Slides:

Advertisements

Similar presentations

Demonstration of Two-Plasmon Quantum Interference Hyunseok Lee 1.

Advertisements

Quantum Teleportation

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.

Fig. 3 Band dispersions along on the KHgSb (010) surface.

Fig. 2 Nonlinearities in a cavity-embedded perovskite single crystal.

Fig. 4 Estimations of nonlinear functionals of a single-qubit state with the quantum Fredkin gate. Estimations of nonlinear functionals of a single-qubit.

Fig. 2 The arrangements of metal core and ligands.

Fig. 1 Demographic shifts in knowledge producers.

Origin of the asymmetry and determination of the critical angle

Fig. 3 Electron PSD in various regions.

Fig. 3 Faculty placement distributions.

Fig. 3 ACID isosurfaces of the model complex 2′ separated into the π- and σ-contribution. ACID isosurfaces of the model complex 2′ separated into the π-

Fig. 5 Analytical performance of the wearable cortisol sensor.

Fig. 2 Fluence-dependent emission characteristics of CH3NH3PbI3 recorded at 15 and 300 K. Fluence-dependent emission characteristics of CH3NH3PbI3 recorded.

Motion Detection: Neuronal Circuit Meets Theory

Fig. 2 Principle of attenuation-compensation for a Bessel light sheet.

Fig. 4 Comparison of East African paleotemperature data with CMIP5/PMIP3 model output. Comparison of East African paleotemperature data with CMIP5/PMIP3.

Full-frame single image recording the violation of a Bell inequality

Fig. 2 Device characteristics.

Fig. 1 Imaging setup to perform a Bell inequality test in images.

Fig. 4 Full-frame single image recording the violation of a Bell inequality and implementing the scanning of the phase circle. Full-frame single image.

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. 4 (Top) Upper curves show the total number of words in initial messages, which increases with desirability gap. Lower curves show the fraction of.

Fig. 1 Concept of the livestock transition in China between 1980 and Concept of the livestock transition in China between 1980 and The left-

Characteristics of the topology-optimized actuator and long-term tests

Fig. 1 Fluctuation-induced dynamic response patterns.

Imaging Bell-type nonlocal behavior

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. 1 Schematic of WPS microscope.

Fig. 1 Experimental setup.

Dynamically self-assembled patterns formed by up to 40 micro-rafts

Fig. 1 Energy levels and laser couplings of the inelastic optical WM-enhanced NMOR effect. Energy levels and laser couplings of the inelastic optical WM-enhanced.

Fig. 3 Transport characterization of dry-assembled devices.

Fig. 4 Experimental outputs.

Fig. 4 Structural design of an F-TENG.

Fig. 1 Experimental setup.

Fig. 2 Characterizing the performance of msTENG.

Fig. 2 Optimization of the sweat control and characterization of individual sensors. Optimization of the sweat control and characterization of individual.

Fig. 2 Images of the optical field at transmitter and receiver.

Integrated photonic platform for quantum information with continuous variables by Francesco Lenzini, Jiri Janousek, Oliver Thearle, Matteo Villa, Ben Haylock,

Fig. 5 Changes in PSD-95 synaptic puncta in the mPFC 6 weeks after exposure to 5 or 30 cGy of 16O or 48Ti charged particles. Changes in PSD-95 synaptic.

Fig. 2 Electrical properties of CNT array FETs and influence of postdeposition treatment on conductance. Electrical properties of CNT array FETs and influence.

Fig. 3 Double-resonance solid-state NMR data of ceria nanoparticles.

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. 1 Fractional coverage of the mapping method used in this study.

Fig. 2 The influence of TPP on the flammability of the electrolyte and the electrochemical performance of the graphite anode. The influence of TPP on the.

Fig. 2 Optomechanical scheme to measure photon angular momentum and optical torque in a waveguide. Optomechanical scheme to measure photon angular momentum.

Fig. 3 Information storage substates.

Fig. 3 The material choices and durability of the STENG.

Optical π phase shift created with a single-photon pulse

Fig. 2 The experimental setup.

Fig. 4 The relationship between the total mean absolute momentum disturbance 〈∣p∣〉zB (in units of ℏ/D) and fringe visibility V. The relationship between.

Fig. 1 Charge manipulation and readout in diamond.

Thermomechanical characterization of the elasticity and plasticity

Fig. 5 Comparison between the results generated with the proposed new algorithm and the preceding state-of-the-art results for a detail of the Adam panel.

Fig. 2 Finite element method (FEM) simulations of the photonic synapse with different structures. Finite element method (FEM) simulations of the photonic.

Fig. 3 Results of the proposed algorithm applied to a detail from the Adam panel. Results of the proposed algorithm applied to a detail from the Adam panel.

Fig. 2 Experimental setup.

Fig. 3 Wavelength and polarization tunable mirrorless lasing from the heliconical superstructure. Wavelength and polarization tunable mirrorless lasing.

Fig. 3 Interference of quantum clocks.

Fig. 1 Prestige hierarchies in faculty hiring networks.

Fig. 3 Voltage-driven phase switching in a 1T-TaS2 nano-thick crystal.

Fig. 2 The working principle and electrical output modulating of BD-TENG by changing the materials of friction layers. The working principle and electrical.

Fig. 3 Optimization of the antidot GNR structure.

Fig. 2 Experimental schematic of photon production from a 138Ba+ ion, QFC, and photonic slowing in a warm neutral 87Rb vapor. Experimental schematic of.

Fig. 5 Enhancers and super-enhancers identified in various brain cell populations. Enhancers and super-enhancers identified in various brain cell populations.

Fig. 1 Photonic implementation of a fractional QKT.

Snapshots of long-range perturbations in aqueous NaCl solutions

Fig. 2 Printed three-axis acceleration sensor.

Presentation transcript:

Fig. 1 Simplified sketch of the experimental design. Simplified sketch of the experimental design. The input quantum state |ψ〉 is imprinted on a single photon using an SLM-A. The single photon is subsequently sent to the cloning machine for optimal cloning. The cloning machine consists of a delay line (DL), to adjust the arrival time of the input photon, a second photon that is in a completely mixed state when exiting SLM-B, and a first beam splitter (BS1). The two photons are made to arrive at the beam splitter simultaneously using the DL. The two photons exiting one of the output ports of the first beam splitter together are separated at a second beam splitter (BS2) and are sent out of the cloning machine. The cloned photons are then detected and characterized using detectors (D1 and D2) and SLMs (SLM-C and SLM-D), respectively. (A to C) Examples of Hong-Ou-Mandel (HOM) coalescence curves for input photons of respectively (top to bottom). The curve is obtained by recording the coincidences between the output ports of BS2 for various delays of one of the input photons. Examples of enhancement peaks of , , and are obtained experimentally, and agree with the theoretical value of Rth = 2, corresponding to a visibility of . Frédéric Bouchard et al. Sci Adv 2017;3:e1601915 Copyright © 2017, The Authors