by Alan She, Shuyan Zhang, Samuel Shian, David R

Slides:



Advertisements
Similar presentations
Forward-looking Metalens
Advertisements

Fig. 5 MicroLED array with 3D liquid metal interconnects.
Fig. 3 The electrical contact of direct-printed and reconfigured liquid metals. The electrical contact of direct-printed and reconfigured liquid metals.
Fig. 2 CFD results. CFD results. Results of CFD simulations in horizontal (left column) and vertical (right column) cross-sections. All models oriented.
Fig. 1 Evolution of magnetic field lines around a foreshock bubble in the GSE-XY plane (z = 0): Results of a hybrid simulation. Evolution of magnetic field.
Fig. 1 Crystal and electronic structure of WTe2.
Fig. 2 Fluidic and electrical characteristics of the wireless optofluidic system. Fluidic and electrical characteristics of the wireless optofluidic system.
Fig. 3 Saturation velocity of BP FETs.
Fig. 1 NP-free Ch-CNC droplets.
Fig. 3 Electron PSD in various regions.
Tuning of the conductance plateau of device 1 and quantum dot model
Fig. 6 Comparison of properties of water models.
Fig. 2 Reference-fixing experiment, results.
Fig. 2 Ferroelectric domains resolved in WTe2 single crystals.
Fig. 2 Principle of attenuation-compensation for a Bessel light sheet.
Interactive morphogenesis in Ch-CNC droplets laden with magnetic NPs
Fig. 3 Rotation experiment, setup.
Fig. 1 Study area and field site setting.
Fig. 1 Phase diagram and FS topologies.
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. 1 Structure of L10-IrMn.
Fig. 3 Measurement of SOT efficiency (θDL,m) from ST-FMR.
Fig. 1 Operation mechanism and scanning electron microscopy images of MTC device. Operation mechanism and scanning electron microscopy images of MTC device.
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,
Fig. 6 WPS imaging of different chemical components in living cells.
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. 1 Histograms of the number of first messages received by men and women in each of our four cities. Histograms of the number of first messages received.
Fig. 5 Schematic phase diagrams of Ising spin systems and Mott transition systems. Schematic phase diagrams of Ising spin systems and Mott transition systems.
Characteristics of ultrathin single-crystalline semiconductor films
Fig. 1 Cross-sectional images of He-implanted V/Cu/V samples.
Fig. 1 Structure and absorption spectra of the P
Fig. 3 Characterization of the current-induced effective fields.
Fig. 2 Results of the learning and testing phases.
Fig. 5 The different fractions of the rates of energy flow in the oscillating thermal circuit for the experiment with L = 58.5 H shown in Fig. 4A. The.
Fig. 2 Schematic drawings of Göbekli Tepe skulls.
Fig. 2 Desirability, quantified using the measures defined here, as a function of demographic variables of the user population. Desirability, quantified.
Fig. 1 Schematic view and characterizations of FGT/Pt bilayer.
Dipole-like electrostatic asymmetry of gold nanorods
Superconducting cavity electro-optics: A platform for coherent photon conversion between superconducting and photonic circuits by Linran Fan, Chang-Ling.
Fig. 2 Asymmetric MR of LMO within the ac plane.
by Thomas Zettl, Rebecca S
Fig. 2 Images of the optical field at transmitter and receiver.
THz pulse-pump optical reflectivity probe spectroscopy on Nd2CuO4
Fig. 4 Relationships between light and economic parameters.
Toward broadband, dynamic structuring of a complex plasmonic field
by Mark T. Edmonds, James L
Fig. 1 Structural and electrical properties of Bi2Se3/BaFe12O19.
Multiplexed four- and eight-channel devices for rapid processing
Fig. 2 Realization of asymmetric photon transport.
Long-range structural order control of SS-annealed cylinder patterns
Fig. 2 Comparison of the observed DRs and the estimates by the VR model and FL. Comparison of the observed DRs and the estimates by the VR model and FL.
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. 3 Comparisons of NDVI trends over the globally vegetated areas from 1982 to Comparisons of NDVI trends over the globally vegetated areas from.
Fig. 3 Experimental verification.
Fig. 3 Characterization of translational and rotational diffusion of platelets. Characterization of translational and rotational diffusion of platelets.
Fig. 1 Sketch and schematic diagram of photobleaching reaction in a strongly coupled system. Sketch and schematic diagram of photobleaching reaction in.
Fig. 3 Electrochemical performances of symmetric cells using control Li and composite Li electrodes. Electrochemical performances of symmetric cells using.
Fig. 5 Superpositions of OAM.
Fig. 6 MD simulations of assembled binary supraballs.
Fig. 3 Supraballs and films assembled from binary 219/217nm SPs/SMPs.
Fig. 2 Supraballs and films from binary SPs.
Fig. 3 Performance of the generative model G, with and without stack-augmented memory. Performance of the generative model G, with and without stack-augmented.
Fig. 2 Growth kinetics of borophene on silver.
Fig. 2 Comparison between the different reflective metasurface proposals when θi = 0° and θr = 70°. Comparison between the different reflective metasurface.
The combined signal spectra of PSD for protons and helium nuclei
Fig. 4 Scaling laws distinguish biochemical networks from random networks across levels of organization. Scaling laws distinguish biochemical networks.
Manipulation of multiple micro/nano objects using patterned SNE
Fig. 3 Rubbery strain, pressure, and temperature sensors.
Fig. 1 Doping schematics and optical properties.
Fig. 2 DFT calculations of stability and bandstructure of gallenene polymorphs. DFT calculations of stability and bandstructure of gallenene polymorphs.
Presentation transcript:

Adaptive metalenses with simultaneous electrical control of focal length, astigmatism, and shift by Alan She, Shuyan Zhang, Samuel Shian, David R. Clarke, and Federico Capasso Science Volume 4(2):eaap9957 February 23, 2018 Copyright © 2018 The Authors, some rights reserved; exclusive licensee American Association for the Advancement of Science. No claim to original U.S. Government Works. Distributed under a Creative Commons Attribution NonCommercial License 4.0 (CC BY-NC).

Fig. 1 Principle of strain field–mediated tunable metalens. Principle of strain field–mediated tunable metalens. A metasurface (left column) is constructed by digitizing an analog optical phase profile on a flat surface into discrete cells, each of which contains a metasurface element that locally imparts the required phase shift to the incident light to reconstruct the desired wavefront (middle column; dashed line: optical axis). The wavefront generated by the metasurface determines the subsequent beam shaping (right column). (A) Original: metasurface without stretch. (B) Defocus: metasurface with uniform and isotropic stretch. (C) Astigmatism: metasurface under asymmetric stretch. (D) Shift: metasurface displaced laterally in the x,y plane. Alan She et al. Sci Adv 2018;4:eaap9957 Copyright © 2018 The Authors, some rights reserved; exclusive licensee American Association for the Advancement of Science. No claim to original U.S. Government Works. Distributed under a Creative Commons Attribution NonCommercial License 4.0 (CC BY-NC).

Fig. 2 DEA metalens device design. DEA metalens device design. (A) A schematic of the device in which a metalens and a DEA with five addressable electrodes are combined to allow for electrical control over the strain field of the metasurface. (B) Optical microscope images (scale bars, 20 μm) at (i) no voltage, (ii) 2.5 kV applied to the center electrode (V5), and (iii) 2.75 kV applied to tune x astigmatism (concurrently, V1 and V3). The dark spots are defects (either missing or tilted silicon posts) introduced during the transfer process. The corresponding two-dimensional Fourier transforms (FTs) of (i) to (iii) are shown in (iv) to (vi), respectively (normalized amplitudes). Alan She et al. Sci Adv 2018;4:eaap9957 Copyright © 2018 The Authors, some rights reserved; exclusive licensee American Association for the Advancement of Science. No claim to original U.S. Government Works. Distributed under a Creative Commons Attribution NonCommercial License 4.0 (CC BY-NC).

Fig. 3 Measurement of tuning. Measurement of tuning. (A) (Left) Z-scan of the intensity profile showing two distinct focal lengths. (Center) Image of focal spot intensity profile (that is, x-y cross sections at the position of maximum intensity). (Right) Line scans of focal spot intensity image in the x (blue) and y (red) directions in comparison to the theoretical diffraction-limited spot size (black). a.u., arbitrary units. (B) Additional images of the focal spots at 1.5, 2, and 2.5 kV are shown, captured directly by the camera without the microscope objective (scale bars, 200 μm). (Bottom right) Measured focusing efficiency for varying voltages (see fig. S6C for setup). (C) Measurement of focal length tuning using the center electrode V5 for DL and SL (inset) devices. Blue circles represent optical measurement of device focal length as a function of applied voltage. The solid blue line indicates the fit of focal length data to Eq. 3 (R2 = 0.9915). Red triangles represent measurement of stretch as a function of the applied voltage. (D) Measured Zernike coefficients of the phase profile (calculated from microscope images of the lens center) showing targeted tuning of vertical astigmatism, whereas other Zernike coefficients exhibit little change. The large defocus value represents the designed focal power of the lens. (E) Measurement of x,y shift control showing two-axis displacement control from the focus position at 0 kV (yellow star) to various positions (red dots) as 1.9 kV is applied. The gray shaded area shows possible displacements, which can be accessed by concurrently activating combinations of electrodes. Alan She et al. Sci Adv 2018;4:eaap9957 Copyright © 2018 The Authors, some rights reserved; exclusive licensee American Association for the Advancement of Science. No claim to original U.S. Government Works. Distributed under a Creative Commons Attribution NonCommercial License 4.0 (CC BY-NC).