about
Spin and wavelength multiplexed nonlinear metasurface holographyPhotonic Weyl degeneracies in magnetized plasma.Helicity multiplexed broadband metasurface holograms.Plasmonic nanoparticle scattering for color hologramsContinuous control of the nonlinearity phase for harmonic generations.Giant Kerr nonlinearity and low-power gigahertz solitons via plasmon-induced transparency.One-way helical electromagnetic wave propagation supported by magnetized plasma.Shaping 3D Path of Electromagnetic Waves Using Gradient-Refractive-Index Metamaterials.Electromagnetic reprogrammable coding-metasurface holograms.Direct observation of topological surface-state arcs in photonic metamaterialsSingle-pixel computational ghost imaging with helicity-dependent metasurface hologram.Electrical access to critical coupling of circularly polarized waves in graphene chiral metamaterials.Spin-enabled plasmonic metasurfaces for manipulating orbital angular momentum of light.Broadband all-dielectric magnifying lens for far-field high-resolution imaging.Imaging through Nonlinear Metalens Using Second Harmonic Generation.Nonlinear Metasurface for Simultaneous Control of Spin and Orbital Angular Momentum in Second Harmonic Generation.Sub-Poissonian shot noise of a high internal gain injection photon detector.Dielectric Meta-Holograms Enabled with Dual Magnetic Resonances in Visible Light.Ideal Weyl points and helicoid surface states in artificial photonic crystal structures.Metasurface holograms reaching 80% efficiency.Ultrathin Nonlinear Metasurface for Optical Image Encoding.Disorder-Induced Topological State Transition in Photonic Metamaterials.Three Dimensional Photonic Dirac Points in Metamaterials.Giant Nonlinear Optical Activity of Achiral Origin in Planar Metasurfaces with Quadratic and Cubic Nonlinearities.Dual field-of-view step-zoom metalens.Multichannel Polarization-Controllable Superpositions of Orbital Angular Momentum States.Enhanced infrared transmission through subwavelength coaxial metallic arrays.Line Degeneracy and Strong Spin-Orbit Coupling of Light with Bulk Bianisotropic Metamaterials.Metasurface Enabled Wide-Angle Fourier Lens.Phenomenological modeling of geometric metasurfaces.Symmetry-selective third-harmonic generation from plasmonic metacrystals.Manipulation of vector beam polarization with geometric metasurfaces.Controlling the plasmonic orbital angular momentum by combining the geometric and dynamic phases.Experimental observation of photonic nodal line degeneracies in metacrystals.Addressable metasurfaces for dynamic holography and optical information encryption.Tailoring MoS2 Valley-Polarized Photoluminescence with Super Chiral Near-FieldMacroscopic broadband optical escalator with force-loaded transformation opticsMimicking celestial mechanics in metamaterialsPseudospin-induced chirality with staggered optical graphene.Observation of chiral zero mode in inhomogeneous three-dimensional Weyl metamaterials
P50
Q27342923-446A6B87-7C8C-470E-BFB5-1EC3445FD7B0Q30375645-C3574F14-27C7-4E91-8AA4-89D01189F87DQ30665260-728744FA-1B8A-439C-97CF-1A1D2FD1AFFEQ34144732-97536110-2D4D-4A40-9F8E-3A5AF3A97EF8Q35596575-D1F4023D-33AB-404D-973B-A9D9A92D3E40Q36035323-7258AC40-9728-4E8D-86C9-F68DD56B0911Q36587506-A3BEF776-40EB-4B63-A70E-16E69A3DE7B1Q37423132-C134EA4C-353D-408D-B8C4-D89D1A27427FQ38642256-D3725E32-E5EB-4E9F-A92B-109FF12E95ACQ41094617-A13FBFCE-3756-41C3-AD8E-C62CC72AB9CCQ41499074-A397BC2C-CB47-4731-9D8B-6E639B5799EBQ42367706-EBA008F0-70DD-4277-9116-8D4E3C5A9F21Q44632314-F18554D2-79F6-464B-9A0E-BB941378519EQ46889185-FDF634D8-2654-4BD8-9B5D-9B9183D8D695Q47189524-9D18637A-D553-4EE0-8611-FBD25D325EB8Q47342254-015239C2-E844-496B-8E76-33F56A81D704Q47393964-319E9DF6-D2BB-4F00-85CB-2F624DD249A4Q47685186-9F5AE4B5-BF27-461D-BA4A-C511DA4F6EA0Q48043444-71F79381-4774-427A-B00C-CC8DE36A538DQ48222569-A48E5D4B-ACE6-4FD3-A799-F8E4D22863DDQ48274138-DBEA5DF2-CC2F-4912-9F65-18A62C3E15BDQ50011342-35341472-F40D-45B0-A0DA-75DE83863A66Q50013563-E7A7B4F8-1162-44B4-97B8-6F606769D079Q50704968-F83819B5-570F-460C-993F-0A81F4BDFF06Q50761126-267ACBA7-9DDE-4D0A-8BFE-C26505DBDDCFQ51001932-94ED7E20-25CE-4773-B461-4E1728BCDB61Q51543076-799CCFB1-2468-4D22-B165-7415C5ADDEB3Q51799703-39951D52-7E07-4A30-8288-8D3291A4B38AQ52577671-BFF753C1-4F58-42A9-B178-A93C4C6FC69BQ53114470-26615613-01C9-48C4-BDB4-97B6D1164CADQ53484293-821A9AE2-60F3-4344-9836-DE3FBC682091Q53804300-086A1405-0052-4238-B08E-0C6011CFAB17Q54365805-AB1C86D9-7A81-4C4D-B390-F4B19EE71E5FQ55097504-78EFDF65-105E-43BD-8795-4AA256E747A1Q55447784-29BE5C70-5E34-4071-AA5B-BF65464D9856Q57721353-1021D042-85F7-4EF7-B2AD-DAAD30B60170Q58468636-A7C5B56D-C9CE-4A06-A219-C5A0074E3C5DQ61773535-980DEA91-21D0-4394-B022-6EAEB128DADDQ64914620-E3F51CAD-E090-4FC6-98AF-64E2237CFB02Q75720782-FE41D9E1-06AC-4EF2-9797-C9746EE32092
P50
description
onderzoeker
@nl
researcher ORCID ID = 0000-0003-4556-2333
@en
name
Shuang Zhang
@ast
Shuang Zhang
@en
Shuang Zhang
@es
Shuang Zhang
@nl
type
label
Shuang Zhang
@ast
Shuang Zhang
@en
Shuang Zhang
@es
Shuang Zhang
@nl
prefLabel
Shuang Zhang
@ast
Shuang Zhang
@en
Shuang Zhang
@es
Shuang Zhang
@nl
P108
P106
P108
P1153
56114326700
P31
P496
0000-0003-4556-2333