ライフサイエンスコーパス: metamaterial

1 hanical energy using a 1D magneto-mechanical metamaterial.

2 anisotropic metasurface atop a 3D isotropic metamaterial.

3 ear field enhancement via the composition of metamaterial.

4 apabilities of the detector for the study of metamaterials.

5 pplications in plasmonics, nanophotonics and metamaterials.

6 l-vortex generation and in tunable plasmonic metamaterials.

7 ffraction limit using transparent dielectric metamaterials.

8 ting, is a promising paradigm for mechanical metamaterials.

9 e chiral Purcell effects in plasmonic chiral metamaterials.

10 t regularizations of stochastic responses of metamaterials.

11 r both the design and application of optical metamaterials.

12 ting large surface area for multi-functional metamaterials.

13 S systems, such as Mobius strips and auxetic metamaterials.

14 ) offers a promising strategy to reconfigure metamaterials.

15 mpromise the wave propagation performance of metamaterials.

16 menting folds to reconstruct sole-cuts-based metamaterials.

17 1 s, as the basis of dynamically responsive metamaterials.

18 ntum states, non-Hermitian wave physics, and metamaterials.

19 le thickness of the dielectric spacer in the metamaterials.

20 analogous to bianisotropy in electromagnetic metamaterials.

21 essable plasmonic devices and reconfigurable metamaterials.

22 ve mixing, and the filtering capabilities of metamaterials.

23 further excavate the potential of versatile metamaterials.

24 ts, but it can be extended to other types of metamaterials.

25 operties are revealed in these ceramic-based metamaterials.

26 ctural and functional limitations of thermal metamaterials.

27 cient impedance mismatch of state-of-the-art metamaterials.

28 achieve mobile information storage in these metamaterials.

29 ng blocks to construct load-bearing cellular metamaterials.

30 y explored to facilitate dynamically tunable metamaterials.

31 nisms leading to Willis coupling in acoustic metamaterials.

32 fields of plasmonics, photonic crystals, and metamaterials.

33 particles, and chiral metal metasurfaces and metamaterials.

34 ffering immense promise in stimuli-dependent metamaterials.

35 rest in recent years from the development of metamaterials.

36 optical sensors and as components of optical metamaterials.

37 ive manufacturing of molecular ferroelectric metamaterials.

38 A mechanical metamaterial, a simple, periodic mechanical structure, i

39 n was made of a unique kind of visible light metamaterial absorber comprising elliptical rings-shaped

40 ve, wide-angle and broadband electromagnetic metamaterial absorber, which can cover either a flat or

41 Achieving the broadband response of metamaterial absorbers has been quite challenging due to

42 By integrating plasmonic metamaterial absorbers with pyroelectric detectors at th

43 a wide range of systems, from cold atoms to metamaterials, active matter, and geophysical flows.

44 nalysis of the complex mode structure in the metamaterial allude to the excitation of circular surfac

45 his limit and exploit more potentialities of metamaterials, an innovative material design strategy is

46 lap between control and signal fields in the metamaterial and hot-electron diffusion effects.

47 ed represents a paradigm shift for nanoscale metamaterial and metasurface design.

48 number of sources, spatial resolution of the metamaterial and system's variables (i.e. source positio

49 ired a new paradigm of design for mechanical metamaterials and deployable structural systems.

50 ty in rotationally symmetric two-dimensional metamaterials and find one-fourth and one-third fraction

51 ilized to design micrometer-scale mechanical metamaterials and magnetically actuated 3D devices.

52 ers hold a key to unlocking the potential of metamaterials and mapping a new direction for the large-

53 aterial designs, it is proposed to represent metamaterials and model the inverse design problem in a

54 towards nanoparticle self-assembly, tunable metamaterials and next-generation spatial light modulato

55 te and experimentally investigate mechanical metamaterials and phononic crystals.

56 The recently introduced concept of rainbow metamaterials and PnCs has shown a significant potential

57 new pathway for engineering electromagnetic metamaterials and reconfigurable optical systems.

58 potential applications as photonic crystals, metamaterials and templates for porous ceramics and meta

59 nked via a shared wing membrane to form this metamaterial, and collectively they generate hard-to-att

60 static periodic topological solitons into a metamaterial, and demonstrate its implementation in real

61 s such as soft robotics, sensors, mechanical metamaterials, and deployable devices.

62 Problems of flexible mechanical metamaterials, and highly deformable porous solids in ge

63 down to 2 nm thickness to create membranes, metamaterials, and machines with micrometer-scale dimens

64 red robots, morphing structures and devices, metamaterials, and multifunctional devices with multiphy

65 which now play crucial roles in plasmonics, metamaterials, and nano-photonics.

66 even new discovery in the research domain of metamaterials, and photonics in general.

67 the scale-invariant design of 3D structures, metamaterials, and robots from 2D starting materials.

68 n certain nanophotonic and optical-frequency metamaterial applications.

69 tions, such as plasmonic, multilayer, 2D, or metamaterial applications.

70 nical design and property prediction for the metamaterials are both greatly simplified due to the pix

71 nsition dynamics in VO2, the proposed hybrid metamaterials are capable of offering ultrafast modulati

72 of ordered and disordered 2D porous elastic metamaterials are discussed.

73 s are rare in nature and no natural acoustic metamaterials are known.

74 Conventionally, kirigami metamaterials are often composed of passive cut unit cel

75 Optical metamaterials are rare in nature and no natural acoustic

76 Space-time metamaterials are represented by effective bianisotropic

77 conductivities of such mixing-based thermal metamaterials are still in digital fashion, i.e., the ef

78 Acoustic metamaterials are structures with exotic acoustic proper

79 opagation properties of the elastic waves in metamaterials are tunable through design of the periodic

80 Mechanical metamaterials are usually designed to show desired respo

81 Although non-reciprocal metamaterials are well developed for wave systems, the s

82 c patterns, a mirror image of the concept of metamaterials, are scalable and biocompatible.

83 the frequency dispersive reflectivity of the metamaterial array, different modes of the QCL output ar

84 nd composite (dual-layer) aluminium/graphene metamaterials as well as graphene and aluminium foils is

85 s been a long-term pursuit in plasmonics and metamaterials, as it can enable a range of appealing opt

86 Metamaterials assemble multiple subwavelength elements t

87 Owing to field concentration in the metamaterial at resonance, the threshold intensity for n

88 be achieved by making use of composites and metamaterials at bulk length-scales, engineering the the

89 onventional materials, generating mechanical metamaterials at multiscale with unique mechanical prope

90 as diverse as driven complex fluids, active metamaterials, biological tissues, and collections of ro

91 ctured three-dimensional units-which we call metamaterial bricks-each encoding a specific phase delay

92 he strategy is demonstrated in a multistable metamaterial by experimental tests, theoretical analysis

93 int at the possibility of designing (3 + 1)D metamaterials by incorporating time-varying bulk ENZ mat

94 w avenues for fabrication of tunable optical metamaterials by manipulating the directional self-assem

95 ate that the stopband frequency range of the metamaterial can be tuned through modification of the me

96 ddition, the relative density of the origami metamaterials can be dramatically reduced to only 2% of

97 s shown that the efficiency of many acoustic metamaterials can be enhanced by controlling an addition

98 Such metamaterials can be used as the functional elements of

99 mages by adjusting the colors of pixels, the metamaterials can form and reconfigure 3D morphologies b

100 to pull himself up, it is demonstrated that metamaterials can undergo intrinsically driven self-asse

101 The focus of this paper is on elastic metamaterials characterised by the presence of wide sub-

102 The ML produces metamaterial collimation that spreads 8x less than the e

103 arger second-harmonic intensity from the MSM metamaterial, compared to contributions from its constit

104 , and demonstrate its implementation in real metamaterials computationally and experimentally.

105 is paper, we propose a type of planar chiral metamaterial consisting of interconnected metal helix sl

106 Second, hyperbolic metamaterials consisting of ultrathin Al-doped Ag films

107 However, the required metamaterial consists of a complex array of meta-atoms,

108 Acoustic metamaterials constructed from conventional base materia

109 gned properties and experimental analysis of metamaterials constructed in 3D printing.

110 e many potential applications, which include metamaterial construction and surface-based biophysical

111 The effect is observed in a terahertz metamaterial containing 3D-chiral metallic inclusions an

112 This kind of metamaterial could find possible applications as a compo

113 approach are called directionally compliant metamaterials (DCMs) because they manifest prescribed co

114 e artificial structure of an electromagnetic metamaterial defines the way the metamaterial will inter

115 ial can be tuned through modification of the metamaterial design.

116 Metamaterials designed using this approach are called di

117 Thermal metamaterials, designed by transformation thermodynamics

118 is implicit relationship and thus facilitate metamaterial designs, it is proposed to represent metama

119 Inside such a spatiotemporal metamaterial, diffusion occurs as if the material had an

120 inematics and force response of the cellular metamaterial during folding were studied to investigate

121 Thermal imaging of the metamaterial during UV illumination reveals an apparent

122 The metamaterial electromagnetic response is controlled via

123 e structure, these systems act as biological metamaterials, eliciting unusual biological responses.

124 Recent developments in metamaterials enable the miniaturization of such computi

125 we show how a customised reflective acoustic metamaterial enables the levitation of multiple particle

126 Our work demonstrates efficient optical metamaterial engineering based on structured ensembles o

127 We demonstrate that this metamaterial exhibits a left-handed behaviour, and we di

128 The proposed cellular metamaterial exhibits unusual properties some of which s

129 re we introduce the concept of "trapped air" metamaterial, fabricated via vat photopolymerization, wh

130 n this paper, we present a novel Laser-based Metamaterial Fabrication (LMF) process for high-throughp

131 range of applications, including plasmonics, metamaterials, flexible electronics and biosensors.

132 ly analyzed by modelling the VO(2) film as a metamaterial for a temperature range close to its critic

133 The work represents the application of a metamaterial for spatial characterization, and subwavele

134 Here we propose employing hyperbolic metamaterials for a broadband impedance matching, while

135 fully leverage the innate duality of chiral metamaterials for future optical technologies, it is ess

136 eam-based lattices have dominated mechanical metamaterials for the past two decades, low structural e

137 cases of a periodic metal-dielectric layered metamaterial, from which a metal can continuously transf

138 A hybrid metamaterial/graphene device is implemented into an exte

139 is performed by electrostatic gating of the metamaterial/graphene device, demonstrating a modulation

140 The research of metamaterials has achieved enormous success in the manip

141 Most of the research effort on PnCs and metamaterials has been focused on the enhanced dynamic p

142 Acoustic filters and metamaterials have become essential components for elast

143 Emerging thermal metamaterials have been deployed to realize effective th

144 Metamaterials have been discovered that can manipulate e

145 d for wave systems, the studies of diffusive metamaterials have been limited by their characteristic

146 In spite of their great promise, however, metamaterials have been slow to find their way into prac

147 The resulting low-density mechanical metamaterials have many advantageous properties: their m

148 These mechanical metamaterials have properties that are a function of the

149 Architected materials or metamaterials have proved to be a very effective way of

150 Metamaterials have the ability to provide (a) lower freq

151 Metamaterials have unprecedented properties that facilit

152 -wavelength imaging in water using polymeric metamaterials highly effective.

153 cible Brillouin zone of the unit cell of the metamaterial (i.e. is a three-dimensional stopband).

154 is observed through a negative permeability metamaterial immersed in gaseous plasma.

155 demonstrated for a holey-structured acoustic metamaterial in water at 200-300 kHz, via both finite el

156 Here we design an inhomogeneous Weyl metamaterial in which a gauge field is generated for the

157 o combine dielectric, plasmonic and magnetic metamaterials in a single platform.

158 sent a design strategy for aperiodic elastic metamaterials in order to achieve the same performances

159 erlattices represent a new class of advanced metamaterials in that they can integrate mechanical flex

160 The emergence of multilayer metamaterials in the research field of enhancing spontan

161 hallenges associated with the development of metamaterials in the visible spectrum are the high costs

162 cturing for realising polymer-based acoustic metamaterials in water at ultrasonic frequencies.

163 Applications for such metamaterials include aerospace and transport components

164 paper, we outline a new design approach for metamaterials incorporating internal resonators, and pro

165 atched acoustic double zero refractive index metamaterial induced by a Dirac-like cone at the Brillou

166 muli-responsive materials in active kirigami metamaterials instead will enable potential mechanical p

167 oint during this transition, classifying the metamaterials into metallic state and dielectric state.

168 on of the dielectric resonator in the hybrid metamaterial is also demonstrated.

169 As the metamaterial is heated, the insulator-to-metal phase tra

170 es, xthe nonlinear chiroptical response of a metamaterial is initially completely inaccessible.

171 artificially engineer colossal permittivity metamaterials is also shown.

172 Designing mechanical metamaterials is overwhelming for most computational app

173 rowth of complex hierarchical multicomponent metamaterials is reviewed, with emphasis on key principl

174 nteraction of light with gold gyroid optical metamaterials is studied and a strong correlation betwee

175 rticles ( 100-200nm), arranged in a periodic metamaterial lattice, in direct and Attenuated Total Ref

176 used as building block of future mechanical metamaterials, leading to a new class of tunable metamat

177 Here, we demonstrate a phononic metamaterial lens (ML) for detection of laterally subwav

178 ion of electromagnetic waves in its layered, metamaterial-like structure.

179 are obtained in the tips and contours of the metamaterials made of the quasi-3D bowtie nanoantennas,

180 recent years due to the advanced functional metamaterial making the microstructures more and more co

181 Hence these metamaterials mimic a relativistic effect without the ne

182 the matching layer, efficiently excites bulk metamaterial modes, which have well-resolved spatial-tem

183 It is demonstrated here that an artificial metamaterial nanostructure comprising arrays of dielectr

184 tes the potential of utilizing quasiperiodic metamaterial nanostructures to engineer the local densit

185 rein, the development of a coupled nonlinear metamaterial (NLMM) featuring a self-adaptive response t

186 s and was found to exhibit a near zero index metamaterial (NZIM) behavior.

187 Metasurfaces are metamaterials of reduced dimensionality which have opene

188 Optical metamaterials offer the tantalizing possibility of creat

189 ipulation of input powers incident on chiral metamaterials offers potential for active optics such as

190 placing active magnetic spinners inside such metamaterials, one makes a powerful tool which allows ma

191 ction, provide a platform for all-dielectric metamaterials operating at visible frequencies.

192 ensitive ZnO spacer layer, which changes the metamaterial optical properties and causes a localized i

193 SSA designs which utilize photonic crystals, metamaterials, or cermets are either cost-inefficient du

194 materials, leading to a new class of tunable metamaterial over a wide range of operating frequencies.

195 cle absorbers called transferable hyperbolic metamaterial particles (THMMP) that display selective, o

196 With this model, metamaterial perfect absorber can be redefined as a meta

197 Here, a metamaterial plate is realized that can be dynamically t

198 Here, architected metamaterial plates with 50 nm thickness are leveraged t

199 We introduce a metamaterial platform capable of solving integral equati

200 elength-scale light-matter interactions in a metamaterial platform, our wave-based, material-based an

201 Gyroid-structured optical metamaterials possess a chiral, cubic, and triply period

202 quantitative comparison of the hierarchical metamaterials presented here to previously reported syst

203 hat electromagnetic waves inside left-handed metamaterials produce negative radiation pressure.

204 However, in all 3D mechanical metamaterials proposed to date, the topological modes ar

205 Metamaterials provide a powerful platform to probe and e

206 rinsic scalability of these photonic fractal metamaterials provide ample opportunities for applicatio

207 ication of device-quality, nanocrystal-based metamaterials [Q.

208 Here we propose and demonstrate the magnetic metamaterial quarter-wave turbines at visible wavelength

209 current physical realizations of mechanical metamaterials remain hindered by the lack of rapid-proto

210 The primary objective of acoustic metamaterial research is to design subwavelength systems

211 tral theme in contemporary nanophotonics and metamaterials research.

212 in the infrared spectral range, by reporting metamaterial resonances in chalcogenide crystals sustain

213 ching system shows for the first time that a metamaterial resonator can be detuned during transmissio

214 ching system that can automatically detune a metamaterial resonator to enhance magnetic resonance ima

215 implementation seen in this evolved acoustic metamaterial reveals enticing ways to design high-perfor

216 ing, allowing dynamic reconfiguration of the metamaterial's frequency band and wave impedance.

217 (i.e. source position, phase and amplitude, metamaterial's geometry, relative position of the levita

218 A metamaterial sensing chip was designed for increasing of

219 Hz time-domain spectroscopy system, THz nano-metamaterial sensing chips were prepared for great enhan

220 ich may find applications for fabrication of metamaterials, sensors, plasmonics, and micro/nanoelectr

221 ing the sensitivity of subwavelength grating metamaterial (SGM) waveguide based sensors is challengin

222 le the four significant functions of thermal metamaterials-shield, concentrator, diffuser, and rotato

223 When backed with a silver coating, the metamaterial shows a noontime radiative cooling power of

224 tching, while a structured layer on top of a metamaterials slab ensures an efficient and directive en

225 many emerging applications (e.g., responsive metamaterials, soft robotics).

226 applications to electromagnetic and photonic metamaterials, some success in extending the operating d

227 scale electrodynamic properties of plasmonic metamaterials, strongly correlated quantum materials, an

228 lectric properties of an active KTaO3 hybrid metamaterial structure and its tunability under external

229 The proposed metamaterial structure can find applications in polariza

230 A split-cube-resonator-based metamaterial structure that can act as a polarization- a

231 This forms a tunable metamaterial structure which couples to the cavity throu

232 Two active metamaterial structures are fabricated that, despite sti

233 The macroscopic metamaterial structures demonstrate the potential of thi

234 the lack of rapid-prototyping ferroelectric metamaterial structures.

235 ch limit the applicability of the concept to metamaterials such as microfabricated metal-air hybrids.

236 Antenna (A-SBFA), augmented with anisotropic metamaterial surfaces (metasurfaces), has been designed

237 ing the potential of this nanoparticle-based metamaterial synthesis platform.

238 alized with an exterior cloaking in a hybrid metamaterial system, is demonstrated.

239 r feature sizes as the basis of a mechanical metamaterials system capable of supporting positive/nega

240 ndomly in a polymeric matrix, resulting in a metamaterial that is fully transparent to the solar spec

241 icated as embedded parts of microarchitected metamaterials that are capable of interacting mechanical

242 nd propose a design principle for mechanical metamaterials that can be easily and reversibly transfor

243 enabled the design of stretchable mechanical metamaterials that can be easily realized by embedding a

244 a kirigami-inspired class of 2D hierarchical metamaterials that can effectively convert the thermal m

245 However, the use of polymer-based metamaterials that could operate in water is difficult,

246 Hybrid metamaterials that exhibit reconfigurable responses unde

247 city in static systems, realizing mechanical metamaterials that exhibit vastly different output displ

248 Mechanical metamaterials that leverage precise geometrical designs

249 n ices are geometrically frustrated magnetic metamaterials that offer vast untapped potential due to

250 -field engineering, including examples of 2D metamaterials that transform into 3D surfaces upon heati

251 By tuning the geometry of the metamaterial, the reflection coefficient of the panel ca

252 Furthermore, using the optimized metamaterials, the acoustic fields with Hopf link and tr

253 By tuning the resonant frequency of the metamaterial through an applied magnetic flux, one can t

254 ry properties of the response of an acoustic metamaterial to establish the fragile nature of the low-

255 plate architectures as a superior mechanical metamaterial topology.

256 Local sensitivity-enhancing metamaterials typically consist of resonant components,

257 intricate scale layer on moth wings forms a metamaterial ultrasound absorber (peak absorption = 72%

258 ng matter and information between autonomous metamaterial unit cells.

259 design and propose a linear diatomic elastic metamaterial using dual-resonator concept to obtain larg

260 of intense study have passed since the term metamaterials was first introduced in 1999.

261 Here, using plasmonic metamaterials, we demonstrate that coherent spectroscopy

262 Hyperbolic metamaterials were initially proposed in optics to boost

263 sformative design demonstrates how practical metamaterials, when applied to conventional antenna tech

264 optimisation technique for the design of the metamaterial, where the local height of the surface is u

265 enabled fabrication of phononic crystals and metamaterials which exhibit spectral gaps, or stopbands,

266 e mechanism, we devise and test a mechanical metamaterial, which curls under homogeneous mechanical s

267 of complex structures, the inverse design of metamaterials, which aims to retrieve the optimal struct

268 symmetric diffusion characteristics inside a metamaterial whose material parameters are space- and ti

269 This study reports origami-based metamaterials whose electromagnetic responses are dynami

270 Nevertheless, hybrid terahertz (THz) metamaterials whose spectral performance can be dynamica

271 l dipolar excitation at optical frequency in metamaterials whose unit cell consists of three identica

272 -wavelength unit cells, the liquid interface metamaterial, whose geometry is controlled by the wave p

273 tromagnetic metamaterial defines the way the metamaterial will interact with electromagnetic waves, a

274 normal lower thermal conductivity in the MIM metamaterial with Ag layer thickness below 25 nm is disc

275 by this wave trapping phenomenon, a rainbow metamaterial with linear spatial-frequency trapping is a

276 For a piece of the 3D pixel metamaterial with m n-unit MPs, the number of programmab

277 s understanding of metal and dielectric: The metamaterial with metal filling ratio larger/smaller tha

278 to-classical analogy, we create a mechanical metamaterial with nonreciprocal interactions, in which w

279 e stiffness for dynamic tuning of mechanical metamaterials with a long lifetime and sustainability.

280 Metamaterials with acoustic and elastic band gaps are of

281 Optical metamaterials with an artificial subwavelength structure

282 Acoustic metamaterials with artificial microstructures are attrac

283 Programmable kirigami metamaterials with controllable local tilting orientatio

284 novel design approaches for metasurfaces and metamaterials with electrical tunability offering real-t

285 ttom-up process with which to create ordered metamaterials with emergent functionalities.

286 rix (or Hamiltonian), enabling the design of metamaterials with emergent properties that escape a sta

287 cal magnetic circuitry, as well as plasmonic metamaterials with high fidelity.

288 oft actuators interaction, including elastic metamaterials with human gesture-controlled bandgap beha

289 ue" chi((0)) < 0 is proposed based on active metamaterials with internal power sources.

290 In spite of previous work on metamaterials with large or ultralow coefficient of ther

291 Artificially structured metamaterials with metallic or dielectric inclusions are

292 al organization, hierarchical multicomponent metamaterials with nonlinear spatially reconfigurable fu

293 tools for the effective design of plasmonic metamaterials with on-demand functionality.

294 embedded into the acoustic field by designed metamaterials with only 24 x 24 pixels.

295 ion of water-soluble molecular ferroelectric metamaterials with precise spatial control in virtually

296 nic density of states provided by hyperbolic metamaterials with the light-scattering efficiency of PC

297 relevance to the design of novel mechanical metamaterials with unique/unusual properties such as str

298 Advanced mechanical metamaterials with unusual thermal expansion properties

299 the creation of acoustic vortex knots using metamaterials, with decoupled modulation of transmitted

300 re, we report the design of a 3D topological metamaterial without Weyl lines and with a uniform polar