ライフサイエンスコーパス: photonic

1 any areas, including catalysis, sensing, and photonics.

2 munication, microwave photonics, and quantum photonics.

3 s, optical frequency division, and microwave photonics.

4 nductor devices for advanced electronics and photonics.

5 d light propagation control in acoustics and photonics.

6 y considered light absorption and structural photonics.

7 nergy conversion devices, photovoltaics, and photonics.

8 roles in plasmonics, metamaterials, and nano-photonics.

9 ay have potential for device applications in photonics.

10 linary fields of materials, electronics, and photonics.

11 such as integrated circuits, memristors, and photonics.

12 omputing, quantum information, and microwave photonics.

13 f excitonic modes, paving the way to exciton-photonics.

14 otonic modes, the cornerstone of topological photonics(13-15).

15 expanded from condensed matter physics into photonics(4), giving rise to a new type of lasing(5-8) u

16 This work shows that a modular and coherent photonic-aided payload is feasible, making way to an ext

17 Here, we demonstrate a coherent photonic-aided receiver meeting such demands.

18 However, photonic amplification is generally tied to high optical

19 Kagome-nets, appearing in electronic, photonic and cold-atom systems, host frustrated fermioni

20 ability of large-size devices to silicon for photonic and electronic applications.

21 ecent advances in microchip-based integrated photonic and electronic circuitry with those from optoge

22 p laser on, thereby eliminating the need for photonic and electronic control circuitry.

23 n transport at room temperature promises new photonic and optoelectronic applications such as efficie

24 stal structure and electronic properties for photonic and optoelectronic applications.

25 to industrial-scale production of integrated photonic and optoelectronic devices on Si platforms in a

26 ed light absorption and hence performance in photonic and optoelectronic devices.

27 In this context, photonic and redox stimuli represent highly appealing mo

28 n filters and low-loss, integrated planar IR photonics and in dictating polarization control.

29 a conceptually new approach for oxide-based photonics and nanoelectronics and opens up new routes fo

30 harge and energy flow in various electronic, photonic, and energy conversion devices.

31 amond via strain engineering for electronic, photonic, and quantum applications.

32 their applicability in organic electronics, photonics, and artificial photosynthesis.

33 res, the fabrication strategies for flexible photonics, and corresponding emerging photonic-related a

34 for applications in the fields of catalysis, photonics, and electronics.

35 ritical for applications in nanoelectronics, photonics, and energy generation and storage.

36 quantum information processing and microwave photonics, and examine how these generic chips can accel

37 -dimensional superconductivity, electronics, photonics, and information technologies.

38 uding biophysics, diagnostics, therapeutics, photonics, and nanofabrication.

39 energy conversion, ultrafast switching, nano-photonics, and nonlinear optics.

40 pplications in data communication, microwave photonics, and quantum photonics.

41 exciting research area for a broad range of photonic applications due to its tunable spectral range

42 ut the scalability of present PCM-integrated photonic applications is still limited by the poor optic

43 -formed nano-crystals prove effective in the photonic applications tested compared to the chemically-

44 However, for several practical photonic applications, efficient near infrared (NIR) to

45 materials facilitates a range of prospective photonic applications, including stereoscopic displays,

46 s new class of low-energy emitters in future photonic applications, such as nonclassical light source

47 ritical needs, as well as promising emerging photonic applications.

48 implanted Si is a candidate for quantum and photonic applications; however, several different Er cen

49 e proposed absorber suitable in varieties of photonics applications, in particular photovoltaics, the

50 ls that contain reconfigurable protein-based photonic architectures and, as a result, possess tunable

51 f dye-appended DNA sequences into programmed photonic architectures is promising.

52 Nature features a plethora of extraordinary photonic architectures that have been optimized through

53 grate large numbers of artificial atoms with photonic architectures to enable large-scale quantum inf

54 ength division multiplexing-based electronic-photonic arithmetic logic unit, which disentangles the e

55 Here we propose integrated photonics as a candidate platform for the implementation

56 of a lens, we demonstrate the use of silicon photonics as a viable platform for computational imaging

57 ce, ranging from ultracold atomic physics to photonics, as it provides a versatile platform for reali

58 d as a self-assembled template for isotropic photonic band gap (PBG) materials for transverse electri

59 ty and 3D long-range periodicity featuring a photonic band gap (PBG) that is tunable through the supe

60 leverage the large, complete, and isotropic photonic band gaps provided by hyperuniform disordered s

61 ndex contrast of about 2, which means that a photonic bandgap could be achieved using known materials

62 mers allows additional degrees of freedom in photonic bandgap design through directed protein conform

63 potentially be used to make materials with a photonic bandgap(1-3).

64 control over the reflection (through the 3D photonic bandgap) and the transmission (through 2D diffr

65 al properties, including a wide and complete photonic bandgap.

66 Photonic bandstructure calculations reveal that the resu

67 ling a grating meta-structure which performs photonic beam engineering.

68 ed nanostructured interfaces that extend the photonic behavior of natural materials, and they spur ma

69 d resonator(17-19) to implement asynchronous photonic Bell-state measurements, which are a key compon

70 apability not typically found in traditional photonic bioderived materials without compromising their

71 t proteins and silk proteins serve as edible photonic biomaterials and the photoluminescent propertie

72 technology, including recent developments in photonic building blocks and circuit architectures, as w

73 portunities not only for adaptive optics and photonics but also for any platform that can benefit fro

74 ogenides, are of interest in electronics and photonics but remain nonmagnetic in their intrinsic form

75 ble in principle their efficient coupling to photonic cavities having the optical mode volume close t

76 ptical and spin transitions while coupled to photonic cavities that enhance the light-matter interact

77 le efficient electro-optic driving of high-Q photonic cavity modes in both adiabatic and non-adiabati

78 tionary impact on many disciplines including photonics, chemical sensing, and medical diagnostics.

79 (MORIMSs) built on a CMOS compatible silicon photonic chip that addresses all of the stringent requir

80 ve method to probe the polarization within a photonic chip.

81 and it suggests future technologies such as photonic chips that can be reconfigured using non-contac

82 devices, in particular for hybrid integrated photonic chips which exploit the out-of-plane dipole ori

83 monstrating key building blocks analogous to photonic circuit components, we establish the functional

84 opportunely designed nanometric holes in the photonic circuit, which are available for analyte detect

85 ke layered crystal waveguides attractive for photonic circuitry and for studying hybrid light-matter

86 egy is successfully adapted for implementing photonic circuits and diffractive elements with greater

87 ips can accelerate the development of future photonic circuits by providing a higher-level platform f

88 ible to build increasingly large and complex photonic circuits on the surface of a chip.

89 in complexity has introduced a generation of photonic circuits that can be programmed using software

90 o implement next-generation light sources in photonic circuits with low energy, high data traffic, an

91 AlN actuators(14) on ultralow-loss Si(3)N(4) photonic circuits(15), we demonstrate voltage-controlled

92 ators, which are the essential components of photonic circuits, still requires considerable improveme

93 um optomechanical resonators, and integrated photonic circuits.

94 turization of components and interconnect of photonic circuits.

95 an enable the development of next-generation photonic circuits.

96 d the degrees of freedom in the design of IR photonic components exploiting the in-plane anisotropy o

97 Here, we propose an electronic-photonic computing architecture for a wavelength divisio

98 uture power-saving and high-speed electronic-photonic computing circuits.

99 Their photonic counterparts recently allowed for the control o

100 Semiconductor III-V photonic crystal (PC) laser is regarded as a promising u

101 ted single-mode nanocavities inside a planar photonic crystal (PC).

102 hexagonal GaN nanorod-based two-dimensional photonic crystal (PhC) slab for phosphor-conversion whit

103 , we experimentally demonstrate two types of photonic crystal (PhC) solar cells architectures that ex

104 er in Maxwell's equations for a gyromagnetic photonic crystal (PhC) through a double-band-inversion p

105 ermal radiation from a micro-cavity/tungsten photonic crystal (W-PC) and a blackbody, which are both

106 eezers comprising plasmonic nanoantennas and photonic crystal cavities have been explored for stable

107 he subwavelength volume of a single, silicon photonic crystal cavity.

108 address this challenge, we use a hollow-core photonic crystal fiber (HC-PCF) that guides light at the

109 nder certain conditions in a one-dimensional photonic crystal is predicted.

110 peed LN electro-optic modulators, based upon photonic crystal nanobeam resonators.

111 layer WS(2) excitons coupled to a nontrivial photonic crystal protected by pseudo time-reversal symme

112 entally demonstrate a class of resonances in photonic crystal slabs that radiate only towards one sid

113 A photonic crystal surface mode imaging (PCSMi) technique

114 tomic motion near the surfaces of nanoscopic photonic crystal waveguides (PCWs).

115 ectional coupling into a six-way crossing of photonic crystal waveguides.

116 plasmonic nanohole array and 1 ng/mL for the photonic crystal-based sensing platform.

117 Photonic crystals are some of the more spectacular reali

118 However, common photonic crystals are unfit for in-operando on/off contr

119 ZAS at elevated temperature forms 3D chiral photonic crystals that enable negative circular dichrois

120 The bioanalytical performance of these photonic crystals was experimentally demonstrated in a m

121 mplates for forming high-dielectric-contrast photonic crystals with cubic diamond symmetry.

122 ass of functional colloids and zeolite-based photonic crystals with the ability to manipulate light i

123 makes use of the valley degree of freedom in photonic crystals(10,11), analogous to two-dimensional g

124 our classic optical phenomena-diffraction in photonic crystals, absorption of plasmonic nanostructure

125 l (2D) counterparts in fields of plasmonics, photonic crystals, and metamaterials.

126 hologies for their potential applications as photonic crystals, metamaterials and templates for porou

127 Current SSA designs which utilize photonic crystals, metamaterials, or cermets are either

128 refractive index, surface plasmon resonance, photonic crystals, turbidity, mechanical displacement, i

129 This work presents the first silicon photonic data link using a monolithic rare-earth-ion-dop

130 ena are found, such as an enhancement of the photonic density of states, polariton canalization and h

131 locations, which severely degrade electronic/photonic device performances(6-8), is fundamentally unav

132 ently, state of the art integrated nonlinear photonic devices are mainly based on dielectric material

133 ogenides, thus opening new opportunities for photonic devices based on high refractive index material

134 Integrated photonic devices based on Si(3)N(4) waveguides allow for

135 hnique, the fabrication of 2D and 3D magneto-photonic devices containing a single QD is performed on

136 nities for controlling optical properties of photonic devices dynamically.

137 loidal nanocrystal solids for electronic and photonic devices necessitates that their thermal-transpo

138 Designing modern photonic devices often involves traversing a large param

139 proach can open up a new route to form novel photonic devices with planar metasurfaces, for example,

140 re confer advantages in applications such as photonic devices(5-7), optical cloaking(8,9), biochemica

141 cales, temperature control within integrated photonic devices, and solid-state laser refrigeration of

142 l importance for their application in future photonic devices.

143 and glasses to cameras, digital displays and photonic devices.

144 escent nanomaterials in imaging, sensing and photonic devices.

145 e material platform for novel electronic and photonic devices.

146 n entirely new range of infrared and thermal photonic devices.

147 ntial for applications in spin-valley-locked photonic devices.

148 y has been extensively studied, with various photonics devices and optical links being demonstrated.

149 ropy, enable control and manipulation of the photonic dispersion of phonon polaritons in van der Waal

150 Here, we theoretically show that the photonic doping concept can be extended to non-Hermitian

151 erforming electronic (e.g., transistors) and photonic (e.g., photovoltaics, photodetectors or LEDs) t

152 this work, we relate these phenomena to the photonic effect.

153 many areas of science and technology such as photonics, electronics, and mechanics with a wide range

154 onians in optical cavities opens the door to photonic emulators of quantum Hamiltonians with internal

155 Next-generation photonics envisions circuitry-free, rapidly reconfigurab

156 el insect observation and control tools, the Photonic Fence detects and tracks mosquitoes and other f

157 nging shape as a result of nonlinearity-in a photonic Floquet topological insulator.

158 s scaling factor and characterization of the photonic flux within each reactor, the cross-coupling wa

159 features and intrinsic scalability of these photonic fractal metamaterials provide ample opportuniti

160 Emerging photonic functionalities are mostly governed by the fund

161 transition from the photonic paramagnetic to photonic glass phase is more subtle in that the Parisi o

162 ies, such as core-shell particles or inverse photonic glasses-explaining recent experimental findings

163 itons at the zigzag edge of a reconfigurable photonic graphene lattice created via the effect of elec

164 -optic circuits on a single chip, integrated photonics has revolutionized the interconnects and has s

165 Recent research advances in photonics have sparked interest in using a network of co

166 eration, attosecond pulse generation, plasma photonics, high-field physics and laboratory astrophysic

167 By exciting Dirac-like cones in photonic honeycomb (pseudospin-1/2) and Lieb (pseudospin

168 c pre-processors or accelerators, electronic-photonic hybrid circuits, and neural networks.

169 Employing its photonic implementation of evanescently coupled waveguid

170 k suggests speedups in heuristic methods via photonic implementations of the PRIS.

171 , making way to an extensive introduction of photonics in next generation communications satellites.

172 Topological photonics in strongly coupled light-matter systems offer

173 e way for future explorations of topological photonics in systems with open boundary conditions and f

174 towards monolithically integrated non-linear photonics in the molecular fingerprint region beyond 6 m

175 We explore and discuss the liquid crystal photonics in the prototype that has a novel optical desi

176 the first time it has been incorporated on a photonic integrated chip.

177 ntaining highly coherent colour centres-on a photonic integrated circuit (PIC).

178 A direction for further developments in photonic integrated circuit technology is also discussed

179 Significant advances have been made in photonic integrated circuit technology, similar to the d

180 Reconfigurability of photonic integrated circuits (PICs) has become increasin

181 Modern advanced photonic integrated circuits require dense integration o

182 cial foundation for realizing large-scale LN photonic integrated circuits that are of immense importa

183 in future large-scale silicon electronic and photonic integrated circuits.

184 the improvement of optoelectronic devices in photonic integrated circuits.

185 ate (LN) emerges as a promising platform for photonic integrated circuits.

186 anisotropic optical devices used for future photonic integration, optical communication and optical

187 ide-integrated DLA that was designed using a photonic inverse-design approach.

188 While integrated photonics is a robust platform for quantum information p

189 ion is increasingly and successfully used in photonics, it has yet to replicate any of these complex

190 with an adiabatic multimode-to-single-mode "photonic lantern" transition formed at the distal end by

191 dent control over both the plasmonic gap and photonic lattice modes of the surface-confined particle

192 allows for mechanically shaping them in the photonic lattice.

193 Although the mapping is observed in photonic lattices where pseudospin-orbit interaction tak

194 quantum walks in new proposed quasiperiodic photonics lattices are highly controllable due to the de

195 fibers provide a new class of quasiperiodic photonics lattices possessing both on- and off-diagonal

196 when the rotation between the layers is at a photonic magic twist angle.

197 Photonic materials designed at wavelength scales have en

198 e learned from plants and animals to produce photonic materials from biopolymers are discussed.

199 iberate engineering of the band structure in photonic materials is known to be an effective approach

200 Newly developed photonic materials permit subambient cooling under direc

201 Photonic materials with angular-independent structural c

202 e for use in advanced organic electronic and photonic materials with burgeoning considerations for bi

203 inescence properties of multipiezo and piezo-photonic materials, and to explore their potential as no

204 ng chemical and electrical barrier coatings, photonic materials, biomaterials, and pharmaceutical ora

205 rted for the engineering of tunable resonant photonic media with thickness exceeding the plasmonic ne

206 Advance of photonics media is restrained by the lack of structuring

207 In applications to electromagnetic and photonic metamaterials, some success in extending the op

208 st biosensing modalities, such as label-free photonic methods based on dielectric resonances.

209 Here, we demonstrate the use of silicon photonic microring resonator arrays as a postcolumn dete

210 itions of semiconductor quantum wells to the photonic mode of a metallic cavity in order to custom-ta

211 Random photonic modes have been investigated for their basic ph

212 Propagating photonic modes make layered crystal waveguides attractiv

213 of lasing(5-8) using topologically protected photonic modes that can efficiently bypass corners and d

214 ur results unveil the intrinsic chirality of photonic modes, the cornerstone of topological photonics

215 d by random systems is their high density of photonic modes, which span a large range of spectral res

216 detector (SNSPD) directly coupled to a CMOS photonic modulator, without the need for an interfacing

217 experimentally, the manipulation of FWM in a photonic molecule based on two side coupled silicon micr

218 of butterfly scale laminae, which are simple photonic nanostructures.

219 red, opal, and chiral structures, as well as photonic networks in contrast to traditionally considere

220 mplement a scalable circuit architecture for photonic neural networks, successfully demonstrating pat

221 on to fabricate sustainable, responsive soft photonic objects.

222 ture experimental exploration of topological photonics on this nonlinear, reconfigurable platform.

223 gical advances in fields including spin-Hall photonics, optical holography, compressive imaging, elec

224 We integrate a photonic oxygen biosensor into the 3D tissue scaffold an

225 we suggest the implementation of the PRIS in photonic parallel networks, which realize these operatio

226 However, the transition from the photonic paramagnetic to photonic glass phase is more su

227 and systemization of chiro-optical chips in photonics, photochemistry, biomedical engineering, chemi

228 Such "photonic pigments" have several key advantages over thei

229 integration of laser sources on the silicon photonic platform, which is fully compatible with the CM

230 physics and material sciences beyond the 2D photonic platform: equivalent mapping occurs for 3D topo

231 r novel, compact and high-speed neuromorphic photonic platforms for future computing and Artificial I

232 also adaptable to other non-centrosymmetric photonic platforms for ultrafast nonlinear optics with s

233 rm conventional electronic solutions such as photonic pre-processors or accelerators, electronic-phot

234 ural networks and general-purpose integrated photonic processors.

235 have shown extraordinary optoelectronic and photonic properties.

236 linear optics have revolutionized integrated photonics, providing on-chip solutions to a wide range o

237 um information processing, architectures for photonic quantum computing place stringent demands on hi

238 applications ranging from GHz electronics to photonic quantum devices.

239 increasingly important in the development of photonic quantum networks.

240 orm would open many avenues in silicon-based photonics, quantum technologies and energy harvesting.

241 This effect has been shown to be photonic rather than thermal, but the exact plasmonic me

242 Here, we present the Photonic Recurrent Ising Sampler (PRIS), a heuristic met

243 or can be fabricated by a single pulse laser photonic-reduction stamping.

244 cellulose can be used to fabricate broadband photonic reflectors, thermally super-insulating aerogels

245 exible photonics, and corresponding emerging photonic-related applications.

246 ng spin coherence and single-shot readout in photonic resonators.

247 nced materials, biomaterials, smart systems, photonics, robotics, textiles, Big Data and ICT (informa

248 ncept has been translated to two-dimensional photonic scenarios in connection with host media charact

249 lts are achieved by a simple modification of photonic sensing chips which are already on the market t

250 nderlying almost all current developments of photonic signal processing units.

251 Miniaturized photonic sources based on semiconducting two-dimensional

252 Yet, hardware-friendly systems of photonic spiking neurons able to perform processing task

253 des (exciton polaritons) that are subject to photonic spin-orbit coupling(11) from which Dirac cones

254 lity for optoelectronics, energy conversion, photonics, spintronics and quantum devices requires crea

255 bulk acoustic wave resonances (HBAR) in the photonic stack.

256 text, we propose a new design for a Si-based photonic structure that enables the realization of on ch

257 dvantage that can be linked to the fact that photonic structures are fundamentally modular: each part

258 Biological photonic structures can precisely control light propagat

259 ngineered dispersion in optical materials or photonic structures constrained by a low delay-bandwidth

260 The integration of chiral organization with photonic structures found in many living creatures enabl

261 s for constructing synthetic multifunctional photonic structures owing to their renewability, biocomp

262 ment found in nature, such as the nanoporous photonic structures that evolved in cuticles of beetles.

263 , single photons that can be integrated into photonic structures to amplify, direct, and tune their e

264 many living creatures enables unique chiral photonic structures with a combination of selective ligh

265 We introduce various photonic structures, including multi-layered, opal, and

266 n of corresponding biopolymers for synthetic photonic structures, the fabrication strategies for flex

267 ave retrieved the most stereotypical natural photonic structures.

268 lding blocks for realizing unique bioenabled photonic structures.

269 Different periodic photonic surface structures with rich diffraction phenom

270 demonstration of CMOS-compatible integrated photonic surface-trap fabrication, robust packaging and

271 able nonvolatile electrically reconfigurable photonic switches using PCM-clad silicon waveguides and

272 Current photonic switches, however, mainly rely on materials wit

273 hese fields usually requires highly scalable photonic switching units as essential building blocks.

274 imple, user-friendly, low-cost, and portable photonic system for in situ detection of low cyanobacter

275 How natural photonic systems manage light scattering and what can be

276 nt due to the growing demands for electronic-photonic systems on a chip driven by emerging applicatio

277 cale CMOS-integrated programmable electronic-photonic systems such as optical neural networks and gen

278 erious effects that limit the performance of photonic systems.

279 rtunities for inference based on optical and photonic systems.

280 orlds of quantum superconducting systems and photonics systems.

281 by micro-electronic platforms, but recently, photonic techniques for neuronal emulation have emerged

282 limits of electrical interconnects, silicon photonic technology has been extensively studied, with v

283 The growing maturity of integrated photonic technology makes it possible to build increasin

284 Using a label-free, silicon photonic technology, we constructed arrays of Nanodiscs

285 f the well-established and developed silicon photonics technology.

286 e physics of microcavities and non-Hermitian photonics, these results help clarify fundamental sensit

287 emerging fields of non-Hermitian optics and photonics, this suggests considering more general gain-l

288 tions in diverse fields ranging from dynamic photonics to energy and safety issues.

289 o use polarization optics via liquid crystal photonics to improve the foveated display performance.

290 bulk, fully using the entire footprint of a photonic topological insulator.

291 s and interacting photons(18-22), but so far photonic topological insulators in synthetic dimensions

292 In photonics, topological lattices with synthetic dimension

293 ersal phenomenon that applies to electronic, photonic, ultracold atomic, mechanical, and other system

294 In photonics, wave instabilities result in modulated light

295 On-chip planar photonic waveguide-based beam engineering offers the pot

296 Previous experiments on edge states in photonics were carried out mostly in linear regimes, but

297 tificial magnetic field in three-dimensional photonic Weyl systems and may have potential for device

298 ration, and high information-capacity planar photonics, which may have a profound impact on transform

299 wards the realisation of solid-state quantum photonics with diamond.

300 n find immediate applications in topological photonics with synthetic dimensions, compact opto-electr