ライフサイエンスコーパス: optical device

1 al nanospectroscopic imaging based on a nano-optical device.

2 ace exposed to the observation system of the optical device.

3 erent oscillation phenomena in an integrated optical device.

4 r quantum information processing and quantum optical device.

5 mportant advances for rare-earth ion magneto-optical devices.

6 w the direct electronic control of nonlinear optical devices.

7 ultra-small, ultra-fast and power-efficient optical devices.

8 rious functionalities(2-7) in electronic and optical devices.

9 t, from solar cell coatings to self-cleaning optical devices.

10 n agents and quantum dots for electronic and optical devices.

11 nic sensing, spectroscopy, and plasmon-based optical devices.

12 or infrared metamaterials and transformation optical devices.

13 great potential for applications in quantum optical devices.

14 nsformation optics to achieve a new class of optical devices.

15 semiconductors into emerging electronics and optical devices.

16 l materials to create nanoelectronic or nano-optical devices.

17 ed from free space, making it functional for optical devices.

18 re hole-transport layer materials in electro-optical devices.

19 ties may lead to applications in sensors and optical devices.

20 of miniaturized electrical, nanofluidic and optical devices.

21 an increasing demand of compact and wearable optical devices.

22 elts with quantum effects for electronic and optical devices.

23 ities for miniaturization and integration of optical devices.

24 new generation of electronics, sensors, and optical devices.

25 ug delivery to catalysis to micrometer-scale optical devices.

26 tals promising for application in a range of optical devices.

27 e and efficient platform for next-generation optical devices.

28 ing next-generation nanophotonic and quantum optical devices.

29 ve A-QWPs and the ability to integrate other optical devices.

30 ion, typically leading to low-quality-factor optical devices.

31 al applications in temperature-resistant and optical devices.

32 al applications in temperature-resistant and optical devices.

33 a promising platform for developing advanced optical devices.

34 a design approach for a new class of compact optical devices.

35 ion and computing, optical displays, and all-optical devices.

36 orms for actively reconfigurable polaritonic optical devices.

37 g platform for next-generation MIR nonlinear optical devices.

38 s, ranging from molecular sensing to magneto-optical devices.

39 ional magnets in nonlinear and nonreciprocal optical devices.

40 alysis of light manipulation with individual optical devices.

41 e offer new approaches to implement advanced optical devices.

42 ed to create next generation agile microwave-optical devices.

43 reproducible manufacturing of advanced nano-optical devices.

44 nic states, offering potential for nonlinear optical devices.

45 films hold much promise for use in advanced optical devices.

46 ch in demand for the development of advanced optical devices.

47 imaging and in the design of many other new optical devices.

48 ocity fundamentally limit the integration of optical devices.

49 es for miniaturized high-performance magneto-optical devices.

50 veloping arbitrarily shaped multi-functional optical devices.

51 to enable compactness and miniaturisation of optical devices.

52 solar cells, and also toward applications as optical devices.

53 ts for flexible light emitter or on-chip all-optical devices.

54 ged to form lithium-niobate based integrated optical devices.

55 waveguide- or nanostructure-based nonlinear optical devices.

56 it attractive for flexible, biopolymer-based optical devices.

57 e applications with functionality switchable optical devices.

58 by gating which allows one to realize active optical devices.

59 ls brings the development of vast variety of optical devices.

60 he [2]catenane attractive for use in electro-optical devices.

61 efractive index gradients for transformation optical devices.

62 operations are difficult to perform with all-optical devices.

63 vity modulation, opening avenues for on-chip optical devices, advanced sensing, and beyond.

64 nufacturing processes and include only a few optical devices alongside simple circuits.

65 transducers, ranging from nanogravimetric to optical devices, also enabling the realization of multif

66 ability of materials for the applications in optical devices, analysis, biosensing, and fluorescence

67 integrated in a range of microelectronic or optical devices and applications.

68 o chemical and electrical stimuli in electro-optical devices and chemical sensors.

69 eving extreme light confinement and low-loss optical devices and enabling simplified device integrati

70 BSS approach that inherits the advantages of optical devices and fully fulfils its "blindness" aspect

71 ctrum illustrates their potential for use in optical devices and imaging applications.

72 rtant ultra thin film materials for sensors, optical devices and magnetic storage media.

73 troduce functionality into soft matter-based optical devices and may enable novel data storage scheme

74 r lasers combine the advantages of nonlinear optical devices and of semiconductor injection lasers, a

75 se QDs promising for applications in electro-optical devices and photochemical reactions.

76 ve technologies such as wavelength-selective optical devices and solar absorbers.

77 provide the possibility to develop synthetic optical devices and structures with enhanced functionali

78 further miniaturization of high-performance optical devices and systems.

79 Nonlinear optical devices and their implementation into modern nan

80 oton spatial conversion relying on a passive optical device, and (iii) single-photon transmission, wh

81 uides is a common requirement for integrated optical devices, and is typically achieved by end-fire o

82 le, organic light-emitting diodes, nonlinear optical devices, and organic solar cells.

83 ctromechanical systems, thin-film metrology, optical devices, and others.

84 in optical sensing, nonlinear optics, active optical devices, and quantum optics.

85 ultidimensional architectures for functional optical devices are covered and the next steps for this

86 However, applications of metasurfaces to optical devices are rare due to fabrication difficulties

87 ising technology platform for terahertz- to- optical devices as well as radio-frequency acoustic devi

88 ay offer a convenient template for producing optical devices based on biomimicry or direct dielectric

89 be considered when designing and fabricating optical devices based on GaAsBi alloys.

90 e various display as well as in non-display (optical devices based on LC) applications.

91 new acousto-optic platform can lead to novel optical devices based on nonlinear Brillouin processes a

92 the road towards tunable terahertz nonlinear optical devices based on topological insulator materials

93 r chip-scale, electrically tunable nonlinear optical devices based on two-dimensional semiconductors.

94 lation (SLIM) represent a novel class of ion optical devices based upon electrodes patterned on plana

95 s to sensors, actuators, electronic devices, optical devices, batteries, water harvesters, and soft r

96 use in catalyst, adsorption, polymer filler, optical devices, bio-imaging, drug delivery, and biomedi

97 The mammalian eye is a remarkable optical device, but its design is not perfect.

98 devise strategies through which miniaturized optical devices can be monolithically fabricated on ligh

99 We demonstrate an optical device capable of decomposing a beam into a Cart

100 , such as for energy conversion and storage, optical devices, catalysts, and various important nanoce

101 ential utility as semiconductors, catalysts, optical device components, and stimuli responsive networ

102 road maps to future innovations in nanoscale optical devices, components, and more intricate nanoscal

103 An optical device configuration allowing efficient electric

104 An optical device configuration allowing efficient electric

105 he traditional notion of what constitutes an optical device continues to evolve.

106 levant for the design of novel electronic or optical devices controllable by temperature.

107 olecules could prove useful in terahertz and optical devices controlled by pure spin currents.

108 les offer unparalleled potential for THz and optical devices controlled by pure spin currents: a low-

109 d benefit the next generation of intelligent optical device design.

110 er, it is challenging to scale the nonlinear optical devices down to the nanoscale dimension due to r

111 onolayer WS2 offers great promise for use in optical devices due to its direct bandgap and high photo

112 endence on incident polarization for several optical devices employing oriented nematic and chiral-ne

113 ual field is brought into view by the use of optical devices; eye movement-based therapies, in which

114 ted in the nanometer scale using a nonlinear optical device for the first time.

115 ucial for the development of next-generation optical devices for monitoring human CBF and brain funct

116 haviors, which can be exploited in patterned optical devices for next-generation UCNP applications.

117 Next-generation optical devices, however, demand nonmechanical, full and

118 se of electrostatic gates to define electron-optical devices in graphene.

119 he widespread adoption of plasmonic and nano-optical devices in real-life applications is the difficu

120 d that the time is ripe for considering many optical devices in the seismic and geophysical context.

121 hene-based materials, a basic ingredient for optical devices, induced by quantum confinement.

122 ic crystals that are particularly suited for optical device integration using a lithographic layer-by

123 However, the function of a nonlinear-optical device is typically determined during design and

124 Conventional design of all-optical devices is based on photon propagation and inter

125 Unique identification of optical devices is important for anti-counterfeiting.

126 mputational analysis and optimization of ion optical devices is still onerous, since the governing eq

127 In addition, metamaterial-based optical devices lend themselves to considerable miniatur

128 nhancing light-matter interaction in quantum optical devices, low-threshold lasers with minimal power

129 Hybridization of atoms with such thin optical devices may offer a material system enhancing th

130 , we demonstrate how standard electrical and optical device measurements obtained during an accelerat

131 In quantum optical devices, microcavities can coax atoms or quantum

132 The optical device mimics the design of the crystalline lens

133 ynthetic applications from photocatalysis to optical devices need to demonstrate increased ability to

134 atile paradigm for high-efficiency nonlinear optical devices, offering opportunities for advancements

135 ics provides a route to develop ultracompact optical devices on a chip by using extreme light concent

136 at replicate the functionality of integrated optical devices on a chip-scale.

137 rtifacts caused by uncertain factors such as optical devices or specimens, which severely affects the

138 ssipative two-photon regime in silicon-based optical devices, or possess small nonlinearities.

139 will be beneficial to develop active magneto-optical devices, orbital angular momentum based applicat

140 By using optical devices, originally developed for astronomy, who

141 tes the development of innovative compatible optical devices, particularly for use in lithography app

142 l quality as well as improved electrical and optical device performances.

143 of integration of nanochiral materials with optical device platforms remains acute(14-16).

144 Nonreciprocity and nonreciprocal optical devices play a vital role in modern photonic tec

145 linations is key to developing novel electro-optical devices, programmable origami, directed colloida

146 llows for a full sensitivity analysis of ion optical devices, providing a quantitative measure of the

147 hly desirable for numerous hybrid ultrasound-optical devices ranging from photoacoustic imaging trans

148 Numerous optical technologies and quantum optical devices rely on the controlled coupling of a loc

149 d then translating such insight into tunable optical devices remains challenging.

150 separation, and crystallization, as well as optical devices requiring specific polarized radiation a

151 ace structures, biomedical devices, adaptive optical devices, smart dry adhesives and fasteners.

152 akes it possible to dramatically miniaturize optical devices so as to integrate them into silicon chi

153 evelopment and study of solid-state electron-optical devices such as beam splitters and quantum point

154 ve been essential for the development of ion optical devices such as electron microscopes and mass sp

155 room-temperature 'prototype' PNLC-based all-optical devices such as optical diode, optical transisto

156 microwave circuits with planar acoustic and optical devices such as phononic and photonic crystals.

157 this design concept by showing how important optical devices such as quantum memory and optical filte

158 dings may pave the way for low-power quantum optical devices, surpassing quantum limits on position a

159 tion has the potential to revolutionize many optical device technologies.

160 rm demonstrates a path towards an integrated optical device that can be utilized for a wide variety o

161 nnections relies on the development of micro-optical devices that are integrated with the microelectr

162 hniques have opened up new possibilities for optical devices that are particularly suitable for these

163 ffer the possibility for fabricating tunable optical devices that are robust against disorder and def

164 Metal-dielectric multilayers are versatile optical devices that can be designed to combine the visi

165 Active planar optical devices that can dynamically manipulate light ar

166 ght on the nanoscale, enabling ultra-compact optical devices that exhibit strong light-matter interac

167 tegy for realizing a wide range of broadband optical devices that exploit the unique properties of me

168 ng resonators are refractive index-sensitive optical devices that feature good sensitivity and tremen

169 hough they can serve as the basis for unique optical devices that mould the flow of light in unconven

170 ing principles for the generalized design of optical devices that operate from the mid- to far-infrar

171 ept can be extensively utilized in designing optical devices that serve a wide range of applications

172 Optical biosensors are defined as portable optical devices that use biorecognition molecules to int

173 Flat optical devices thinner than a wavelength promise to rep

174 In parallel, the coherent excitation of optical devices through the tailored interference of mul

175 raction and harvesting of light in thin film optical devices to probing of molecular species and thei

176 ave recently been proven to provide superior optical devices to those on conventional c-plane substra

177 ical states of light and sound.Nonreciprocal optical devices traditionally rely on magnetic fields an

178 namics motivate the invention of a series of optical devices triggered by moisture, including anticou

179 new opportunities for advancing anisotropic optical devices used for future photonic integration, op

180 at large scale and at high yield, we design optical devices using a standard microelectronics foundr

181 Theoretical considerations show that all-optical devices using photonic crystal designs promise t

182 present a computer-aided design tool for ion optical devices using the adjoint variable method.

183 an unconventional route for engineering all-optical devices using the photon's internal degrees of f

184 p the tailored chemical design of nanocarbon optical devices, via gap tuning and side-chain functiona

185 pproach toward development of transformation optical devices where active all-optical control of the

186 onality regimes informs new design rules for optical devices where complex microstructures are involv

187 ctors and other metal or semiconductor based optical devices where resistive losses and power consump

188 cture thereby producing a broadband low-loss optical device with a desired response.

189 rier types to create electronic analogues of optical devices with both positive and negative indices

190 provide enormous promise for next-generation optical devices with excellent conversion efficiencies a

191 dates for use in stimulus-controllable chiro-optical devices with high optical efficiency, stable opt

192 ves the way towards practical flat nonlinear optical devices with large functional areas and massive

193 Metamaterials have the potential to create optical devices with new and diverse functionalities bas

194 itches to the toolbox for the development of optical devices with relaxation rates across multiple or

195 hitectures have enabled a panoply of tunable optical devices with the ability to perform useful funct

196 rest due to its potential for future magneto-optical devices with ultra-high sensitivity and ultra-fa

197 -are poised to form the platform for tunable optical devices with unprecedented functionality and per

198 ntrol opening the way for the development of optical devices with wide impact for on-chip photonics f

199 be processed directly by metamaterial-based optical devices without any additional coupling componen