ライフサイエンスコーパス: optics

1 ne of the most intensively studied topics in optics.

2 magnetic waves is a key objective in quantum optics.

3 ed applications in both linear and nonlinear optics.

4 ation modulation with and without postsample optics.

5 vel applications such as sensors and tunable optics.

6 s an important goal in all facets of quantum optics.

7 s of refractive and conventional diffractive optics.

8 erture lenses, color holograms, and wearable optics.

9 s and opens up new vistas in surface plasmon optics.

10 h-resolution proton tomography using magneto-optics.

11 ologies that are impossible with traditional optics.

12 s for a wide range of experiments in quantum optics.

13 lack material for paintings, camouflage, and optics.

14 nic standing waves by means of infrared nano-optics.

15 nts to modify the illumination and detection optics.

16 nstitutes one of the cornerstones of quantum optics.

17 ics, classical mechanics, and transformation optics.

18 pic of considerable interest in the field of optics.

19 dices with meta-materials and transformation optics.

20 ication potential in spintronics and magneto-optics.

21 ave radio frequencies devices and integrated optics.

22 udging the world through the eye with poorer optics.

23 spectroscopy, signal processing and quantum optics.

24 solutions down to 100 nm without using X-ray optics.

25 xample, in optical communication and quantum optics.

26 non-volatile computer memories, sensors and optics.

27 ys are caused by limitations in conventional optics.

28 ersion has always been an important topic in optics.

29 properties of media is crucial in nonlinear optics.

30 ty which have opened up new avenues for flat optics.

31 ematical operation which arises naturally in optics.

32 ve flat waveplates, and adaptive diffraction optics.

33 d with the application of soft components in optics.

34 ral retina of human observers using adaptive optics.

35 etection with standard wide-field microscope optics.

36 solitary wave propagation in nonlinear fibre optics.

37 imaging, optical communications and quantum optics.

38 found applications in classical and quantum optics.

39 effect, presenting a unique tool for quantum optics.

40 y of planar-fabricated dielectric integrated optics.

41 devices that couple ionics, electronics, and optics.

42 optical properties is crucial for nonlinear optics.

43 ure fundamental and applied research in nano-optics.

44 one of the central organizing principles of optics.

45 luation of forthcoming commercial absorbance optics.

46 and cannot be adjusted using standard fiber optics.

47 des that adapt to the user via computational optics.

48 pen up new perspectives on practical tunable optics.

49 fields from protein spectroscopy to quantum optics.

50 review recent work on incorporating adaptive optics, a technology originally applied in astronomical

51 and mini-microscopy, relying on conventional optics--a process we refer to as Expansion Mini-Microsco

52 Baerveldt 350, Baerveldt 250 [Abbott Medical Optics, Abbott Park, IL], or Ahmed FP7 [New World Medica

53 Freeform optics aims to expand the toolkit of optical elements by

54 a = lambdaprobe/2n) and not on the NA of the optics allowing sub-optical wavelength acoustic sectioni

55 nipulation and placement of components using optics alone promises a route towards increasingly dynam

56 n transverse ultrasound using Abbott Medical Optics' (AMO) WhiteStar Signature Pro with the Ellips FX

57 ture in influencing floral light capture and optics, analysing colour, gloss and polarization effects

58 n put into the field of integrated nonlinear optics and a medium with large nonlinearity is desirable

59 ultrahigh vacuum environment of the electron optics and detector.

60 herent diffractive imaging, non-linear x-ray optics and high field physics, and single molecule imagi

61 ay open new research directions in nonlinear optics and high-energy-density science, compact plasma-b

62 (SPs) is of particular interest in nonlinear optics and highly integrated plasmonic circuitry.

63 eral resolution is dependent on the delivery optics and is limited by ocular aberrations.

64 systems but also broadly for few-mode fiber optics and its applications in amplifiers, lasers, and s

65 ndamental role in the development of quantum optics and its applications.

66 Recent development in instrumentation, optics and manufacturing approaches has facilitated the

67 ng blocks for next-generation reconfigurable optics and metasurfaces.

68 spirit of optofluidics technology-fusion of optics and microfluidics for advanced functionalities.

69 ven an intermediate level of experience with optics and microscopy, for instance graduate-level famil

70 tonics, including optical sensing, nonlinear optics and nanolasers, where the broad resonant modes ca

71 Chiral-selective non-linear optics and optoelectronic signal generation are demonstr

72 emitters (SQEs) are at the heart of quantum optics and photonic quantum-information technologies.

73 scientific disciplines ranging from quantum optics and photovoltaics to metamaterials and medicine.

74 s an additional degree of freedom for modern optics and practical applications.

75 in areas from imaging and sensing to quantum optics and quantum information science.

76 ial resolution that is a convolution of beam optics and sampling frequency.

77 and optimizations of mechanics, electronics, optics and software programs that are central to the rea

78 ave opened new avenues in photonics, quantum optics and solar energy harvesting.

79 of elasto-optic metamaterials that combines optics and solid mechanics.

80 iguing physics and applications in ultrafast optics and supercontinuum generation.

81 he analogy between this problem in classical optics and that of tomographically reconstructing the de

82 combination of wavefront sensorless adaptive optics and the use of dual deformable transmissive optic

83 th that puts stringent requirements on X-ray optics and their metrology.

84 , the method does not require the use of any optics and thus can be used to monitor the location of u

85 Jones formalism was extended to nonlinear optics and was used to bridge the experimental observabl

86 of physics, such as atomic physics, quantum optics and, more recent, cavity optomechanics.

87 rating other components, such as electrodes, optics, and additional channels.

88 in catalysis, biomedicine, sensing, imaging, optics, and energy conversion.

89 cated experimental geometry, preparation and optics, and is limited by low data-acquisition efficienc

90 metallic nanocrystals in terms of catalysis, optics, and magnetism and conclude the Review by highlig

91 es, yet additional expertise, more elaborate optics, and phase-locked detectors are needed for ultras

92 omized between bilateral Crystalens Advanced Optics (AO) (Bausch + Lomb Surgical, Aliso Viejo, Califo

93 allic nanowires for plasmonics and nonlinear optics applications, as well as the integration of funct

94 ible displays, chemical sensors and electron optics applications.

95 Here we present transformation optics applied to thermoelectric phenomena, where therma

96 The geometrical optics approximation is used to provide a description of

97 rum and a disposable microfluidic device; no optics are involved in the implementation.

98 line-focused laser and wide-field collection optics are used to excite and collect the fluorescence e

99 Antennas, from radiofrequencies to optics, are bound to transmit and receive signals equall

100 dination polymers in the field of non-linear optics as an example, we consider synthetic approaches u

101 rganic frameworks in the field of non-linear optics as chemically obtained metamaterials of the futur

102 Transformation optics, as the underlying mathematical tool, has proven

103 eyes that followed the preoperative adaptive optics assessment, the mean PAV increase at near was sig

104 cope (NST) equipped with high order adaptive optics at Big Bear Solar Observatory (BBSO).

105 m parametric mode sorting based on nonlinear optics at the edge of phase matching to improve the trad

106 tion of novel actively tunable, yet low-loss optics at the nanoscale.

107 Nonlinear optics based on bulk materials is the current technique

108 results pave the way for realizing electron optics based on graphene p-n junctions.

109 Computer simulations of the fiber optics based on the finite element method (FEM) were con

110 e of the most distinctive aspects of quantum optics, being the trigger of multiple nonclassical pheno

111 ations of inorganic nanoparticle colloids in optics, biology, and energy, their surface chemistry has

112 ation not only enriches the diffraction-free optics, but also has potential applications for photolit

113 Adaptive optics by direct imaging of the wavefront distortions of

114 They are poised to revolutionize optics by enabling complex low-cost systems where multip

115 lity of this approach for integrated quantum optics by interfering and detecting photon pairs directl

116 obtained using a flood-illumination adaptive optics camera.

117 Adaptive optics can correct for optical aberrations.

118 crucial for a range of applications spanning optics, catalysis, electronics and energy.

119 cro-lasers are key ingredients in non-linear optics, communication, sensing and low-threshold solar-p

120 ysical magnification, coupled to inexpensive optics, could together match the performance of high-end

121 t can be revealed from such electrochemistry/optics coupling.

122 rating organic nanorobots to inorganic fiber optics creates a hybrid system that we demonstrate as a

123 e massive size of the silicon single-crystal optics currently used.

124 ast or the use of high magnification upright optics difficult.

125 This device relies on magnetic optics, distinguishing it from most published proton ima

126 cial for the development of new paradigms in optics, electronics and spintronics.

127 -derived assemblies and materials for use in optics, electronics, optoelectronics, photonics, magneti

128 by means of monolithically integrated micro-optics elements, continuous enzymatic reactions can be s

129 of soft photonics and biologically inspired optics, emphasizes the ties between the two fields, and

130 ical operators and photonic elements in wave optics enables quantitative analysis of light manipulati

131 challenges in applied nonlinear and quantum optics, enabling manipulation and interaction of quantum

132 engineering, architecture, food processing, optics, energy technology, dentistry, drug delivery, and

133 ng center experts, retinal histologists, and optics engineers.

134 blur encountered through the eye with better optics, even when judging the world through the eye with

135 etection is a requisite technique in quantum-optics experiments in both the optical and the microwave

136 -xTe2 a promising platform for transport and optics experiments on Weyl semimetals.

137 rend of moving complicated table-top quantum optics experiments onto the fully integrated CMOS-compat

138 Nonlinear optics experiments performed in a solution of graphene n

139 paves the way to a new generation of quantum optics experiments with two-dimensional semiconductors.

140 ntations have been mainly limited to quantum optics experiments.

141 and it is at the core of many famous quantum optics experiments.

142 oned challenges, as indicated in recent bulk-optics experiments.

143 absorption spectrometer making use of fiber optics for delivery and return of low intensity diode la

144 ility for future dynamic and miniature X-ray optics for focusing, wavefront manipulation, multicolour

145 lementary information, fabricating dedicated optics for high energies still remain a challenge.

146 We report development of micro-focusing optics for high-energy x-rays by combining a sagittally

147 ed here provides the path to efficient X-ray optics for imaging at 1 nm resolution.

148 interface between the torch and the entrance optics for inductively coupled plasma optical emission s

149 r applications, which span from microwave to optics for the control of surface plasmon polaritons (SP

150 y the Wigner model in the 10(-14) s range in optics had to await femtosecond lasers to be detected wi

151 The introduction of hardware-based adaptive optics (HAO) has pushed the limits of optical imaging, e

152 It is to this end that transformation optics has been developed, exploiting Faraday's picture

153 Integrated quantum optics has the potential to markedly reduce the footprin

154 Nonlinear optics has traditionally focused on frequency conversion

155 ligned magnetic dipoles, their equivalent in optics have not been fully explored so far.

156 ns for renewable energy, biosensing, quantum optics, high-density magnetic data storage, and nanoscal

157 disappearance of the cone mosaic on adaptive optics images.

158 Adaptive-optics imaging identified a small, focal hyporeflective

159 Conclusions and Relevance: Adaptive optics imaging may provide high-resolution en face image

160 Adaptive-optics imaging previously demonstrated a sparse mosaic o

161 rteriovenous overlap were imaged by adaptive optics imaging.

162 However, bulk optics implementations suffer from the lack of integrati

163 Compared with conventional optical methods, optics implemented on microfluidic chips provide small,

164 vokes us to rethink the established rules of optics in both the linear and nonlinear regimes.

165 omography scan can be correlated to adaptive optics in terms of photoreceptor density.

166 bserving delicate effects typical of quantum optics in the context of strongly correlated systems.

167 tforms for dynamic beam shaping and adaptive optics in the crucial infrared wavelength range.

168 as atomic physics, plasma physics, nonlinear optics in the x-ray range, and protein crystallography.

169 Removing the need to raster the optics in two directions significantly reduces the acqui

170 ors have inspired analogues in photonics and optics, in which one-way edge propagation in topological

171 abled (150-kHz IntraLase iFS; Abbott Medical Optics Inc) wavefront-guided ablation.

172 ecnis-1 or three-piece AR40E, Abbott Medical Optics Inc.) had been previously placed.

173 A Signature (Abbott Medical Optics, Inc) phacoemulsification machine was used in per

174 ) or a Baerveldt-350 implant (Abbott Medical Optics, Inc, Santa Ana, CA) using a standardized surgica

175 he Catalys femtosecond laser (Abbott Medical Optics, Inc., Santa Ana, CA).

176 Previous research on transformation optics indicated that such absorption cannot easily be i

177 by preoperative assessment using an adaptive optics instrument.

178 Optics-integrated microfluidic systems can significantly

179 e miniaturization of conventional refractive optics into planar structures.

180 through photonic nanostructures in coherent optics involves the utilization of a nonlinear optical m

181 Parity-time (PT)-symmetry in optics is a condition whereby the real and imaginary par

182 hort pulse widths using methods of nonlinear optics is a well-established technology of modern laser

183 ndous developments in AM, the 3D printing of optics is lagging due to the limits in materials and tig

184 A central goal of quantum optics is to generate large interactions between single

185 This means that by using adaptive optics it may be possible to eliminate the impact of sel

186 ith the Raindrop Near Vision Inlay (ReVision Optics, Lake Forest, CA); 340 eyes underwent the 1-year

187 In linear optics, light fields do not mutually interact in a mediu

188 We propose a new precision additive freeform optics manufacturing (AFOM) method using an pulsed infra

189 ndamental phenomenon in electromagnetics and optics, material absorption has been extensively investi

190 We used adaptive optics microstimulation to measure psychophysical detect

191 tions for PT symmetric physics in acoustics, optics, microwaves and electronics, which are essential

192 The method utilizes a wave optics model to account for the dominant diffraction eff

193 The optics module containing the laser has dimensions 60 x 4

194 We developed multi-pupil adaptive optics (MPAO), which enables simultaneous wavefront corr

195 ducing the laser power required for adaptive optics multiphoton imaging, and for facilitating integra

196 readily available building blocks of quantum optics, namely coherent states, single photons, beam spl

197 ental implications for classical and quantum optics, nanoscale metamaterials provide a platform for d

198 unique properties in the field of non-linear optics (NLO) over the past three years.

199 Despite such interest in nano-optics, no experimental evidence of Fano interference wa

200 ff has no correspondence in either nonlinear optics of a normal gas or a phonon-based condensed matte

201 e can improve human vision by correcting the optics of our lenses [1-3].

202 rogressing mid- and long-wavelength-infrared optics of the atmosphere.

203 s for developing nanoscale nonlinear quantum optics on the single-molecule level.

204 afforded by recent advances in computational optics open up the possibility of creating a computing p

205 In the field of biomedical optics, optical scattering has traditionally limited the

206 s a great potential for impact on integrated optics, optical sensors, and photovoltaic devices.

207 les with large lattice mismatches for use in optics, optoelectronics, catalysis, or bioimaging.

208 al and ancillary testing, including adaptive optics, outcomes in autoimmune retinopathy (AIR) patient

209 nd experiment how frequency domain nonlinear optics overcomes the shortcomings arising from the convo

210 The field of transformation optics owes a lot of its fame to the concept of cloaking

211 small differences with standard fluorescence optics, particularly in situations where sample volume i

212 s possess huge potential for applications in optics, photonics, adaptive materials, nanotechnology, e

213 nlinear systems including superfluids, fibre optics, plasmas and Bose-Einstein condensates.

214 ties will catalyze studies involving quantum optics, plasmon laser physics, strong coupling, and nonl

215 ing polarization rotation with no postsample optics, polarization-in polarization-out measurement, an

216 Scaling up linear-optics quantum computing will require multi-photon gates

217 xperiment for its demonstration using linear optics quantum gates.

218 In atomic and molecular optics, radiation pressure can be used to trap or cool a

219 vival or loss, based on analysis of adaptive optics retinal images, was valuable to monitor disease p

220 r Tecnis +4D Multifocal (MF) (Abbott Medical Optics, Santa Ana, California, USA) IOL.

221 this report, we present sensorless adaptive optics (SAO) using low-coherence interferometric detecti

222 Transformation optics says what has to be done to place the lines of fo

223 Imaging with an adaptive optics scanning laser ophthalmoscope (AOSLO) showed depl

224 aculae were imaged using a research adaptive optics scanning laser ophthalmoscope.

225 In this study, we used adaptive optics scanning laser ophthalmoscopy (AO-SLO) to examine

226 t of patients was also imaged using adaptive optics scanning laser ophthalmoscopy (AO-SLO).

227 e tomography angiography (OCTA) and adaptive optics scanning laser ophthalmoscopy (AOSLO).

228 Imaging with an adaptive optics scanning light ophthalmoscope (AOSLO) enables dir

229 h imaging of the living retina with adaptive optics scanning light ophthalmoscopy (AOSLO) provides mi

230 retinal pigment epithelial lesions, adaptive optics scanning light ophthalmoscopy reveals increased c

231 Conformal transformation optics scheme leads to cloaks that possess isotopic medi

232 Together with the fitted phase plate the optics shows diffraction-limited performance, generating

233 ng as an approach to extend the DIY theme to optics, specifically the table-top fabrication of planar

234 ent branches of physics, including nonlinear optics, spintronics and plasmonics.

235 ul for advanced applications in polarization optics, stereochemistry and spintronics.

236 al metamaterials offers potential for active optics such as all-optical switching and light modulatio

237 d have become important in various fields of optics, such as quantum and classical information scienc

238 However, diffractive optics suffers from large chromatic aberrations due to t

239 under ordinary light source without complex optics system, giving rise to practical applications inc

240 oved by the use of state-of-the-art adaptive optics systems.

241 ble light (<1mWcm(-2)) with the aid of fiber optics technology.

242 Using adaptive optics that allows accurate measurement of bouton activi

243 esent several fundamental problems in modern optics that are of great importance for the development

244 use interference filters and interferometric optics that limit their photon efficiency, resolution an

245 In optics, the ability to measure individual quanta of ligh

246 In optics, the abrupt nature of the phase transitions that

247 nse laser light is intrinsic to relativistic optics, the development of compact laser-driven particle

248 Without complex optics, the device negated large signal drifts (1/f nois

249 Oculus, Wetzlar, Germany) and the Cassini (i-Optics, The Hague, Netherlands).

250 Optics then validates in situ the concept of EC nanoimpa

251 % reflectivity, and as a dynamic diffractive optics they can generate nanosecond time windows with ov

252 We demonstrate that, as X-ray reflective optics they can maintain the wavefront properties with n

253 scheme can be applied to any other focusing optics, thus solving the X-ray optical problem at synchr

254 a means to extend the domain of geometrical optics to a deep sub-wavelength scale.

255 This technique opens up nonlinear optics to a regime of relaxed phase matching, with the p

256 The adaptation of freeform optics to a sub-wavelength metasurface platform allows f

257 We show integrated optics to be suitable for simulating specific target Ham

258 To test this, we used adaptive optics to control and manipulate the blur projected on e

259 ploit the inherent dispersion in diffractive optics to demonstrate planar chromatic-aberration-correc

260 , spectral demultiplexers and reconfigurable optics to generate a path-entangled two-qubit state and

261 ) on an ultramicroelectrode are coupled with optics to identify chemical processes at the level of in

262 first successful demonstration of using DVD optics to image DNA molecules with high-speed AFM.

263 ity functional theory and high field magneto-optics to investigate the metal chalcogenide InSe, a rec

264 y scattered images by: (i) marrying adaptive optics to optical coherence tomography to avoid optical

265 frequency demultiplexers and reconfigurable optics to perform both quantum state tomography and the

266 ectrode ion funnels or more conventional ion optics to SLIM can involve discontinuities in electric f

267 er beam enables the application of nonlinear optics to solar energy conversion and storage.

268 rd manner by fastening the laser and guiding optics to the instrument chassis itself, making alignmen

269 ron radiation sources demands improved X-ray optics to utilise their capability for imaging and probi

270 The Pacific Biosciences sequencer uses optics to view a polymerase and its interaction with a s

271 Both concepts of Transformation Optics (TO) and metamaterials have been regarded as one

272 Here we calculate PTIR spectra via thin-film optics, to identify subtle changes (band shifts, deviati

273 uding low-intensity nonlinear transformation optics, topological photonics, and the broader area of s

274 and theranostics, optical sensing, nonlinear optics, ultrahigh-density data storage, as well as plasm

275 ion) was monitored with backscattering fiber optics under strongly attenuated laser power (7 mW).

276 Linear optics underpins fundamental tests of quantum mechanics

277 s, which benefits size reduction and minimal optics used.

278 hodology for designing analogues of freeform optics using a silicon nitride based metasurface platfor

279 Phonon optics using external control broadens the spectrum of p

280 etector, including mirror source and imaging optics, UV sensitive acquisition modes and revised data

281 ource of spin-orbit coupling to non-paraxial optics vortices.

282 eactivation beams generated with diffractive optics was combined with a serpentine microfluidic chann

283 ng of a stainless steel capillary and DC ion optics was designed to conduct ions into the mass spectr

284 al alteration of the cone mosaic on adaptive optics was performed.

285 nstrate a macroscale (>35 mm) transformation-optics wave bender (293 mm(2)) and Luneburg lens (855 mm

286 Traditional approaches to adaptive optics wavefront correction are not effective in thick o

287 With linear optics, we design a W-state analyzer in order to disting

288 In the context of classical optics, we implement discrete fractional Fourier transfo

289 re, inspired by the method of transformation optics, we propose and demonstrate a transformation medi

290 applications of such structures, focusing on optics, wetting, sensing, catalysis, and electrodes.

291 spatial shifts were only observed in 1947 in optics, whereas the time delay values predicted by the W

292 New functionalities in nonlinear optics will require systems with giant optical nonlinear

293 re one of the most important tools in modern optics with a broad spectrum of applications in, for exa

294 can be overcome by replacing interferometric optics with a two-dimensional absorptive filter array co

295 into nonlinear quantum effects in microwave optics with artificial atoms.

296 c assessments are performed using free-space optics with bulky optical components.

297 ple are accomplished by combining line focus optics with sheath-flow SERS detection.

298 ed to demonstrate on-chip effects of quantum optics with single atoms in the microwave range.

299 teStar Signature Pro machine (Abbott Medical Optics) with the Ellips FX handpiece and a 0.9-mm bent D

300 alignment afforded by the integration of the optics within the trap chip, this approach presents a pa