ライフサイエンスコーパス: optical

1 Here, we show that the optical 2D photon echo spectra of this complex at ambien

2 t-graphene interactions by investigating the optical absorption in the SLG, the density of optical st

3 ptical sample, compared to any future direct optical absorption measurement using classical light.

4 This illustrates how optical absorption methods have become a competitive alt

5 d y >/= 0.6) is studied experimentally using optical absorption, photomodulated transmission, contact

6 20 animals at the favorable orientation for optical access needed for precise laser surgery and high

7 nd can therefore avoid the highly dispersive optical activity resulting from resonances.

8 As a result, fast animals often exhibit optical adaptations comparable to nocturnal animals, but

9 Despite these changes in optical aerosol characteristics, increases in dried aero

10 Afterglow optical agents, which emit light long after cessation of

11 Optical analog computing offers high-throughput low-powe

12 Ion-selective optodes (ISOs), the optical analog of ion-selective electrodes, have played

13 This technique, previously identified as the optical analogue of the electrical Hall effect, permits

14 The optical and electronic properties of semiconducting mate

15 gen-vacancy (NV) diamond quantum sensor with optical and microwave waveguide delivery enables thermom

16 w family of tunable materials with excellent optical and photochemical properties for exploitation in

17 ition camera system as well as Arduino-based optical and thermal control circuits.

18 tracked using a combination of gravimetric, optical, and electrical sensing modes, enabling accurate

19 ysis of a concentric circular ring plasmonic optical antenna (POA) array using a simple lumped couple

20 zation manipulations are required for varied optical applications.

21 e-matter interactions for radiofrequency and optical applications.

22 curvature leads to a radial variation of the optical axis along the plane of the film.

23 scence intensity profiles measured along the optical axis of human eye lenses with age-related nuclea

24 wisted molecular framework, NITI shows a low optical bandgap of 1.49 eV in thin film and a high molar

25 n lifetime is consistent with their relative optical bandgap.

26 ich serve as bridges connecting conventional optical beam and structured light.

27 nd propagation, and demonstrate a variety of optical beam structures emerging upon vortex beam propag

28 ilbert-space analyzer' capable of projecting optical beams onto any modal basis.

29 n of postoperative refraction using a single optical biometry device.

30 d spectroscopy (fNIRS) is a field-deployable optical brain monitoring technology that provides a dire

31 Single-vesicle optical (by TIRF microscopy) and biophysical measurement

32 By placing cold atoms in optical cavities and inducing strong coupling between li

33 by using two laser beams far detuned from an optical cavity resonance, efficient state transfer is po

34 ned across several longitudinal modes of the optical cavity.

35 covery that the microwave dielectric and the optical characteristics of an EC cell can be engineered

36 ver macroscopic length scales accessible for optical characterization.

37 for subwavelength optical components in nano-optical circuits and metasurfaces.

38 Optical clearing methods can facilitate deep optical ima

39 al keratoplasty (DSAEK) using intraoperative optical coherence tomography (iOCT) in the Prospective I

40 crimal punctum with infrared photographs and optical coherence tomography (OCT) and to identify chara

41 cup-to-disc ratio (VCDR, HCDR) by an updated optical coherence tomography (OCT) Bruch membrane openin

42 In recent years, optical coherence tomography (OCT) has become a powerful

43 ork for the estimation of visual acuity from optical coherence tomography (OCT) images of patients wi

44 or images, fluorescein angiography (FA), and optical coherence tomography (OCT) in eyes with NVAMD th

45 Assess the role of handheld optical coherence tomography (OCT) in guiding management

46 Optical coherence tomography (OCT) is a powerful biomedi

47 To assess the ability of swept-source (SS) optical coherence tomography (OCT) of the anterior segme

48 Retinal fluorescein angiography and optical coherence tomography (OCT) revealed the presence

49 Fourier-domain optical coherence tomography (OCT) was used to map the t

50 Optical coherence tomography (OCT) was used to visualise

51 on using scotopic electroretinography (ERG), optical coherence tomography (OCT), and immunohistochemi

52 ), fundus fluorescein angiography (FFA), and optical coherence tomography (OCT).

53 rom the same tissue while being imaged under Optical Coherence Tomography (OCT).

54 hickness as measured by spectral-domain (SD) optical coherence tomography (OCT).

55 e of serous retinal detachments confirmed by optical coherence tomography (OCT).

56 ve and Perioperative Ophthalmic Imaging with Optical Coherence Tomography (PIONEER) study with postop

57 course of recovery by serial spectral-domain optical coherence tomography (SD OCT) and the correlatio

58 orescein angiography (UWFA), spectral-domain optical coherence tomography (SD-OCT), and optical coher

59 hs, fluorescein angiography, spectral-domain optical coherence tomography (SD-OCT), best-corrected vi

60 te AMD from 68 patients with spectral-domain optical coherence tomography (SDOCT) imaging.

61 cence, blue reflectance, and spectral-domain optical coherence tomography (SDOCT).

62 (Zeiss) axial length measurements and fundus optical coherence tomography (Zeiss).

63 To describe the optical coherence tomography angiograhy (OCTA) of drusen

64 radial peripapillary capillary network with optical coherence tomography angiography (angio-OCT) in

65 n optical coherence tomography (SD-OCT), and optical coherence tomography angiography (OCT-A) detect

66 lliform macular dystrophy (BVMD) by means of optical coherence tomography angiography (OCT-A).

67 ibing multimodal imaging findings, including optical coherence tomography angiography (OCT-A).

68 Optical coherence tomography angiography (OCTA) allows v

69 ral-domain optical coherence tomography, and optical coherence tomography angiography.

70 ent visual acuity was worsening with similar optical coherence tomography examination.

71 the prevalence of thin cap fibro-atheroma by optical coherence tomography in DM and non-DM patients.

72 went choroidal imaging using spectral-domain optical coherence tomography with enhanced depth imaging

73 m cell-derived epithelial cultures and micro-optical coherence tomography, a new imaging modality tha

74 cyanine green angiographies, spectral-domain optical coherence tomography, and optical coherence tomo

75 also after enucleation using spectral domain optical coherence tomography.

76 titative neuroimaging with 3-T brain MRI and optical coherence tomography.

77 Fs) have been recently employed in classical optical communication to increase the data transmission

78 Conventional optical components are limited to size scales much large

79 anoantennas is of interest for subwavelength optical components in nano-optical circuits and metasurf

80 We determine the optical conductivity of LMH and find metallic hydrogen's

81 oupling depends extremely sensitively on the optical confinement and the orientation of electronic di

82 uiding counterpart, while maintaining strong optical confinement at telecommunication wavelengths.

83 PUT takes advantage of the high native optical contrast among biological tissues and can treat

84 These data offer the first example of optical control of analgesia in vivo using a photocaged

85 A generalizable method for optical control of kinases would enable fine spatiotempo

86 e findings provide a route to the systematic optical control of the gigahertz response of metallic na

87 Survey 2017a (SSS17a) was discovered as the optical counterpart of the binary neutron star gravitati

88 radio bursts have similarly faint radio and optical counterparts, our findings imply that direct sub

89 the lens centre in accord with the increased optical density in the lens nucleolus.

90 oprotanomaly, suggesting decreased effective optical density of the cone photopigments.

91 cillus reuteri C1 strain as evidenced by the optical density of the culture broth.

92 erference from the nanomaterial when reading optical density, and the residue left from the exposure

93 a random forest model incorporating aerosol optical depth (AOD) data, meteorological fields, and lan

94 ed voltage indicators have shown promise for optical detection of voltage transients, many indicators

95 To extend the applicability of such optical detection schemes, we herein report the developm

96 mplementary metal-oxide-semiconductor (CMOS) optical detection system for a rapid and highly-sensitiv

97 sensing platform for real-time detection and optical determination of intracellular ions.

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

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

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

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

102 f cell membrane voltage responses beyond the optical diffusion limit.

103 hoton sources for next generation flat panel optical display devices, bio-medical applications, lumin

104 ayer tungsten disulfide (WS2) under infrared optical driving.

105 semimetal that hosts unique chiral electron-optical effects due to its honeycomb crystalline lattice

106 superposition of orthogonal fields, such as optical eigenmodes.

107 Next we deliberate on the mechanical, optical, electrical, and electromechanical properties, w

108 ronics probe station capable of simultaneous optical-electrical excitation and simultaneous optical-e

109 tical-electrical excitation and simultaneous optical-electrical response measurement has been designe

110 s offers to biosensing platforms exceptional optical, electronic and magnetic properties.

111 van der Waals heterostructures with tunable optical-electronic-magnetic coupling properties are prom

112 radable, and biofunctionalizable diffractive optical elements (DOEs) using silk proteins as the build

113 Optical elements that convert the spin angular momentum

114 design of novel magnetic resonance shift and optical emission probes that are sensitive to the local

115 was performed by inductively coupled plasma optical emission spectrometry and the digestion efficien

116 phase by means of inductively coupled plasma optical emission spectroscopy (ICP-OES).

117 ked rice using an inductively coupled plasma-optical emission spectroscopy.

118 The use of optical excitation would allow for overcoming all these

119 uch innovations for their ability to support optical excitations persisting for nearly 1 billion cycl

120 itude fewer spins and which require resonant optical excitations to spin-polarize the ensemble.

121 s in the ITO counter-electrode, altering the optical extinction response.

122 al data are supported by a model to show how optical feedback affects the laser frequency as it is sc

123 can trap light and function as high-quality optical feedback for microscale lasers and nanolasers.

124 tion methods, thanks to the light guiding in optical fibers and small distance between the fiber tips

125 Using optical fibers with enhanced Rayleigh backscattering pro

126 We demonstrate that optical fibers with tapered tips can be used to illumina

127 e show that localized states of a disordered optical fibre are single mode: the transmission channels

128 of a quantum repeater, akin to repeaters in optical fibre networks.

129 along a 10 km length of normally dispersive optical fibre.

130 oadening when propagating through lengths of optical fibre.

131 g padeliporfin intravenously over 10 min and optical fibres inserted into the prostate to cover the d

132 on a flexible fibre bundle of six multimode optical fibres, each terminated with a distal polariser

133 occurs for molecules residing in high local optical fields of plasmonic nanostructures.

134 n), variable linear polarization of a prompt optical flash that accompanied the extremely energetic a

135 iving cells as an alternative to traditional optical fluorescence.

136 riven vibrations and perturb its motion with optical force fluctuations at a level dictated by the He

137 ttern of Ultimaster drug-eluting stent using optical frequency domain imaging.

138 , CaMPARI enables network-wide, tunable, all-optical functional circuit mapping that captures supra-

139 However, their applications as optical-gain media are complicated by a non-unity degene

140 The ability to image nuclei tagged with MR/Optical gene markers may also find wide use in cell line

141 lique incidence thin film deposition onto an optical grating substrate, it is possible to increase th

142 This conventional picture of optical heating is supplemented by radiative cooling, wh

143 by circularly polarized light, so-called all-optical helicity dependent switching, has renewed intere

144 mimNTf2 liquid (870 +/- 20 ps) measured with optical heterodyne-detected optical Kerr effect (OHD-OKE

145 place aversion and a reduction in the above optical ICSS in VgluT2-cre control mice, but not in Vglu

146 optoacoustic imaging device that fuses laser optical imaging (OA) with grayscale ultrasonography (US)

147 We used voltage-sensitive dye optical imaging and somatosensory and motor behavioral t

148 We developed molecular assays and portable optical imaging designs that permit on-site diagnostics

149 Optical clearing methods can facilitate deep optical imaging in biological tissue by reducing light s

150 Optical imaging is uniquely suited to assess organoid fu

151 Three-dimensional (3D) optical imaging of whole biological organs with microsco

152 croneedle penetration following staining and optical imaging.

153 termed memory by engineered mutagenesis with optical in situ readout (MEMOIR), is based on a set of b

154 We demonstrate a highly efficient optical interface between Si3N4 waveguides and single-qu

155 The large dilution ensured minimal optical interference from the nanomaterial when reading

156 ilities include wireless pharmacological and optical intervention for dissecting neural circuitry dur

157 hese approaches have yet demonstrated linear optical isolation with ideal characteristics over a micr

158 Low-loss optical isolators and circulators are critical nonrecipr

159 s) measured with optical heterodyne-detected optical Kerr effect (OHD-OKE) experiments.

160 We have applied far-infrared and ultrafast optical Kerr effect spectroscopies on carefully selected

161 Strontium optical lattice clocks have the potential to simultaneou

162 sults lay the groundwork for using fermionic optical lattice clocks to probe new phases of matter.

163 The atoms are trapped in a two-dimensional optical lattice that enables cycles of compression to in

164 P) ensures the precise adjustment of the AFM optical lever system, a prerequisite for all kinds of fo

165 Here, we utilize an optical light transmission method to continuously monito

166 li, such as temperature, magnetic field, and optical light.

167 Optical manipulation and label-free characterization of

168 Optical mapping is a technique for capturing fluorescent

169 Optical mapping of perfused hearts confirmed slowed cond

170 ule real-time sequencing and high-resolution optical mapping.

171 identifying structural variations (SVs) from optical maps.

172 to coordinate large metal ions; as nonlinear optical materials, MRI contrasting agents, and sensitize

173 igh-resolution mass spectrometry, as well as optical measurements revealed that the chemical composit

174 The electrical and optical measurements, in combination with density functi

175 twin domains are observed using a polarized optical microscope.

176 icult to achieve due to the lack of adequate optical microscopic resolution to study human synapses.

177 lized by scattering-type scanning near-field optical microscopy (s-SNOM), the real-space imaging of s

178 We present a combination of optical microscopy and AFM-IR imaging to characterize OM

179 cal near field that is inaccessible to other optical microscopy methods can be obtained.

180 erovskite crystals is scrutinized by in situ optical microscopy tracking to understand the crystalliz

181 es (h degrees , C *, DeltaE) microstructure (optical microscopy), and ascorbic acid (AA) degradation

182 substrate, their locations determined using optical microscopy, and the cell locations used to guide

183 aterial subjected to an in-depth analysis by optical microscopy, calorimetry and small angle X-ray sc

184 nificant gain in resolution over traditional optical microscopy, enabling the localization of individ

185 The millivolt-scale optical modulation is attributed to a new modulation mec

186 are suggested to also be responsible for the optical modulation of naturally occurring bacteriochloro

187 ll-plasmonic 116-gigabits per second electro-optical modulator in which all the elements-the vertical

188 In this work, we apply an optical nano-imaging technique to determine the anisotro

189 ntly, molecular structure information in the optical near field that is inaccessible to other optical

190 put-output transfer function requires strong optical nonlinearity, e.g. self-phase modulation, which,

191 r nearly 1 billion cycles, and for their low optical nonlinearity.

192 ute values of the elastic moduli from purely optical observations.

193 hysiological function, allowing simultaneous optical pacing and Vm mapping.

194 le pulse synthesiser based on a mid-infrared optical parametric amplifier and its application to high

195 Optical parametric gain of 42.5 dB, as well as cascaded

196 rption edge, representing one of the largest optical parametric gains to date on a CMOS platform.

197 gnetic fields are accrued gradually along an optical path.

198 manipulate the LDOS via field effect-induced optical permittivity modulation of an ultrathin titanium

199 ing, real-time image analysis, and automated optical perturbations.

200 ss based microfluidic device with integrated optical pH, oxygen sensors and algal fluorescence.

201 Considering the unique optical phenomena associated with plasmonic nanostructur

202 We investigate the influence of optical phonon coupling across interfaces comprised of d

203 he influence of scattering from acoustic and optical phonons.

204 Orthogonal optical probes offer a low-noise alternative for direct

205 ent, we show that tactoids can also serve as optical probes to delineate the role of temperature and

206 Anisotropic optical properties also give rise to a magnetic writing

207 spacer layer, which changes the metamaterial optical properties and causes a localized increase in em

208 sition method has a significant influence on optical properties and composition of the films, but neg

209 Optical properties appear to be particularly predetermin

210 ications are contingent upon retaining their optical properties in an aqueous environment.

211 lyze trends in the electronic structures and optical properties of expanded, contracted, and isomeric

212 ia opsins by modifying fundamental nonlinear optical properties of light interacting with the retinal

213 orphology, crystal structures, chemical, and optical properties of the MoS2 QDs were characterized by

214 se), and these have a profound effect on the optical properties of the system, for both one and two p

215 thin metasurface coating can control several optical properties simultaneously over a broad frequency

216 pounds give rise to interesting physical and optical properties with applications in biomedicine and

217 reening quantum dots not only based on their optical properties, but also their surrounding surface t

218 The particles were characterized for their optical properties, growth rate, elemental composition,

219 exchange providing facile tunability of the optical properties, which is usually achieved by mixing

220 entimeters) and heterogeneous electrical and optical properties.

221 anotubes (SWNTs) offer unique electrical and optical properties.

222 ers, which helps achieve good electronic and optical properties.

223 structural coloration often yields emergent optical properties.

224 signals or distorted by variations in tissue optical properties.

225 ectronics due to their unique electronic and optical properties.

226 ove 850 degrees C without degradation of its optical properties.

227 field provides a new method to extend their optical properties.

228 combined with large-area monolayer MoS2 for optical property enhancement and array processing, our r

229 ealed a high degree of similarity between RI-optical property relationships across DOM samples of div

230 Optical pulse-chase experiments with Dendra2-tagged aSyn

231 surface potential is screened with a second optical pump pulse.

232 In our scheme, that we name Optical Pump Rectification Emission, a THz field is gene

233 ulation of QD emission intensity at constant optical pumping rate.

234 ariton lasing up to 200 K under non-resonant optical pumping.

235 Together with the optical qualities of graphene, its acoustic capabilities

236 Scaling of nonlinear optical quantum devices is of significant interest to en

237 The optical radiative force on the mechanical structure is a

238 Here, we use 3D direct stochastic optical reconstruction microscopy (dSTORM) to show that

239 based on information derived from stochastic optical reconstruction microscopy.

240 Optical rectification of 35 fs pulses at the technologic

241 enerated directly on the surface via surface optical rectification of an ultrashort pulse after which

242 We applied handedness-resolved optical reflection spectroscopy to probe the inter-LL tr

243 te analogue by using ultrafast time-resolved optical reflectivity to uncover an intimate connection b

244 e index semiconductor nanostructures support optical resonances that endow them with valuable antenna

245 zed resonances in ultrathin metal nano-strip optical resonators consisting of an array of metallic su

246 nic metasurface with an electrically tunable optical response that operates at strikingly low modulat

247 nsumption is required for the reading of the optical responses and data transmission to a remote user

248 rcular dichroism spectra and of the specific optical rotations.

249 ce single, stable, and centralized rotors by optical S1-S2 cross-field stimulation.

250 in the total number of photons traversing an optical sample, compared to any future direct optical ab

251 Here we propose an all-optical scheme for ultra-bright gamma-ray emission and d

252 Time-lapse video imaging compiled from the optical screening images revealed unexpected differences

253 inherently capable of multicolor imaging and optical sectioning and, with sufficiently fast implement

254 Through the use of optical sectioning structured illumination microscopy (S

255 cent waves are ubiquitous at interfaces with optical, seismic or acoustic waves, and also with electr

256 multi-view App was developed to control the optical sensing parameters and to align each sample to t

257 ns in thin-film solar cells, transistors and optical sensors.

258 The optical signal is hysteresis-free within this range, whi

259 00 large-scale PSM gives both electrical and optical signals by itself without applying an external p

260 rs of ANs communicating by either one or two optical signals, and triads of ANs arranged in both feed

261 To enhance the optical signatures of individual viruses and increase th

262 l power supply or signal generation, the all-optical simplicity of virtual-electrodes may prove signi

263 We demonstrate that optical spatial solitons with non-rectilinear trajectori

264 Here, we report optical spectroscopic and electronic transport evidence

265 confined electronic states, as observed from optical spectroscopy and resonant inelastic X-ray scatte

266 Online process monitoring with a focus on optical spectroscopy can provide a fast, nondestructive

267 -NN, and PPP-NN were investigated by EPR and optical spectroscopy combined with DFT calculations.

268 icult to identify unambiguously using linear optical spectroscopy methods.

269 nd therapeutic purposes over a wide range of optical spectrum.

270 oximately the same in Fe, Ni and Co, but the optical spin-transfer torque is strongly enhanced by add

271 ptical absorption in the SLG, the density of optical states at the location of the SLG, and the extra

272 hermal fluctuation can excite the near-field optical states, creating the potential for thermal radia

273 ntrast agents with an external near-infrared optical stimulus, we can further suppress the background

274 es of isolated nuclei in suspension using an optical stretcher.

275 Modulating the second-order nonlinear optical susceptibility (chi((2))) of materials at the na

276 All-optical switches have been considered as a promising sol

277 fers potential for active optics such as all-optical switching and light modulation.

278 data above and beyond standard limits of the optical system.

279 BCO crystals is measured by means of a local optical technique in the temperature range of 25-300 K.

280 Beyond optical techniques, however, options for noninvasive ima

281 The influence of Tm(3+) or Ho(3+) ion on optical temperature behavior of Y2O3:Er(3+) microtubes i

282 t 121 mW/mm(2) excitation power, which makes optical temperature measurement in wide temperature rang

283 Here, we use optical tissue clearing and a TAM-targeting injectable f

284 Optical tissue clearing has revolutionized researchers'

285 Their applications include spectroscopy, optical tomography, wavefront sensing, and imaging.

286 ng prefrontal activation were recorded using Optical Topography.

287 A strong multiband emission associated with optical transitions from the conduction band to lower E-

288 res, which are associated with the forbidden optical transitions, have been observed.

289 Here, we demonstrate achromatic optical transmission through a planar Fabry-Perot micro-

290 integrin-molecule adhesion kinetics using an optical trap, and diffusion using fluorescence correlati

291 Using an in vitro optical trapping and fluorescence assay, we found that K

292 In this study, we established the optical trapping technique for determining membrane mech

293 Using optical tweezers (OT) and steered molecular dynamic simu

294 or the spatial position of a bead trapped in optical tweezers, which enables us to reconstruct its dy

295 e-by-stage complexity by simply removing the optical tweezers.

296 oscopy and while trapping individual GUVs in optical tweezers.

297 ort on the generation of extreme-ultraviolet optical vortices with femtosecond duration carrying a co

298 cuses on single nanoparticle detection using optical whispering gallery microcavities and photonic cr

299 Conventional optical, X-ray and photoelectron probes often fail to pr

300 Using simultaneous infrared, optical, x-ray, and radio observations of the Galactic b