ライフサイエンスコーパス: optical

1 We achieved this goal by correcting optical aberrations in gradient index lens-based ultrath

2 ur ablation in mice, and that they have high optical absorbance in a broad near-infrared region spect

3 A detailed analysis of the optical absorption gives access to the value of the zero

4 ocessed in the frequency-domain to obtain an optical absorption spectrum.

5 Here, we combine optical absorption, magnetic circular dichroism and firs

6 rol over coherent spin rotations by using an optical AC Stark shift.

7 s individual nanoparticles while maintaining optical access to the molecular junction.

8 The membrane configuration also provides optical access to the sensing interfaces at a broad rang

9 This enabled optical access, while microfluidic trapping allowed for

10 e report on a multi-method approach based on optical, acoustic, satellite remote sensing, and simulat

11 As a result, efficient induction of optical activity in the chromophoric system is observed.

12 The hyper-Rayleigh optical activity study reveals important charge-transfer

13 r the automated generation, maintenance, and optical analysis of human midbrain organoids in standard

14 Optical and electron microscopies as well as electron an

15 Optical and electron microscopy of HIPK4-null male germ

16 roscopy, vibrational circular dichroism, and optical and electron microscopy.

17 ectron microscopy reveal the well-associated optical and electron signal at a high specificity, with

18 e of the nanoparticle is demonstrated by its optical and electronic properties, with metal-like elect

19 single-molecule tools and techniques such as optical and magnetic tweezers, atomic force microscopy (

20 ion between the 3D fibrillar network and the optical and mechanical properties of the macroscopic mat

21 y loss and thermal noise errors in realistic optical and microwave communication channels and study t

22 Unlike other exoplanets, it is bright in the optical and nondetected in the infrared, and its orbit a

23 inted perovskite NWs array exhibit excellent optical and optoelectronic properties and can be conveni

24 of these fluid inclusions was determined by optical and spectroscopic methods.

25 These ions have optical and spin transitions that are first-order insens

26 ASnBr(3) , obtained by means of diffraction, optical and X-ray photoelectron spectroscopy.

27 as a result of their superlative electrical, optical, and mechanical properties.

28 In addition, strong in-plane optical anisotropy is demonstrated via polarized Raman s

29 velopment, optimization, and applications of optical approaches to measure the spatial and temporal p

30 These works can be divided into paper-based optical aptasensors and paper-based electrochemical apta

31 ges to overcome a strong evaporation-induced optical artifact in heated glass fiber pads due to chang

32 ic polariton propagation, as their auxiliary optical axis is in the plane.

33 NHCs results in a bathochromic shift of the optical band gap of CdSe QDs (R = 1.17 nm) of up to 111

34 f the beta-Ga(2)O(3) nanowires including the optical bandgap and photoconductance.

35 bandgap edge, the Se(0.32) Te(0.68) film (an optical bandgap of ~0.8 eV)-based photoconductor exhibit

36 on along one molecular axis, engendering low optical bandgaps and improved oscillator strength for th

37 These studies demonstrate a powerful in situ optical battery platform for unraveling the complex reac

38 Corneal power measured by optical biometers was higher than measurements by Pentac

39 Over the past decade, so many new optical biometers, formulas, and methods (whose accuraci

40 The metal-clad leaky waveguide (MCLW) is an optical biosensor consisting of a metal layer and a low

41 eflective Phantom Interface (RPI) label-free optical biosensor.

42 An optical buffer featuring a large delay-bandwidth-product

43 By utilizing optical calcium imaging, which records calcium ion flux

44 The fast-optical camera could lead to multiple applications in Qu

45 Incorporating optical cavities in ion traps is becoming increasingly i

46 Interactions between atoms and light in optical cavities provide a means of investigating collec

47 By using an optical cavity substrate consisting of Au/Al(2) O(3) to

48 In contrast to an optical cavity, a two-level system operates with no more

49 eport on the development of a simple, linear optical cavity-based system combining evanescent wave (E

50 Using a combination of machine learning, optical character recognition, and manual curation, we i

51 In this work, the optical characterization of 2D materials is used as a ca

52 of morphological, structural, electrical and optical characterization of the beta-Ga(2)O(3) nanowires

53 Structural and optical characterization showed that the inorganic latti

54 of our probes in simultaneous recording and optical/chemical modulation of brain activities across d

55 nd provide a brief overview of the different optical clearing methods as well as different imaging mo

56 With the use of a transgenic mouse line, optical clearing, and imaging techniques, combined with

57 However, the best optical clocks have not seen their performance transferr

58 ency synthesis(4), frequency division(5) and optical clocks(6).

59 Dynamic optical coherence elastography (OCE), which launches and

60 Anterior segment optical coherence tomography (AS OCT) is a helpful tool

61 ue (K-max), thinnest point, anterior segment optical coherence tomography (AS-OCT)-based stage of ect

62 Optical coherence tomography (OCT) imaging of the optic

63 Previous deep learning studies on optical coherence tomography (OCT) mainly focused on dia

64 one alternative non-invasive system based on Optical coherence tomography (OCT) technology, called OC

65 for amblyopia treatment, fundus photographs, optical coherence tomography (OCT), and visual acuity.

66 Magnetic resonance imaging (MRI), optical coherence tomography (OCT), VF, and optic disc p

67 of quantitative micro-elastography (QME), an optical coherence tomography (OCT)-based elastography te

68 producibility and interocular symmetry using optical coherence tomography (OCT)-based measurements of

69 Optical coherence tomography (OCT)-derived retinal measu

70 assessed for established patients receiving optical coherence tomography (OCT)-guided intravitreal i

71 hen tissue overlying the struts is >0 mum by optical coherence tomography (OCT).

72 s of patients with ECE using spectral-domain optical coherence tomography (SD-OCT) imaging and presen

73 e by using SW-AF imaging and spectral-domain optical coherence tomography (SD-OCT) scans.

74 r angle status was evaluated by swept-source optical coherence tomography and IOP was estimated by th

75 on is a critical step in analysis of retinal optical coherence tomography angiography (OCTA) images,

76 e unique capabilities of our adaptive optics-optical coherence tomography approach and owing to their

77 Optical coherence tomography demonstrated decreased reti

78 Swept-source optical coherence tomography helps ophthalmologist inves

79 children (ages 5.8 to 15.8 years) underwent optical coherence tomography imaging to quantify foveal

80 Electroretinogram (ERG) and optical coherence tomography of Erdj5-/- and P23H+/-:Erd

81 esponse to anti-VEGFs, using spectral-domain optical coherence tomography scans obtained from a cohor

82 Using in vivo imaging, such as optical coherence tomography, scanning laser ophthalmosc

83 n metabolic rate in rats using visible-light optical coherence tomography.

84 foveal microstructure using spectral-domain optical coherence tomography.

85 Optical colonoscopy follow-up rates for positive results

86 zation of light, such as digital holography, optical communications and biomedical imaging.

87 -product-a critical component for future all-optical communications networks-remains elusive.

88 gh-performance preconcentration elements and optical components for fluorescence measurement of speci

89 However, these optical components inherently exhibit chromatic behavior

90 With the push towards miniaturization of optical components, static metasurfaces are used as comp

91 Our optical computations using a unit cell approach reproduc

92 ion-the reverse Pulfrich effect-is caused by optical conditions induced by monovision, a common corre

93 onic amplification is generally tied to high optical contrast materials which limit the applicability

94 nd can be broadened by engineering selective optical coupling mechanisms to the resonator.

95 ble light pulses with duration down to a few optical cycles; we then discuss the pump-probe technique

96 ngle layer, where a single device can record optical data, convert it into a conductance state and st

97 oriented vessels nasally and the horizontal optical defocus induced by WTR astigmatism.

98 ility of the technique to map visual pigment optical density and synthesis rates in eyes with and wit

99 nonical cell-wall cross-links achieve a high optical density in culture, divide and elongate successf

100 ication of enzyme-linked immunosorbent assay optical density thresholds and the serotonin release ass

101 photonics in the prototype that has a novel optical design using volume gratings with polarization s

102 Here we report the optical detection of strongly correlated phases in semic

103 However, coherent and incoherent optical detection results in fundamentally different noi

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

105 opy lacks high spatial resolution due to the optical diffraction limit and difficulty to preserve a h

106 ode resonance (LMR) could be observed in the optical domain, where electrical properties of the film

107 n(5-7) and giant second-order non-reciprocal optical effects(8) in antiferromagnetic (AFM) bilayers.

108 pments and technical breakthroughs including optical, electrochemical and electrical biosensors for e

109 e understanding and exploitation of combined optical, electronic, and magnetic properties.

110 erostructures are central to next-generation optical, electronic, and quantum information application

111 promising routes for tailoring the chemical, optical, electronic, or mechanical properties of MXenes.

112 alternative to both conventional diffractive optical elements (DOEs) and metalenses for applications

113 Spatial light modulators are essential optical elements in applications that require the abilit

114 l metasurfaces over conventional diffractive optical elements is their capability to efficiently defl

115 e successfully implemented without any extra optical elements nor external power supplies, explicitly

116 s in nanophotonics, enabling a new family of optical elements with exceptional degrees of freedom.

117 Enhancement of optical emission on plasmonic nanostructures is intrinsi

118 id chromatography-inductively coupled plasma-optical emission spectrometry (HPLC-ICP-OES) in addition

119 scopy (FAAS), and inductively coupled plasma optical emission spectroscopy (ICP-OES).

120 the semiconductor moiety, which harvests the optical energy and funnel it to the luminescent metal ce

121 frequency is brought onto resonance with the optical excitation, a 12-fold increase of the amplitude

122 We describe an optical feedback loop involving both partners of the ass

123 micro-optrode (also termed micro-optode and optical fiber microsensor) is a tapered optical fiber wi

124 Optical fiber presents a 100-1,000x lower heat load than

125 noglobulin G (IgG) was deposited on a silica optical fiber surface previously functionalized with PAN

126 /manipulation with light-emitting diodes and optical fiber technologies which now allows for a broad

127 on through mid-infrared ablation with a fine optical fiber tip for ionization by f-LAESI.

128 and optical fiber microsensor) is a tapered optical fiber with an O(2)-sensitive fluorophore coated

129 Two inclined optical fibers are permanently fixed to a common board,

130 r experiments of quantum effects in low-loss optical fibers which is critical for scalability of real

131 ack is the need for invasive implantation of optical fibers.

132 When coupled to a plastic optical fibre (POF) plasmonic platform, the analyte-indu

133 A section of optical fibre was integrated into an active fibre ring c

134 A sensor consisting of an optical fibre with the exposed tip coated with the polyo

135 men for holding the imaging probe, and three optical fibres equally and spirally distributed on the o

136 , tying isolated vortex knots in the complex optical field has been realized.

137 lying topological principles(4,5) to control optical fields and could lead to energy-efficient gratin

138 ap quantum information between microwave and optical fields.

139 Here, we report an unconventional nonlinear optical filtering effect resulting from the interfacial

140 ation, we adopt a novel brightness-invariant optical flow algorithm that helps us reduce error in blo

141 Here we implement variational optical flow analysis as a new approach to analyze the p

142 can be translated into the classical linear optical framework.

143 ive terahertz rotational transitions with an optical frequency comb, and read out the final state non

144 sonator solitons are critical to miniaturize optical frequency combs to chip scale and have the poten

145 py(11-13), the search for exoplanets(14,15), optical frequency synthesis(16), time keeping(17) and ot

146 We demonstrate an optical frequency-domain multiplexing technique, allowin

147 edback control of frequency combs is used in optical-frequency synthesis(4), frequency division(5) an

148 Our concept offers a practical, all-optical, fully three-dimensional tomography of electroni

149 hierarchical biopolymer frameworks for added optical functionalities, such as enhanced iridescence an

150 grated into an active fibre ring cavity with optical gain and interrogated by the OFDR system for 11

151 However, applications relying on their optical gain suffer from nonradiative Auger decay due to

152 an access planarized structures with reduced optical gaps and redox potentials.

153 Optical glutamate sensors combined with patch-clamp and

154 Graft survival for optical grafts was significantly better than therapeutic

155 titative imaging, conditional knockdown, and optical highlighting indicate that papilin, a poorly stu

156 Here we conceptualize an IR-optical hybrid (IR-OH) approach that sensitively measure

157 Consequently, this pH-activatable optical imaging agent may be clinically beneficial in di

158 visual cortical areas using intrinsic signal optical imaging and then injected fluorescently tagged r

159 Here, we used integrated optical imaging in a rat self-administration and a mouse

160 ve cortical areas, we undertook simultaneous optical imaging of intrinsic signals in macaque V1, V2,

161 Here, we show that AND-gate optical imaging probes that require the processing of tw

162 A high-resolution, three-dimensional, optical imaging technique for the murine brain was devel

163 pare in vivo radiologic imaging with ex vivo optical imaging techniques for assessing hypoxia, microv

164 l quantification of cell viability by simple optical imaging using "single cell adhesion dot arrays"

165 an be considered for functional integrations optical-induced sensing.

166 es to electromagnetic fields have focused on optical intensity-related effects, but phase information

167 otential for the OTM in various self-powered optical interactive applications.

168 for the next generation of Si-based on-chip optical interconnects.

169 reas inhibition of SNr GABA neurons produced optical intracranial self-stimulation and place preferen

170 As an application, a Si(3)N(4)-based optical isolator is demonstrated by spatiotemporal modul

171 cts manifest themselves in the large magneto-optical Kerr effect(1,2), spontaneous helical light emis

172 ive to magnetic field fluctuations, enabling optical linewidths of less than one megahertz and spin c

173 studied, with various photonics devices and optical links being demonstrated.

174 such tight confinement inevitably increases optical losses through various damping channels.

175 show experimentally that the often neglected optical magnetic field can nevertheless play an importan

176 e in bacterial sensing owing to their unique optical, magnetic, and electrical properties.

177 n boundaries (GB defects) on the electrical, optical, magnetic, mechanical and chemical properties of

178 pplied a recently introduced non-destructive optical manipulation technique to measure the tension in

179 We perform optical mapping and transmission electron microscopy in

180 egration locus, demonstrating the utility of optical mapping for the analysis of genomic regions that

181 ls) cells, biochemistry, dual Ca(2+)/voltage optical mapping in intact hearts from alcohol-exposed or

182 pplication of spaced seeds in the context of optical mapping, which allows for spurious and deleted c

183 n heart rate, as measured by ECG and ex vivo optical mapping.

184 The sensor has been used to optical measurements also simultaneously interrogated el

185 Optical measurements show as-deposited FAPI films have a

186 Our work demonstrates efficient optical metamaterial engineering based on structured ens

187 erials that are broadly used for fabricating optical metasurfaces for visible light applications.

188 One of the important advantages of optical metasurfaces over conventional diffractive optic

189 or actions on single trials, we developed an optical method (COSMOS) for tracking neural activity in

190 nition of the pH value, a brief look back on optical methods for sensing of pH, on the effects of ion

191 Conventional optical methods, based on autocorrelation, are very diff

192 ads to periodic textures that can be used as optical microarrays, templates for soft lithography, and

193 The resulting gels were characterized using optical microcopy and atomic force microscopy.

194 Spatially targeted optical microproteomics (STOMP) is a method to study reg

195 y measures molecular composition based on an optical microscope with wide-field interferometric detec

196 ifferential scanning calorimetry, polarizing optical microscopy and X-ray diffraction provided insigh

197 CMOS (sCMOS) technology has greatly advanced optical microscopy for biomedical research with superior

198 lipid-lipid interactions in vitro, alongside optical microscopy techniques aimed at directly visualiz

199 racterized through UV-VIS spectrometry, SEM, optical microscopy, and light exposure.

200 Four articles that explore using ray-tracing optical modeling suggest an "illumination gap," in which

201 -phonon coupling to specific fully symmetric optical modes during the buildup of a three-dimensional

202 to three broad classes: nanomotors driven by optical momentum transfer, photothermal heating, and pho

203 Simultaneous optical monitoring of CaCC activity and Ca(2+) dynamics

204 ith tunable luminescence as a new option for optical multiplexing.

205 stems and within data centres for high-speed optical networking of computers.

206 overing new deep-ultraviolet (DUV) nonlinear optical (NLO) materials is currently a great challenge.

207 theless play an important role in a class of optical nonlinearities driven by both the electric and m

208 Here we report optical observations of lightning flashes by the Juno sp

209 Combined with simple optical or electrical feedback, the structure is suitabl

210 trons and more disperse bands for holes upon optical or thermal excitation.

211 annot be explained with classical models for optical outcoupling.

212 est in using a network of coupled degenerate optical parametric oscillators (DOPOs) to effectively fi

213 ented setup combines high sensitivity, large optical path lengths, and short measurement times and th

214 We reveal two measurement dimensions: optical phase, and time-of-flight (TOF), the latter with

215 , as well as novel explorations in microwave-optical photon entanglement and quantum sensing mediated

216 It provides an optical platform to develop new multimolecular and funct

217 (2020) evaluated dual-wavelength optical polarization imaging (OPI) for the detection for

218 the speed of particle motion increases with optical power absorption and is also affected by particl

219 Optical probes operating in the second near-infrared win

220 need to design and develop sensitive chiral optical probes that can function within a biological set

221 tures (e.g. intact wood patterns), excellent optical properties (an average transmittance of ~ 80% an

222 en developed on the nanoscale with excellent optical properties (e.g., semiconductor quantum dots, pe

223 rticle spectroscopy in revealing the diverse optical properties and functionalities of nanomaterials,

224 llizable when meticulously designed, and the optical properties are more affected at the single atom

225 These optical properties are observed in MeCN solution and the

226 icle-based materials and devices with unique optical properties at the macroscale.

227 lymer LED array and demonstrate its improved optical properties compared with a purely inorganic micr

228 Due to optimized thickness and optical properties of ITO film, a lossy-mode resonance (

229 ovide exciting opportunities for controlling optical properties of photonic devices dynamically.

230 The equilibrium and non-equilibrium optical properties of single-layer transition metal dich

231 omal collagen is closely associated with the optical properties of the cornea, the absence of any lar

232 the photoacid generators and changes in the optical properties of the QDs at each patterning step.

233 Optical properties suggest that permanganate oxidation d

234 idate the dynamic changes in DOM composition/optical properties with molecular weight within individu

235 on of circularly polarized light and display optical properties with prominent handedness, that is, c

236 y studied for their structural coloration or optical properties within the visible spectrum, their pr

237 lation in chemical, electronic, magnetic and optical properties, mediated by the reversible transfer

238 Uncertainties in the contrail age, coverage, optical properties, radiative forcing, and energy forcin

239 bility (pH, lipid oxidation, lipolysis), and optical properties.

240 es with prominent handedness, that is, chiro-optical properties.

241 ations in the linker stacking geometries and optical properties.

242 nd-gap modification which exhibit tailorable optical properties.

243 nd strength) and interesting physical (e.g., optical) properties.

244 h the composite architecture and last beyond optical pulse temporal characteristics.

245 chitectures and improving the structural and optical quality of III-nitride-based devices.

246 The optical quality of the cornea was preserved with lower H

247 Optical quantum states are uniquely suited for this purp

248 s, we found an extraordinarily large magneto-optical Raman effect from an A(1g) phonon mode due to th

249 ed compounds and offers a future pathway for optical readout of these molecules.

250 lic voltammetry (CV) scans under synchronous optical readout were performed to study the effects of e

251 d localization microscopy (PALM), stochastic optical reconstruction microscopy (STORM) and structured

252 erturbation to cells, ECORE allows long-term optical recording over multiple days.

253 We present optical recordings, receptive field maps, and sensitivit

254 iazem) and compared the outcomes to in vitro optical recordings.

255 large changes in its electric conductivity, optical reflectivity and density.

256 ctromagnetic waves for frequencies up to the optical region.

257 However, currently available optical reporters are not capable of detecting small cha

258 perimental and theoretical approaches of the optical response visible region were studied to understa

259 ographic direction significantly affects the optical response, and can serve as a key tuning paramete

260 ymmetry and substantially enhanced nonlinear optical response.

261 derable challenge despite their advantageous optical responses and applications in energy storage sys

262 The optical rotation angle is determined by measuring the ph

263 Furthermore, the spin-valley optical selection rules(12-14) of transition metal dicha

264 sized CDs was applied as a fluorophore in an optical sensor after modification with molecularly impri

265 lopment of simple, novel, and cost-effective optical sensor to detect and quantify Bisphenol A (BPA)

266 In this work, a modern optical sensor was developed for IXC, based on environme

267 Optical sensors can provide a non-invasive, inexpensive,

268 using a smartphone coupled to an appropriate optical setup, opening the way to simple and inexpensive

269 t the three pillars of the virtual ultrafast optical spectrometer, able to deliver transient spectra

270 Here we used NMR and optical spectroscopy to identify conditions that enable

271 Optical spectroscopy-based online monitoring offers a po

272 lecting frequency-modulated input and output optical states in a nearly orthogonal manner, a sensitiv

273 r recording and genetic-engineering-assisted optical stimulation is a powerful tool for the study of

274 than a typical spike detection threshold, at optical stimulation of >50 mW mm(-2) irradiance.

275 Chronic optical stimulation revealed normal homeostatic plastici

276 The high-bandwidth optical-stimulation capacity of the device might facilit

277 The propagation of the beam along the optical system has been studied using the Gaussian beam

278 Here, by adopting an optical technique in the context of freezing-namely, tot

279 Established electrical and optical techniques typically break down at this scale du

280 Optical technologies allowing modulation of neuronal act

281 ridge superconducting quantum processors and optical telecommunication channels.

282 ered involving different activation methods (optical, thermal, or combined) for generating liquid-sta

283 in a magnetic field is a model system where optical transitions between Landau levels (LLs) are desc

284 l Weyl fermions are excited during selective optical transitions between the tilted anisotropic Weyl

285 tates and thus the energy and dynamics of QD optical transitions.

286 dular optical tweezers (AFMOTs), in which an optical trap can be reliably created and freely moved on

287 by changing the types of fibers for both the optical trap creation and particle position detection.

288 Here, we present the all-fiber modular optical tweezers (AFMOTs), in which an optical trap can

289 measurements of microdroplets using aerosol optical tweezers (AOT) and analysis of the whispering ga

290 Miniaturization and integration of optical tweezers are attractive.

291 Here, we use single-molecule optical tweezers measurements to compare translocation o

292 Manipulation of individual molecules with optical tweezers provides a powerful means of interrogat

293 Using a dual-trap optical tweezers setup, we found the fusion speeds of fo

294 These measurements were conducted using optical tweezers, which enabled high temporal and spatia

295 d nucleotide conditions using high-precision optical tweezers.

296 g was overcome by trapping particles with 2D optical tweezers.

297 can serve as a cocktail sensor for multiplex optical urinalysis in the mouse models of drug-induced a

298 ostinjection), the reporters can be used for optical urinalysis of immunoactivation simply by detecti

299 al vector (CV) beams and helical phase front optical vortex (OV) beams.

300 We demonstrate time reversed optical waves with a device capable of independently con