ライフサイエンスコーパス: optical system

1 in this work is a ray trace analysis of the optical system.

2 ofabricated laminar-flow mixer to a confocal optical system.

3 a single wavelength and analyzed by a simple optical system.

4 try and stability, and low dispersion in the optical system.

5 scintillating nanoparticles, captured by an optical system.

6 ies to overcome limitations specific to each optical system.

7 ction determines the minimum thickness of an optical system.

8 D SIM with minimal or no modification to the optical system.

9 ution limit, without any modification to the optical system.

10 esign that incorporates an augmented reality optical system.

11 d by misalignment and instability due to the optical system.

12 lly been treated as a fixed parameter of the optical system.

13 assification accuracy (~73.2%) in free-space optical system.

14 ave packet and the numerical aperture of the optical system.

15 n aspects of protein structure in a benchtop optical system.

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

17 imaging with no additional complexity in the optical system.

18 ever, it is challenged to conceive a compact optical system.

19 ent points as well as the performance of the optical system.

20 ncrease the telecommunication capacity of an optical system.

21 within the depth of focus (DOF) of the Raman optical system.

22 c range for sensitivity without altering the optical system.

23 nts were measured using a high-resolution 3D optical system.

24 achieved within 95 min using the integrated optical system.

25 evaluate the performance of the fluorescence optical system.

26 e control is a fundamental building block of optical systems.

27 dispersion and have been studied in numerous optical systems.

28 e liquids tunes the characteristics of these optical systems.

29 plications such as reconfigurable sensors or optical systems.

30 , rapid and compatible with a broad range of optical systems.

31 lating and controlling classical and quantum optical systems.

32 OAM sources are critical to the operation of optical systems.

33 s, and rebuilding & duplicating the physical optical systems.

34 the power flow, as expected for conventional optical systems.

35 cial for many applications requiring compact optical systems.

36 are a vital building block of electrical and optical systems.

37 ering the miniaturization and integration of optical systems.

38 nd coherent OAM light sources in fiber-based optical systems.

39 aterial with many applications in lasers and optical systems.

40 a metaform will support a new generation of optical systems.

41 providing a pathway towards achromatic micro-optical systems.

42 tial benefits of these structures for future optical systems.

43 r the assembly, alignment and control of its optical systems.

44 non-equilibrium electrons in nanostructured optical systems.

45 ancing the spatial resolution of traditional optical systems.

46 tromagnetic metamaterials and reconfigurable optical systems.

47 le optical properties not present artificial optical systems.

48 rigid instruments that relied on rudimentary optical systems.

49 ar components enables the miniaturization of optical systems.

50 nsmission and reflection spectra of resonant optical systems.

51 ith the same accuracy as standard microscopy optical systems.

52 the effects of loss are major challenges in optical systems.

53 ed with a measuring tape and then by the two optical systems.

54 egration and scale-up of solid-state quantum optical systems.

55 d specificity potentially rivaling bench-top optical systems.

56 ipulation of microwave signals in chip-scale optical systems(1,2).

57 formed with expensive, specialized ultrafast optical systems(1-12).

58 ures for the setup and calibration of an all-optical system (~3 h), the preparation of an indicator a

59 within transparent cages two meters from the optical system; a proof-of-principle demonstration of a

60 In contrast, traditional man-made optical systems achieve focusing by physical displacemen

61 Given a particular optical system and a finite image acquisition time, what

62 n, characterization, and application of this optical system and demonstrate the rapid application of

63 es of experiments to develop and validate an optical system and image analysis algorithm based upon a

64 , we leverage the rotability of the physical optical system and replace task-specific layers with rot

65 development of the photoelectric absorption optical system and the incorporation of the Rayleigh int

66 The optical system and the source of aberrations in a confoc

67 Photonic nanostructures are used for many optical systems and applications.

68 als has applications for device fabrication, optical systems and biotechnology.

69 hese phases are typically realized in linear optical systems and characterized by their intrinsic pho

70 based detection technique requires expensive optical systems and complex bioinformatics tools.

71 ubwavelength scales enable fundamentally new optical systems and device applications.

72 damental restriction on the vast majority of optical systems and devices.

73 are challenging because they require complex optical systems and diagnostics.

74 ological potential in drug delivery, 'smart' optical systems and microelectromechanical systems.

75 hods enable nanosecond imaging with standard optical systems and sensors, opening a new temporal dime

76 methodology by applying it to two different optical systems and show that this level of accuracy can

77 rther exploring topological phases in driven optical systems and their optoelectronic applications.

78 Each replica was scanned 10 times with a 3D optical system, and 3D datasets representing the compute

79 zation control is therefore pivotal for many optical systems, and achieved using bulk devices such as

80 complexity of nonlinear, heavily multimoded optical systems, and could lead to highly tunable optica

81 aging optical fibres and lasers in nonlinear optical systems, and gravitational singularities associa

82 hR2) or halorhodopsin (eNpHR3.0), via an all-optical system applied to monolayers of neonatal rat ven

83 Resolution limitations of optical systems are major obstacles for determining whet

84 Except for the optical system, as in the calcified lenses of trilobite

85 el methods to increase light transmission in optical systems, as well as to eliminate unwanted reflec

86 n the optical properties of Bragg mirrors in optical systems at temperatures above 700 degrees C beca

87 numerical digits monocularly within a Badal optical system (at both 0.0 and -3.0 D) while performing

88 Ablation characteristics of an optical system based on a diffraction optical element ar

89 have developed a non-invasive and label-free optical system based on Raman spectroscopy for monitorin

90 refractive power was measured with a custom optical system based on the Scheiner principle.

91 h a modified commercial lensmeter or with an optical system based on the Scheiner principle.

92 e sheds light on the potential of free-space optical systems based on engineered surfaces for advanci

93 Here we demonstrate an analogy in optical systems based on epsilon-near-zero materials, ac

94 report the observation of rogue waves in an optical system, based on a microstructured optical fibre

95 uclear magnetic resonance, cold ion trap and optical systems, but a solid-state realization has remai

96 thus arise not via the exchange of different optical systems, but by harnessing the timing of natural

97 tchable direction of light propagation in an optical system by steering it to an exceptional point (E

98 llustrates how transient nonlinearity in the optical system can be exploited to tackle complex optimi

99 ng traditional absorbance or an interference optical system can be used for protein-protein interacti

100 ter simulations further demonstrate how this optical system can track extended objects in 3D, highlig

101 Disorder-based optical systems can be implemented in one-dimensional st

102 5 nm laser excitation with a linear-scanning optical system capable of multichannel real-time fluores

103 A new, in situ sensing system, Channelized Optical System (CHANOS), was recently developed to make

104 The optical system combines optical sectioning with a stereo

105 A simple optical system, comprising a diode laser (405 nm), an op

106 Here we describe measurements of an optical system consisting of a pair of specially pattern

107 In this study, we employed a hybrid diffuse optical system consisting of diffuse correlation spectro

108 The optical system consists of 96 microscopy units, where ea

109 the microarray substrate at the focus of the optical system delivering the light and which can be con

110 with a protein, and a plasmonic surface, the optical system described here selectively amplifies a si

111 ulting issues for both GGG and GOS regarding optical system design are addressed.

112 omise of combining nanophotonic devices, new optical system designs, and machine learning for new fro

113 o advances in materials science and creative optical system designs.

114 -level bias fields injected into multistable optical systems enable a controllable source of quantum

115 the current study is to report an innovative optical system for dual oxyphor phosphorescence lifetime

116 Here we report an achromatic Fresnel optical system for EUV or X-ray radiation that combines

117 ble femtosecond laser and a state-of-the-art optical system for fluorescence studies of mass-selected

118 m dot (QD)-based immunosensor using a simple optical system for human serum albumin (HSA) detection i

119 is problem, we developed a robotic nonlinear optical system for iterative multiphoton microscopy and

120 Here we describe a new optical system for rapid uncaging in arbitrary patterns

121 ial of this technology in the development of optical systems for microscopy, photography, and compute

122 rce solution for multiple-camera tandem-lens optical systems for multiparametric mapping of transmemb

123 ese SVPCs will serve as a unique solution to optical systems for optical computing, multiplexing, dat

124 ns can be found in linking optical qubits to optical systems for which coupling is best described in

125 molecule to the point spread function of an optical system greatly improves the precision with which

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

127 emonstrating blind quantum computation in an optical system has raised new challenges regarding the s

128 rrection of complex vectorial aberrations in optical systems has become an increasingly important are

129 topologically-protected robust transport in optical systems has recently been of great interest.

130 ion-enabled self-powered flexible electronic/optical systems have aroused a new surge of interest in

131 ntal studies in heavily multimoded nonlinear optical systems have demonstrated that the optical power

132 on exceptional points (EPs) in non-Hermitian optical systems have revealed unique traits, including u

133 Compared to near-infrared optical systems, however, mid-infrared component technol

134 We employed this optical system in the setting of ventricular tachycardia

135 d demonstrate it by fabricating the complete optical system in thin-film lithium niobate.

136 t, fully implantable, wireless, battery-free optical systems in miniaturized forms offer attractive o

137 as a potential alternative to the bench-top optical systems in monitoring nucleic acid amplification

138 er provide a proxy for the interpretation of optical systems in some other ancient arthropods.

139 essential to the performance of most modern optical systems including fiber-optic devices.

140 This study introduces a novel optical system integrating laser ablation with saturated

141 With this optical systems integration, the MyoRobot 2.0 allows to

142 The optical system is able to provide a clean, high-flux X-r

143 The optical system is completed by a low-numerical-aperture

144 Our optical system is conceptualized to provide optimal perf

145 An optical system is described for simultaneous video imagi

146 monstration of chaotic communication with an optical system is described.

147 f objective speckles and demonstrate how the optical system is designed for spatially bandlimited ill

148 copy, the signal-to-noise ratio (SNR) of the optical system is directly linked to the numerical apert

149 ing is employed to encrypt a 3-D object, the optical system is incoherent, resulting in negligible am

150 The overall size of an optical system is limited by the volume of the component

151 A simple optical system is used to generate a polarization-varian

152 s while allowing intrinsic errors due to the optical system makes a giant step forward toward realizi

153 ailable temporal and spatial channels of the optical system, making it difficult to represent informa

154 ectrode arrays, video microscopy, and an all-optical system measuring calcium transients.

155 The move towards optical system miniaturization therefore motivates the d

156 rther, given the challenges of miniaturizing optical systems, most cameras do not leverage the wealth

157 This study shows why and when optical systems need thickness as well as width or area.

158 Electronic, magnetic and optical systems now offer an unprecedented combination o

159 Improvement of the optical system of minilaparoscopes may allow reliable be

160 The optical system of the GCAS device tracks the localized c

161 Although optical systems offer high-throughput and energy-efficie

162 All-optical systems offer unique benefits due to their inher

163 The ability to fabricate a complete optical system on a chip offers unrivalled scalability,

164 is expected to find immediate application in optical systems-on-a-chip for metrology, spectroscopy, a

165 This optical system opens possibilities for rapid, inexpensiv

166 holds promise for integration within compact optical systems operating at visible frequencies.

167 Despite the intrinsic bandwidth of optical systems operating at ~200 THz carrier frequencie

168 Advancements in miniaturized optical systems overcome these limitations and allow for

169 in radio frequency, terahertz, infrared, and optical systems, paving a promising avenue toward applic

170 g effects necessary to characterize deployed optical system performance.

171 a step toward compact and efficient quantum optical systems posed to leverage the rapid advances in

172 Vision, which consists of an optical system, receptors and image-processing capacity,

173 llent in many ways, scaling to large quantum optical systems remains challenging.

174 Many modern optical systems require dynamic manipulation of light, a

175 Most practical optical systems require that the device properties be ti

176 his approach presents a path to creating the optical systems required for large-scale trapped-ion qua

177 y verified to work with off-axis and on-axis optical systems, showing the versatility of the approach

178 hiPSC-CM) technology and by contact-free all-optical systems simultaneously measuring action potentia

179 However, in optical systems such as microwave synthesizers(6), optic

180 ications for CMOS-integrated, reprogrammable optical systems such as optical neural networks for deep

181 s enhancement can be achieved using resonant optical systems such as plasmonic particles or nanoanten

182 Optical systems, such as colorimetric and fluorescence-b

183 the door for a new class of atomically thin optical systems, such as rapidly switchable beam arrays

184 An image-forming optical system that is based on a mirror with an unconve

185 The Photonic Fence (PF) is an optical system that uses machine vision, infrared light,

186 Here we present an optical system that, under appropriate conditions, ident

187 nd readout, experiments so far have employed optical systems that are cumbersome to scale to even a f

188 escent coupling scheme works well for planar optical systems that are naturally waveguide based, many

189 ic properties in nanomaterials and designing optical systems that efficiently excite and collect ligh

190 es in miniaturization technology have led to optical systems that no longer require complicated mecha

191 al demonstrations have been implemented with optical systems that used both discrete and continuous v

192 The combination of a confocal optical system (that confines incident light to a reduce

193 ture of the objective, the efficiency of the optical system, the emission rate of the single molecule

194 ticular attention to the organization of the optical system, the retinular cells, the rhabdom, and of

195 Differing from conventional optical systems, the point-spread function in DAR is det

196 oposed for the transport of light through an optical system; this involves photon-photon interactions

197 he high speed and high bandwidth inherent to optical systems, thus enabling the direct processing of

198 These results show the promise of an all-optical system to acquire action potentials with precise

199 flexible substrate was incorporated into an optical system to demonstrate high resolution imaging of

200 We design and build a high-speed optical system to measure action potential, cytosolic ca

201 blue] and 623 [red] nm) were presented by an optical system to one eye after dilation, while the cons

202 into the design and operation of free-space optical systems to create new functionalities.

203 reconstructions used expensive, specialized optical systems to gather information about the hidden s

204 However, using conventional optical systems to generate, analyse and detect circular

205 ar field and near field, it allows far-field optical systems to project an image of the near-field fe

206 y images acquired using inexpensive portable optical systems to train networks for the evaluation of

207 The miniaturization of optical systems (to the micro and nanoscale) has resulte

208 on is up to 10 times higher than that of the optical system used to take the measurements.

209 tasurfaces are especially important, as most optical systems used in practice operate in transmission

210 The customized optical system uses multiple fixed-wavelength lasers to

211 neural activity, we designed a needle-based optical system using gradient-index (GRIN) rod lens.

212 was measured with a custom-built, noncontact optical system, using a focus detection technique.

213 A three-channel optical system was developed that simultaneously measure

214 A novel fluorescence microscope/laser optical system was developed to measure fast transients

215 A custom optical system was used for video recording of tear film

216 An eight-channel optical system was used to generate lights that differed

217 Videos and images from a schlieren optical system were analyzed during spontaneous breathin

218 Maxwellian-view and direct-view optical systems were used to obtain foveal and extrafove

219 lasers play a significant role in precision optical systems where an electro-optic laser frequency s

220 ment or modification leads to reconfigurable optical systems, whereas the implementation of optics th

221 s on two critical challenges: the inertia of optical systems, which limits image speed, and aberratio

222 tes within the limited depth-of-focus of the optical system while maintaining the necessary reagent f

223 A Maxwellian-view optical system with a xenon light source was used to pre

224 An optical system with a Xenon-arc light source, chromatic

225 mages has been demonstrated in an incoherent optical system with biometric keys.

226 An optical system with shaping optics is used to direct a w

227 matic effect in a one-dimensional disordered optical system with spatial features a thousand times sm

228 The demand for high-resolution optical systems with a compact form factor, such as augm

229 Although integration of optical systems with classical microfluidic analysis tec

230 very important class of dissipative (active) optical systems with cyclic gain and losses, such as las

231 The realization of programmable, active optical systems with fast, tunable components is among t

232 commercial pol-PDs use bulky and complicated optical systems with lenses, polarizers, and mechanical

233 e that the two modes can also be observed in optical systems with only a few (artificial) atoms insid

234 hese ECM patterns currently require advanced optical systems with signaling processing analysis.

235 BB particles can be a complicated optical system, with scattering and absorption contribut

236 aluation of directly filtered data, using an optical system without extensive numerical spectral anal