ライフサイエンスコーパス: multimode

1 We demonstrate how multimode 2D IR spectroscopy of the protein amide I' and

2 entrated among clinical trial ($110,869) and multimode ($59,916) principal investigators.

3 ational (61.3%), clinical trial (67.3%), and multimode (70.9%) researchers were significantly more li

4 Presented here is a novel multimode ambient ion source termed desorption electrosp

5 We used a spatially multimode amplifier based on four-wave mixing in a hot v

6 linear-resonator phenomena are intrinsically multimode and exhibit complex modelocking, here we demon

7 Here we introduce an all-optical platform in multimode and multicore fibres.

8 Using this approach, we show that both multimode and single-mode rhombohedral-stacked MoS(2) wa

9 spray (DESI-like)-only, MICI-only, and DEMI (multimode), and can be thus operated in each of these mo

10 In this work, we utilize a multimode approach to characterizing energy losses in su

11 om strongly deteriorated beam quality due to multimode behavior, diffraction of light and self-focusi

12 It relies on a multimode blue laser diode receiving optical feedback fr

13 The application of a multimode BODIPY-type fluorescence, photometry, and X-ra

14 states with large time-bandwidth product and multimode capacities.

15 r individual photon modes as well as for the multimode case.

16 lves monitoring of foulant deposition during multimode cation exchange chromatography based purificat

17 otential to study similar questions in fully multimode cavities.

18 conductor superlattice gain medium, inside a multimode cavity between two acoustic Bragg reflectors.

19 ole of an active quantum gas microscope, the multimode cavity QED system both images the phonons and

20 t such an experiment using a superconducting multimode cavity, the nonlinearity of which was tailored

21 The multimode coupling depends on the spatial profiles of th

22 We developed a multimode dermoscope that combines polarization and hype

23 Here we propose a platform for on-chip multimode devices with minimal inter-mode coupling, open

24 For broadband and multimode devices, however, more complex structures, her

25 of both phase-preserving and phase-sensitive multimode directional amplifiers.

26 Various transient and random phenomena of multimode DSs are revealed, highlighting the importance

27 or a research field at the junction of laser multimode dynamics and Kerr parametric processes.

28 oids fundamental limitations associated with multimode effects for traveling optical photons.

29 Characterization of the products by multimode electron tomography and analysis of the NC mor

30 ero as the size grows, leading to inevitable multimode emission.

31 s on 38 arbitrary pairs of modes and prepare multimode entangled states, all using only two control l

32 s improved scaling with Wigner tomography of multimode entangled W states of up to 4 modes on a 3D ci

33 mbrane and Fabry-Perot resonators will allow multimode entanglement involving electromagnetic, mechan

34 hwarz inequality, witnessing the presence of multimode entanglement.

35 tonic material to host phonon dynamics and a multimode excitation spectrum.

36 e broadening of the Brillouin spectrum under multimode excitation, without broadening of transmitted

37 ning of the Brillouin scattering spectrum by multimode excitation.

38 vidence for oligomer decomposition producing multimode F-TD/CIMS thermograms is provided by the measu

39 tted through the dichroic and focused onto a multimode fiber (core diameter 50 microm), which carried

40 rot (FP) mesoresonator based on graded index multimode fiber (GRIN-MMF).

41 h multimode optical fibers, we show that the multimode fiber (MMF) output speckles contain the three-

42 Our multimode fiber amplifier can operate at high power with

43 Here, we explored a highly multimode fiber amplifier in which stimulated Brillouin

44 Here, we study theoretically using a highly multimode fiber amplifier with many-mode excitation for

45 multi-point deformation sensing via a single multimode fiber by using k-nearest neighbor (KNN) machin

46 -shaping of coherent input light to a highly multimode fiber can increase the power threshold for sti

47 an assembly of a graded-index and large core multimode fiber directly spliced to a single mode fiber.

48 Multimode fiber lasers thus open new directions in studi

49 roscopy, multicolor fluorescence microscopy, multimode fiber micro-endoscopy and light-sheet fluoresc

50 Since conventional multimode fiber power flow model does not take into cons

51 Large core optical multimode fiber provides benefits such as a large light-

52 s for an optical pulse propagating through a multimode fiber with strong random mode coupling.

53 r than the spectral correlation width of the multimode fiber, the amplified light maintains high spat

54 human multicellular microtissues by adopting multimode fiber-based, low repetition rate, high peak po

55 interfaced with a pressure-flow system and a multimode fiber-loop cavity using concave fiber lenses w

56 es on a continuum of plane-wave modes, their multimode-fiber counterparts must be constructed from th

57 is done by laser epi-illumination through a multimode fiberoptic whose micron-sized tip can be intro

58 Multimode fibers (MMFs) are gaining renewed interest for

59 scopic memory effect emerging in square-core multimode fibers and demonstrate fluorescence imaging wi

60 While light propagation through multimode fibers and scattering media share many analogi

61 any analogies, reconstructing images through multimode fibers from speckle correlations remains an un

62 umber of spatial modes supported by standard multimode fibers is a promising platform for boosting th

63 However, the practical use of long multimode fibers is severely hampered by modal crosstalk

64 Our work shows that multimode fibers provide a fertile ground for studying c

65 g fields, coupling spatiotemporal light into multimode fibers remains a fundamental experimental chal

66 xed quantum communication protocol over long multimode fibers to illustrate potential applications th

67 monstrate near-video-rate 3D imaging through multimode fibers with a total aperture of several hundre

68 es can function as single-mode, few-mode, or multimode fibers, with spines serving as illumination po

69 econfigurable group velocity in graded-index multimode fibers.

70 dal interactions in core-diameter decreasing multimode fibers.

71 The optical transport of images through a multimode fibre remains an outstanding challenge with ap

72 iton self-frequency shifting in graded-index multimode fibre.

73 We apply this concept to multimode fibres (MMFs) and identify a 'quasi-radial' me

74 unication systems rely almost exclusively on multimode fibres for short- and medium-haul transmission

75 such as present in holographic diffusers and multimode fibres.

76 Multimode fluorescent microscopy was used to correlate m

77 We have used multimode fluorescent speckle microscopy (FSM) and corre

78 We have used multimode fluorescent speckle microscopy (FSM) to direct

79 Using multimode focusing, the activation function features bot

80 ing, using both experimental measurements of multimode frequency shifts and numerical simulations, to

81 A major limitation on the bandwidth of multimode glass and plastic optical fibers is modal disp

82 gy exchange akin to a beam splitter for easy multimode handling.

83 tinol (NiTi) tubes configured in a versatile multimode heat exchange architecture, which allows the h

84 Our results align with an extended multimode Hopfield model that accounts for spatial field

85 Multimode HPLC should prove useful for preparing low pmo

86 formed in the same chromatographic analysis (multimode HPLC) and unambiguous separation between neutr

87 A multimode imaging system allows the tracking of microtub

88 require docking suggests that Far1 acts as a multimode inhibitor that antagonizes both kinase activit

89 er with selected ion monitoring, utilizing a multimode inlet allowed for lower injection temperatures

90 The most relevant parameters of a multimode inlet were optimized to increase the injection

91 fects, like the Risken-Nummedal-Graham-Haken multimode instability, we envisage the usefulness of the

92 The light from the lasers is coupled via an multimode interference (MMI) coupler into a semiconducto

93 Multimode interference (MMI) devices promise a straightf

94 A solid-core multimode interference (MMI) waveguide crosses multiple

95 We use a single multimode interference (MMI) waveguide to create wavelen

96 composes of four Y-multijunctions and 2 x 2 multimode interference coupler using silicon-on-insulato

97 The device relies on imaging multimode interference from leaky modes along a multimod

98 This tapered fibre multimode interference spectrometer achieves a spectral

99 Multimode interference spectroscopy is suitable in a var

100 is implemented by multispot excitation on a multimode interference waveguide platform, and detection

101 tion of these waveguides forms a liquid-core multimode interference waveguide that allows for multi-m

102 GC x GC-HR-ToF MS with a multimode ion source (MMS) offers consecutive runs in EI

103 proach has been used to optimize the Agilent multimode ion source.

104 avefront shaping enables coherent control of multimode laser amplification, with potential applicatio

105 ias current and output power, we demonstrate multimode laser emission centered around 3 THz, with dis

106 ectively bound within the evanescent zone of multimode laser-illuminated fibers.

107 uperior manipulation of the modal content of multimode lasers, and adiabatic control of topological e

108 es at 83 K, thus allowing the observation of multimode lasing with an optical pumping threshold densi

109 eal-time tunable wavelengths, and controlled multimode lasing.

110 D-shaped cavity optimized to achieve highly multimode lasing.

111 paper presents a physical frequency-diverse multimode lens-loaded cavity, designed and used for the

112 I have been defined using the semiautomated, multimode light microscope, together with a fluorescent

113 re fibres provide an efficient way to couple multimode light to an array of single-photon avalanche d

114 ed single-mode wavelength-to-time mapping of multimode light using a multicore fibre photonic lantern

115 s can perform optical equalisation to smooth multimode light, or act as a distributor, guiding it int

116 damping feedback and unexpectedly observe a multimode maser that oscillates at frequencies of transi

117 between separate silicon chips throughout a multimode-matched fibre.

118 This multimode mechanism of action concordantly results in co

119 the IN-LEDGF/p75 interaction, determines the multimode mechanism of ALLINI action.

120 p anchoring at cell tips via a multistep and multimode mechanism.

121 temporal bifurcation responses in a passive multimode microresonator, with strongly coupled chaotic

122 e, we build chaotic states by perturbing the multimode microring resonators with densely packed silic

123 his paper describes the modifications to our multimode microscope imaging system [2,3], the acquisiti

124 The effects of multimode-microwave (MW), and low-frequency-ultrasound (

125 ptide mixture, in a 2-microL volume, using a multimode MS approach.

126 e results demonstrate the utility of using a multimode, multimethod approach (AFFQ and 24-hour dietar

127 am splitters is shown to provide a source of multimode N00N-type entanglement.

128 The multimode nature of the membrane and Fabry-Perot resonat

129 We demonstrate the potential of multimode NEMS-based mass spectrometry by analysing IgM

130 SSPs is derived analyt- ically by combining multimode network theory with rigorous mode matching met

131 Applying our theory to a multimode nonlinear cavity supporting cascaded nonlinear

132 ol over structured light fields for advanced multimode nonlinear photonics remains a grand challenge.

133 Recent experimental studies in heavily multimoded nonlinear optical systems have demonstrated t

134 strate the spatial self-cleaning of a highly multimode optical beam, in the process of second-harmoni

135 ments in laser-based technologies, including multimode optical communications, imaging, ultrafast lig

136 channels in PDMS and the encapsulation of a multimode optical fiber (100-microm core diameter) in th

137 n principle, this can be reduced to a single multimode optical fiber (MMF), the width of a human hair

138 indium tin oxide (ITO) overlaid section of a multimode optical fiber fused silica core.

139 that OAM modes can be (de)multiplexed over a multimode optical fiber with higher than -15 dB mode sel

140 Mode division multiplexing (MDM)- using a multimode optical fiber's N spatial modes as data channe

141 concept is applied to data transmission over multimode optical fiber, and the result is an optical mu

142 stered on a CCD camera), that emerges from a multimode optical fiber.

143 l end of a silanized 125 micrograms diameter multimode optical fiber.

144 Multimode optical fibers have recently reemerged as a vi

145 Multimode optical fibers represent the ideal platform fo

146 lications are generating a new assessment of multimode optical fibers to serve as high-speed fiber li

147 recent renewed interest in information-rich multimode optical fibers, we show that the multimode fib

148 ed by both chromatic and modal dispersion in multimode optical fibers.

149 utilizing disordered light within a standard multimode optical fibre for lensless microscopy and opti

150 n is based on a flexible fibre bundle of six multimode optical fibres, each terminated with a distal

151 sly used to remove the fundamental mode of a multimode optical structure while establishing global ph

152 Multimode optical switch is a key component of mode divi

153 e-designed surface-normal couplers to enable multimode optical transmission between separate silicon

154 physics and complexity of nonlinear, heavily multimoded optical systems, and could lead to highly tun

155 opening up the possibilities for integrated multimode optics.

156 re we study the dynamic properties of such a multimode optomechanical device, in which the coupling b

157 g the parametric phonon-phonon coupling in a multimode optomechanical system, where a low damping mec

158 e mode operation becomes unstable, signaling multimode oscillatory dynamics, (2) For a wide range of

159 ight transmitted through the object for each multimode pattern.

160 We show that distinct multimode patterns of light can be projected from the ou

161 truct the object using only the pre-measured multimode patterns themselves and the detector signals.

162 Interestingly, we also observed multimode phase locking with multiple whisks within a sn

163 as quantum information technologies such as multimode photon-by-photon switching.

164 Here, we demonstrate a multimode photonic computing core consisting of an array

165 a compact device footprint, the demonstrated multimode photonic core is promising toward large-scale

166 icant sensitivity enhancement in contrast to multimode planar silver halide waveguides.

167 The tunable multimode plasmonic resonances of these crystals and the

168 fabricated from coiled segments of low-cost multimode plastic-clad silica optical fibers.

169 er coupling effects in physically accessible multimode platforms.

170 latory and steady electric potentials, i.e., multimode potentials, that induce electrokinetic flows a

171 ising approach for developing long-lifetime, multimode quantum memories.

172 e, but lead to robust devices exhibiting new multimode resonances with characteristics that are inacc

173 loss-induced lasing, single-mode lasing from multimode resonators, and non-reciprocal effects in conj

174 Using multimode ridge waveguides, guided s-SWCNT photoluminesc

175 rating multiple sensing elements or adopting multimode sensing principles.

176 metric microlens array and was attached to a multimode silica fiber's tip during photopolymerization,

177 Here we demonstrate high-frequency multimode silicon carbide microdisk resonators and spati

178 cture based on a single-mode-tapered U-shape multimode-single-mode fiber probe is proposed and experi

179 d cloud condensation nuclei and parcel-based multimode size-resolving Lagrangian methods.

180 v/v%) and then purified by using ISOLUTE(R) multimode solid phase extraction.

181 leration can lead to relatively blue-shifted multimode solitons and blue-drifting dispersive wave com

182 Furthermore, we demonstrate frequency-multimode storage and memory-based spectral-temporal pho

183 er correlation functions, and characterize a multimode structure, which implies that several tens of

184 Here, using a multimode superconducting parametric cavity, we implemen

185 re, the conceptual principle of the proposed multimode switch can be reconfigurable and scalable in m

186 e introduce for the first time a novel 2 x 2 multimode switch design and demonstrate in the proof-of-

187 The multimode switch exhibits a low insertion loss and a low

188 tform for experimental realization of such a multimode switch.

189 we study nonlinear properties of finite-size multimode -symmetric couplers and predict the nonlinear

190 eas of attraction and rejection in nonlinear multimode systems of arbitrary dimension, which paves th

191 However, for multimode systems with higher-order EPs or multiple low-

192 to be tailored for advanced applications in multimode systems.

193 lity to spatially multiplex data channels in multimode systems.

194 studies, the complex nature of such heavily multimoded systems can be effectively exploited to obser

195 timode interference from leaky modes along a multimode tapered optical fibre, resulting in spectrally

196 ow, upconversion and downshifting to realize multimode time-dependent multicolour evolutions.

197 ng a multicore fibre (MCF) with an adiabatic multimode-to-single-mode "photonic lantern" transition f

198 plane the proposed antenna array operates as multimode transmitter (i.e., it provides broad-, uni- an

199 r QPCs with increasing aspect ratio are: (1) multimode transport in QPCs with larger channel width le

200 Here, we demonstrate multimode ultrastrong coupling between cavity modes of a

201 and introduce relevant figures of merit for multimode ultrastrong coupling.

202 the crucial role of spatial inhomogeneity in multimode ultrastrong coupling.

203 Here, we realize multimode ultrastrong light-matter coupling and theoreti

204 ually combined the DF with our multispecies, multimode version of the frequently used ligand-based co

205 n spectra provide information for developing multimode vibronic models of the excited-state structure

206 tion of an exemplary device: a low-crosstalk multimode waveguide bend.

207 of multiple transverse modes within a single multimode waveguide to achieve arbitrary spectral shapes

208 odulated modal power distribution (MPD) in a multimode waveguide.

209 ense counter-propagating beams interact in a multimode waveguide.

210 This is because multimode waveguides cannot be compactly routed on-chip

211 perty, finite-thickness slabs of h-BN act as multimode waveguides for the propagation of hyperbolic p

212 This work paves the way to efficient multimode wavelength-to-time mapping systems with the sp