ライフサイエンスコーパス: single mode

1 ional firing-rate vectors rapidly decay to a single mode.

2 uinoline was subsequently shown to bind in a single mode.

3 be described by the finite displacement of a single mode.

4 ilize around near-steady-state movement in a single mode.

5 han an order of magnitude larger compared to single-mode.

6 demonstrating low losses and densely packed single modes.

7 kewed and complex probability distributions (single mode, 10 cm, at 2100; two modes, 49 cm and 6 cm,

8 -subdomain conformational changes; second, a single mode 7 (for structure 1VOM) is found to dominate

9 However, these systems are constrained to single-mode actuation within a fixed structure under the

10 While we describe only a single mode and do not explicitly account for collective

11 can sustain switchable nanolasing between a single mode and multiple modes.

12 small mode volume, our LED is intrinsically single mode and, therefore, useful for communicating inf

13 Here, a new type of single-mode and self-powered mechanoreceptor that can mi

14 ing speed, can be well interpreted with this single-mode and self-powered mechanoreceptor.

15 The transmission system operates in singles mode and uses point sources of 137Cs that emit 6

16 designed to facilitate the propagation of a single mode at a wavelength of 10.3 microm emitted from

17 rs: the density of states in flow displays a single mode at another frequency scale omega(min) << ome

18 Because the PCFs used are single-mode at all wavelengths, the light always emerges

19 such vanishing four-terminal resistance in a single-mode ballistic quantum wire.

20 ting a mid-IR comb with an integrated mid-IR single mode based on distributed-feedback grating withou

21 ed with a waveguide width of 5 mum to ensure single mode behavior, avoiding optically undefined inter

22 nz 96 model, the ROMQG algorithm with just a single mode captures the transient response to random or

23 ntributions, though the effects in idealized single-mode cavities tend to diminish quickly as the tem

24 Two-level atoms ultrastrongly coupled with single-mode cavity photons are predicted to exhibit a qu

25 vskites to a nanoslot array functioning as a single-mode cavity.

26 2 relaxation distributions bifurcated from a single mode centered about approximately 650 ms into a f

27 ns compared to those from isolated storms or single-mode clustering.

28 , which combine the number fluctuations of a single-mode condensate state and competition between dif

29 ic selectivity of three-step excitation with single-mode continuous wave lasers results in measuremen

30 The system employs a compact doubled-diode single-mode continuous-wave laser operating at 488 nm an

31 a multicore fibre photonic lantern with 121 single-mode cores, coupled to 121 detectors on a 32 x 32

32 Magnetization precession was fitted with a single-mode damped sinusoid to extract the Gilbert dampi

33 d of applying optical sensors that only use "single-mode" detection, i.e., coordination of the metal

34 For monochromatic and single mode devices, high performance grating couplers h

35 The single-mode dispersive wave can therefore provide quiet

36 This represents the whole single-mode domain of commercially used fibers.

37 A highly sensitive single-mode EA-IOW device was used to optically follow t

38 Above all, we show here that OIS with single-mode EA-IOW's provide strong analytical signals t

39 ance spectroscopy (OIS) technique based on a single-mode electro-active-integrated optical waveguide

40 A single-mode, electroactive waveguiding platform capable

41 A quantum point contact was used to inject single-mode electrons into a mesoscopic electron beam sp

42 Compared with existing methods allowing single mode (electrophysiology or electrochemistry) reco

43 quality, achieving near-diffraction-limited single-mode emission with M(2) 1/e values maintained bel

44 These diffraction-limited single-mode emitters, ranging in size from 170 to 280 nm

45 with the output (approximately 417 nm) of a single-mode external cavity diode laser, which was conti

46 The spicules can function as single-mode, few-mode, or multimode fibers, with spines

47 vity) and a 4% Fresnel-reflecting facet of a single mode fiber (SMF).

48 ission of these high energy pulses through a single mode fiber into the microendoscope is a significa

49 embly transforms the propagating mode of the single mode fiber to match with the mode of a FFPC.

50 y the functionalization of LPGs inscribed in single mode fiber using two different methods of immobil

51 The technology used a single mode fiber with MgO-based nanoparticles doped cor

52 ed to conventional FFPCs coupled with just a single mode fiber, especially at long cavity lengths.

53 e can be matched with the mode of almost any single mode fiber, making this approach highly versatile

54 o-comb configuration, we demonstrate a 10 km single mode fiber, O-band, coherent, heterodyne, 12.1 Tb

55 fiber grating (Ex-TFG) inscribed in standard single mode fiber, we developed a novel label-free immun

56 The development of a single mode fiber-based pulsed laser with variable pulse

57 ore fiber (MCF) fusion spliced to a standard single mode fiber.

58 e core multimode fiber directly spliced to a single mode fiber.

59 The system is based on a single-mode fiber (about 18 m long) doped with Er3+ ion.

60 s type hollow-core fiber (NANF) and standard single-mode fiber (SMF).

61 ed artificial Rayleigh scattering centers in single-mode fiber cores.

62 d the fundamental limits of current standard single-mode fiber networks.

63 d on a single-mode-tapered U-shape multimode-single-mode fiber probe is proposed and experimentally d

64 ugh the use of a long, adiabatically tapered single-mode fiber probe.

65 ~0.6 dB Q improvement after 2800 km standard single-mode fiber transmission using 32 Gbaud signal.

66 gh the chromatic dispersion of a meter-scale single-mode fiber used for endoscopic applications is ne

67 30 GBd 1000 km transmission over a standard single-mode fiber, and demonstrate that it is feasible t

68 ic diffractive metalens on the end face of a single-mode fiber, capable of performing achromatic and

69 As current single-mode fiber-based transmission systems are reachin

70 nabled the telecommunication revolution, but single-mode fiber-optic communication systems have been

71 tomic Layer Deposition (ALD) on the tip of a single-mode fiber.

72 ments of MCF are sandwiched between standard single mode fibers.

73 structed using a simple device incorporating single-mode fibers (SMFs) and a segment of a multicore f

74 gher than is supported by currently deployed single-mode fibers, paving the way for next-generation u

75 The diode heads were coupled directly to single-mode fibers, which were terminated into a single

76 and interfaced with polarization-maintaining single-mode fibers.

77 ing optical nonlinearities are restricted to single-mode fibers.

78 mplanting rare earth ions into the core of a single mode fibre.

79 on in a setting that is intermediate between single-mode fibre and free-space propagation.

80 phenomenon is most cleanly observed using a single-mode fibre transmission line, where spatial mode

81 ow spectral response ranges and operate in a single mode (for example, non-volatility), limiting thei

82 Landauer theory as well as the conventional single-mode Franck-Condon model.

83 order spin-wave modes, thus stabilizing the single-mode generation regime.

84 erpositions of distinct coherent states in a single-mode harmonic oscillator, known as "cat states,"

85 ble-wavelength light at lambda = 674 nm from single-mode, high index-contrast dielectric waveguides t

86 tripping allow for the identification of the single mode in the spectrograms and the determination of

87 e V(V) distribution characterized by a major single mode in the ultrafine (<0.25 mum) size range and

88 dings; instead, their focus was on inferring single, mode-independent social interaction rules that r

89 , we explore a model S(N)2 reaction within a single-mode infrared resonator.

90 py allowed interpretations not possible from single-mode investigations.

91 e that a surface emitting laser that remains single mode irrespective of its size, a scale-invariant

92 We demonstrate an electrically pumped, single-mode, large area, edge-emitting InGaAsP/InP two-d

93 We have demonstrated stable single mode laser output with side-mode suppression of o

94 lti-mode laser and negligible mode shifts in single-mode laser are clearly observed.

95 Even when pumped by a single-mode laser, the signal and idler photons are typi

96 ns contribute significantly to the design of single mode lasers, coherent perfect absorbers, isolator

97 low linewidth, high output power, integrated single mode lasers, that operate from the visible to sho

98 the beating note of two frequency-stabilized single-mode lasers to generate an asymmetric time-period

99 Single mode lasing was achieved for a large area laser,

100 Single-mode lasing at 1,554.148 nm with a sidemode suppr

101 A single-mode lasing from a coupled-ring resonator system

102 rectional invisibility, loss-induced lasing, single-mode lasing from multimode resonators, and non-re

103 We obtain single-mode lasing in the blue-violet spectral region wi

104 A suitable physical mechanism that allows single-mode lasing irrespective of the cavity size-a 'sc

105 rity-time microring laser exhibits intrinsic single-mode lasing regardless of the gain spectral bandw

106 ng of losses in reciprocal space, leading to single-mode lasing that is maintained as the cavity is s

107 mode control, to achieve wavelength-tunable single-mode lasing with an improved mode suppression rat

108 rcome minimized optical losses, resulting in single-mode lasing with an ultralow threshold of ~5.3 ki

109 reduce the number of cavity modes to achieve single-mode lasing.

110 nit cells in the cavity in phase, leading to single-mode lasing.

111 es, such as free spectral range doubling and single-mode lasing.

112 Deforming along a single mode leads to most successful predictions.

113 measure electron-phonon interactions at the single-mode level, especially their effect on phonon tra

114 ctivity and affinity compared to traditional single-mode ligands.

115 Photonic crystals are etched into single mode low refractive index SiON film on both SiO2/

116 of the lantern by individually exciting the single-mode MCF cores, and that these patterns are highl

117 ination of accurate reaction temperatures in single-mode microwave reactors are discussed.

118 In particular the introduction of benchtop single-mode microwave reactors just over ten years ago h

119 the variation in local diffusivity, while a single-mode model does not.

120 rate that photonic lanterns based on tapered single-mode multicore fibres provide an efficient way to

121 mall changes in position and momentum with a single-mode multiparameter sensor.

122 V) centers placed in two spatially separated single-mode nanocavities inside a planar photonic crysta

123 we demonstrate a microring laser producing a single-mode OAM vortex lasing with the ability to precis

124 ition frequency in a trapped Mg+ ion using a single mode of a UV frequency comb.

125 es is an example of how unrelenting use of a single mode of action herbicide in agricultural weed con

126 However, those studies have not yielded a single mode of action.

127 ive cytotoxic agent than an inhibitor with a single mode of action.

128 Together, these data show that a single mode of activation endows macrophages with the ab

129 cal processes that cannot be inferred with a single mode of assay, the integration of very large, com

130 ic 3,6-diphenyl-1,2,4,5-tetrazine, display a single mode of cycloaddition with reaction only across C

131 However, most approaches are limited to a single mode of data, leaving integrated approaches acros

132 genotype-phenotype mapping are limited to a single mode of genomic alteration, i.e. overexpression,

133 In contrast to this single mode of killing of protozoa, we have recently pro

134 by treating it as a bipartite one between a single mode of phonons and a single photon.

135 A single mode of recognition for these two classes of liga

136 is partitioned into distinct regions where a single mode of response (reversible phenotypic plasticit

137 Because the results did not implicate a single mode of transmission, the possibility of multiple

138 nciple a second threshold exists after which single mode operation becomes unstable, signaling multim

139 , (2) For a wide range of design parameters, single mode operation of PT lasers having relatively lar

140 ely suppressed using lithographic tuning and single mode operation of the multi-mode laser is enforce

141 ser frequency content between multi-mode and single mode operation.

142 ur findings shine light on the robustness of single-mode operation against saturation nonlinearity in

143 l in a laser cavity is critical for a stable single-mode operation of a ring laser.

144 perimental characterization indicates stable single-mode operation over a wide injection current rang

145 fforts to scale-up cavities while preserving single-mode operation since the invention of the laser s

146 mped InAs/GaAs quantum-dot PC lasers exhibit single-mode operation with an ultra-low threshold of ~0.

147 tionally symmetric structure leads to stable single-mode operation with the selective whispering-gall

148 The wires allow single-mode operation, and have an optical loss of less

149 ovel design of Si3N4 microresonator in which single-mode operation, high quality factor, and anomalou

150 he nanopillar array band-edge lasers exhibit single-mode operation, where the mode frequency is sensi

151 when the waveguiding effect is optimized to single-mode operation.

152 and lasers with reversed pump dependence or single-mode operation.

153 The measurement head was made of a single mode optical fiber with a microsphere structure c

154 ransmission capacity N-times with respect to single mode optical fibers.

155 Our MCF is designed to mode match a standard single mode optical fibre.

156 implify the detection setup by using a long, single-mode optical fiber and a fast photodiode.

157 iber Bragg grating (eTFBG) is developed on a single-mode optical fiber targeting biomolecule detectio

158 on light is conducted to the microscope in a single-mode optical fiber, and images are scanned using

159 eflector (DBR) gratings on the end-face of a single-mode optical fiber.

160 This self-recovery is demonstrated on single-mode optical fibers with 80 microns diameter (3.1

161 In single-mode optical fibers, Rayleigh scattering serves a

162 mpatible silicon-on-insulator technology and single-mode optical fibre.

163 isolation found in the homogeneous core of a single-mode optical fibre.

164 ance in both cases is provided by the use of single-mode optical fibres.

165 e use cold (87)Rb atoms in the vicinity of a single-mode optical nanofiber (ONF) that coherently exch

166 effect, both the magnon modes are coupled to single-mode optical WGM through nonlinear interaction.

167 The single-mode optode can be used for 30,000 measurements w

168 systemic antimicrobial agents, having only a single mode or site of action, will not alleviate the si

169 optical microscopy (s-SNOM), using either a single-mode or a frequency comb THz quantum cascade lase

170 ar process, but these were mostly limited to single-mode or few-mode fiber amplifiers, which have goo

171 ve via currently existing methods, including single-mode output (only voltage signal), greatly simpli

172 Moving out of the single-mode paradigm, we show experimentally that wavefr

173 Single mode peak power up to 6.7 W is demonstrated with

174 This single-mode perovskite laser reaches a low threshold ( a

175 Here, we demonstrate a single-mode phase estimation that approaches the Heisenb

176 Single-mode photodynamic therapy (PDT) based on photoche

177 frequency up-converted, electrically driven, single-mode photonic sources in the 9.0-10.5 THz range,

178 Here we integrate T centres into single-mode photonic waveguides in a silicon-on-insulato

179 e fibre (MCF) with an adiabatic multimode-to-single-mode "photonic lantern" transition formed at the

180 uated total reflection element consists of a single-mode, planar integrated optical waveguide fabrica

181 Single-mode plans were much more often confirmed: system

182 ur scheme, we exploit the birefringence in a single-mode polarization maintaining fiber in order to m

183 Here we present the first single-moded, polarization-maintaining HCF with large co

184 ance peaks, impressive results exceeding the single-mode prediction are produced from a very modest q

185 are designed with appropriate dimensions for single-mode propagation at 1550 nm.

186 aveguides for blue light to date: we achieve single-mode propagation losses of 0.8 dB/cm at a propaga

187 t the entire range in which the waveguide is single mode, providing a sensitive and broadband method

188 We study particle and spin transport in a single-mode quantum point contact, using a charge neutra

189 Our channel correction for single-mode quantum states will find use in quantum repe

190 een each pair of terminals and access to the single-mode regime coexistent with the presence of super

191 egrated photonics operate exclusively in the single-mode regime.

192 continues to operate almost strictly in the single-mode regime.

193 two or more two-level systems (qubits) in a single-mode resonator has recently been theoretically pr

194 nsisting of a two level qubit coupled with a single-mode resonator in arbitrary coupling strength reg

195 is approach, we show that both multimode and single-mode rhombohedral-stacked MoS(2) waveguides suppo

196 ely heated reactor is compared to a standard single-mode sealed-vessel microwave instrument with resp

197 lecom band around 1.55 mum, achieved using a single-mode silicon resonator with Q of 10(6).

198 Their ultra-low thresholds and single-mode, single-exciton emission make these hybrid l

199 Results show that aerosol Fe had a single-mode size distribution, peaking at 4.4 um in diam

200 isons between FM pre-amplified receivers and single-mode (SM) pre-amplified receivers with or without

201 Here we demonstrate single-exciton, single-mode, spectrally tuned lasing from ensembles of o

202 he same photon flux, they can outperform the single mode squeezed vacuum state.

203 the interplay between Kerr nonlinearity and single-mode squeezing(1,3) in a superconducting microwav

204 y proposing a single mode-tapered seven core-single mode (STSS) fiber ring laser (FRL) biosensor for

205 ing systems with the spectral performance of single-mode systems.

206 addresses this critical issue by proposing a single mode-tapered seven core-single mode (STSS) fiber

207 nanonewton force sensor structure based on a single-mode-tapered U-shape multimode-single-mode fiber

208 ities are demonstrated in a single strand of single-mode telecommunication fibre, using a setup consi

209 Two modes of exocytosis were identified: a single mode that leads to release of the contents of ind

210 zed states of a disordered optical fibre are single mode: the transmission channels possess a high de

211 Consequently, single-mode therapies fail to comprehensively ameliorate

212 ated multi-mode thermal state instead of the single-mode thermal state of the same energy.

213 is highly efficient design, continuous wave, single mode THz emissions with a wide frequency tuning r

214 The TEM quasi-single mode THz waveguide excitation and non-dispersive

215 photonic design forcing the emitter and cell single modes to cros resonantly couple and impedance-mat

216 s identification and characterization of the single-mode transmission channels in a disordered matrix

217 Single-mode vacuum waveguides have a multitude of potent

218 While electrode engineering and single-mode voltammetry enabled detection of sub-micromo

219 to >60-fold and >120-fold improvements over single-mode voltammetry.

220 e climate modes, more than the effect of any single mode, was associated with large fluctuations in p

221 The sensor generated a single-moded waveguide signal with a RI sensitivity of 1

222 novel microresonator is consisted of uniform single-mode waveguides in the semi-circle region, to eli

223 mplitudes of an array of spatially separated single-mode waveguides.

224 s capability, we demonstrate the multiplexed single-mode wavelength-to-time mapping of multimode ligh

225 The waveguide can be designed to support a single mode whose properties are very similar to the uni

226 a plasmonic gap waveguide is directed into a single mode with >99% efficiency.