ライフサイエンスコーパス: interferometer

1 ven after the photon has already entered the interferometer.

2 the enabler of non-classical dynamics in an interferometer.

3 using a conventional x-ray tube and grating interferometer.

4 turn in living gerbil cochleae using a laser interferometer.

5 the bR adlayer over one or both arms of the interferometer.

6 iliary motions with a dual-beam differential interferometer.

7 ins deterministically via a modified Franson interferometer.

8 r with a nearly shot-noise limited microwave interferometer.

9 e passes of the e/4 quasiparticle around the interferometer.

10 from two longitudinal locations with a laser interferometer.

11 vidual atoms are detected using a novel atom interferometer.

12 that can be used as a terahertz Mach-Zehnder interferometer.

13 sitive gerbil cochlea using a scanning laser interferometer.

14 in terms of Fabry-Perot modes in an electron interferometer.

15 is applied with a dual-beam optical trapping interferometer.

16 cochlea using a displacement-sensitive laser interferometer.

17 tected using a photorefractive crystal-based interferometer.

18 molecular size in our time-domain Talbot-Lau interferometer.

19 d cylindrical magnetic shield of a cold atom interferometer.

20 ulses into a 14-micrometer-long Mach-Zehnder interferometer.

21 nction by means of a superconducting quantum interferometer.

22 ay facilitated on porous silicon Fabry-Perot interferometer.

23 ual photons within a temporal linear optical interferometer.

24 e experiments with quantum point contact and interferometer.

25 n be determined in operando in a Fabry-Perot interferometer.

26 trol exceeding 10n radians in a Mach-Zehnder interferometer.

27 a proper choice of the scan interval of the interferometer.

28 -all Ising-like interaction in a matter-wave interferometer.

29 ectively forming an interlayer Aharonov-Bohm interferometer.

30 rved and evaluated in a table-top Talbot-Lau-Interferometer.

31 frequency shifts introduced from a Michelson interferometer.

32 two dimensions and a vector atomic Michelson interferometer.

33 InAs-Al island embedded in an Aharonov-Bohm interferometer.

34 a magnetic field sensor based on a spin wave interferometer.

35 brid (SOH) slot waveguide based Mach-Zehnder interferometer.

36 smear statistical photon bunching in the HOM interferometer.

37 he repeatability of a commercially available interferometer.

38 s, such as common- and double path waveguide interferometers.

39 ase contrast than current near-field grating interferometers.

40 ent, most sensitive methods based on crystal interferometers.

41 background, or later with direct space-based interferometers.

42 year could be detected by gravitational wave interferometers.

43 ravity models, could be detected using laser interferometers.

44 d via the propagating states of Mach-Zehnder interferometers.

45 entanglement is performed using fiber-based interferometers.

46 create gyroscopes and rotational matter-wave interferometers.

47 ctron-channel plasmon eigenstates in quantum interferometers.

48 eters, superconducting gravimeters, and atom interferometers.

49 enhancing the sensitivity of molecular-scale interferometers.

50 n is central for modern atomic clocks(1) and interferometers(2).

51 optical and near-infrared or (sub)millimetre interferometers(3,4).

52 e Hamiltonian simulators(4,5) and chip-scale interferometers(6).

53 ploring quantum entanglement in the two-mode interferometers, a single bosonic mode also promises a m

54 The extreme miniaturization of a cold-atom interferometer accelerometer requires the development of

55 reading out the signal of Fabry-Perot based interferometers acting as biotransducers.

56 GO) film is deposited on a fiber-optic modal interferometer, acting as both the fluorescent quencher

57 sured with a radial shearing speckle pattern interferometer after an increase in intraocular pressure

58 Deployment of ultracold atom interferometers (AI) into space will capitalize on quant

59 icroscopic examination of the fundus, an OCT interferometer, an OCT beam delivery system designed for

60 ter Gravitational-Wave Observatory and Virgo Interferometers, an associated optical transient, SSS17a

61 citation spectra using a compact common-path interferometer and broadband excitation, which is implem

62 specialized imaging system, combining Sagnac interferometer and CCD camera images to reconstruct spec

63 spectrometer assembly, employing a step-scan interferometer and focal plane array detector, is analyz

64 The combination of our sensitive interferometer and nonresonant transmission line provide

65 d neutrons through a perfect silicon crystal interferometer and perform weak measurements to probe th

66 conditional quantum gates in a Mach-Zehnder interferometer and report a proof-of-principle experimen

67 y comb to self-reference a Ramsey-Borde atom interferometer and synchronize an oscillator at a subhar

68 Using a Mach-Zehnder interferometer and time-delayed femtosecond laser pulses

69 e the gravitational sensitivity of a lattice interferometer and use a system of signal inversions to

70 xperimental data sets from a neutron grating interferometer and we have obtained improved images both

71 The devices act as graphene Fabry-Perot interferometers and allow for direct probing of the tran

72 f photonic components including Mach-Zehnder interferometers and lattice filters, and for waveguide i

73 ny components, such as waveguides, couplers, interferometers and modulators, could be directly integr

74 se a miniaturised version of beam-splitters, interferometers and optical cavities for light propagati

75 ems, leading to the construction of electron interferometers and proposals for low-power electronics

76 mple, quantum point contacts (QPC), electron interferometers and quantum dots.

77 Photonic circuits including interferometers and resonators have been transferred ont

78 , a fully general and programmable four-mode interferometer, and photon number-resolving readout on a

79 rinciples underlying future planet-searching interferometers, and our laboratory instrument will serv

80 Mach-Zehnder interferometer- and ring resonator-based wavelength demu

81 These results can be used in grating interferometer applications which uses phase stepping me

82 The reflectivity signals of each interferometer are amplified by biochemical reaction pro

83 Two kinds of multidimensional atom interferometers are demonstrated that are capable of mea

84 Interferometers are essential tools for measuring and sh

85 ltaOT(eff)) of PEI-GA-PEI-functionalized NAA interferometers are monitored in real-time by RIfS, and

86 Atom interferometers are powerful tools for both measurements

87 Atom interferometers are powerful tools for investigating, fo

88 Our results show that interferometers are sensitive probes of microscopic inte

89 Two adjacent porous Si Fabry-Perot interferometers are simultaneously utilized to quantify

90 These interferometers are widely used for precision measuremen

91 Deflections of each interferometer arm due to the source mass are independen

92 s forming a Mach-Zehnder interferometer with interferometer arms electrically poled in opposite direc

93 ng an integrated cavity-coupled Mach-Zehnder interferometer as a frequency noise discriminator.

94 cted from an integrated optical Mach-Zehnder interferometer as a passive structure, covered by a bact

95 n electronically reconfigurable Mach-Zehnder interferometer as the frequency reference to reduce the

96 c frequency (CF) tones were measured with an interferometer at up to 15 locations across the basilar

97 demonstrate a fully magnonic Gires-Tournois interferometer based on a subwavelength resonator made o

98 Here we report a far-field, two-arm interferometer based on the new nanometric phase grating

99 erated by using a highly sensitive microwave interferometer-based detection circuit.

100 ceed the performance of tabletop grating and interferometer-based devices.

101 A differential interferometer-based microcantilever sensor was develope

102 CCD and a BBCEAS coupled with a Fabry-Perot interferometer (BBCEAS-FP).

103 ed signal to a short XRL amplifier and as an interferometer beam to measure two-dimensional local gai

104 We report here the application of a photonic interferometer biosensor based on a bimodal waveguide (B

105 Integrated planar optical waveguide interferometer biosensors are advantageous combinations

106 es about integrated planar optical waveguide interferometer biosensors can mostly be found in the lit

107 These interferometers, built from ultracold Bose-Einstein cond

108 e localized states of electronic Fabry-Perot interferometers, but almost no quantum interference when

109 l interferograms, namely IAW, obtained on PS interferometer by subtraction (wavelength by wavelength)

110 Millimetre interferometers can probe this stage but only for the co

111 free-solution assay (FSA) and a compensated interferometer (CI) can provide a novel alternative to e

112 y training methods for programmable photonic interferometer circuits, a leading analog NN platform, d

113 mber of quantum technologies, including atom interferometers, clocks, Rydberg atoms, and hybrid atom-

114 The interferometer combines the benefits of both a double-pa

115 trument, based on a common-path birefringent interferometer, combines high spatial (~1 mum) and spect

116 ify this finding, we propose an astronomical interferometer composed of satellites with the tailored

117 The interferometer consists of two 45-nm-thick silicon layer

118 o by passing single photons through a Sagnac interferometer containing both a metamaterial with a neg

119 Here we describe the Degree Angular Scale Interferometer (DASI), an array of radio telescopes, whi

120 ion of the CMB with the Degree Angular Scale Interferometer (DASI).

121 modalities were performed using a step-scan interferometer, demonstrating improved spectral range (5

122 The instrument is based on an interferometer design in which illumination patterns are

123 Here we present an X-ray interferometer design that is practical for adaptation t

124 Here we use a small-area edge state interferometer designed to observe quasiparticle interfe

125 tic vibrometer based on a modified Michelson interferometer, designed to serve as a middle-ear microp

126 usly encodes the metasurface-based multiport interferometer designs and its resulting nonclassical co

127 tional-Wave Observatory (LIGO) and the Virgo interferometer detected gravitational waves (GWs) emanat

128 implementation of a dual-phase X-ray grating interferometer (DP-XGI) for DF imaging in a lab-based se

129 n integrated device containing three coupled interferometers, eight spatial modes and many classical

130 Quantum Hall interferometers enable direct observation of the anyon b

131 Furthermore, a near common-path interferometer enables quantifying nanometer-scale membr

132 We demonstrate the interferometer for a graphene-type hexagonal optical lat

133 ailor and co-workers (1997) on the use of PS interferometer for biosensing, and lowers of 4 orders of

134 o introduce and realize an enantio-sensitive interferometer for efficient chiral recognition without

135 how how this setup may be used to realize an interferometer for macroscopic objects doped with a sing

136 the realization of a full-loop Stern-Gerlach interferometer for single atoms and use the acquired und

137 act devices and lead to portable guided-atom interferometers for applications such as inertial naviga

138 res as a versatile alternative to GaAs-based interferometers for future experiments targeting anyonic

139 ential limitations of the use of porous SiO2 interferometers for quantitative determination of protei

140 Finally, the analytical performances of both interferometers for real-life scenarios are confirmed us

141 developed arrayed nanostructured Fabry-Perot interferometer (FPI) microchips.

142 r, theoretical model of cascaded Fabry-Perot interferometer (FPI) with thin film based on Vernier eff

143 channel recording of the OCT and calibration interferometer fringe signals, as well as sweep to sweep

144 twin extreme UV pulses to create a molecular interferometer from direct and sequential two-photon ion

145 depolarization effect detected by the Sagnac interferometer further confirms its nematic nature.

146 Conventional Mach-Zehnder interferometers generate sinusoidal output intensities,

147 ing blocks, which permit composing arbitrary interferometer geometries in a digital manner.

148 s for atomic clocks, quantum gates, and atom interferometer gravimeters.

149 ll soon be observed and studied by the Laser Interferometer Gravitational Wave Observatory and its in

150 On 17 August 2017, the Laser Interferometer Gravitational-Wave Observatory (LIGO) and

151 of gravitational waves by the Advanced Laser Interferometer Gravitational-Wave Observatory (LIGO) det

152 spectrogram images and labels) of the Laser Interferometer Gravitational-wave Observatory (LIGO) fir

153 rrelation is naturally produced in the Laser Interferometer Gravitational-wave Observatory (LIGO).

154 vitational wave source GW170817 by the Laser Interferometer Gravitational-Wave Observatory and Virgo

155 -mass binary black hole mergers by the Laser Interferometer Gravitational-wave Observatory opened the

156 Quantum Hall interferometers have been used to probe fractional charg

157 Thus, lattice interferometers have yet to be used for precision tests

158 Our prototype interferometer, having just under one millimetre of base

159 he present experiment using a scanning-laser interferometer, I detected forward-traveling but not bac

160 Agency's (ESA) Infrared Atmospheric Sounding Interferometer (IASI) and CAFO animal unit density in 20

161 tions from the infrared atmospheric sounding interferometer (IASI).

162 ing instrument to be implemented on the Keck interferometer in 2001.

163 and simultaneously with a modified spectral interferometer in 30 healthy subjects with two different

164 Here we report a matter-wave interferometer in a cavity quantum-electrodynamics syste

165 r, self-aligned, amplitude-division electron interferometer in a conventional transmission electron m

166 ere we used a high-precision, GHz-ultrasonic interferometer in conjunction with a newly developed opt

167 thod by using a thermal-stabilized reference interferometer in conjunction with an ultrahigh-Q microc

168 y and defects on the quality of a Talbot-Lau interferometer in terms of visibility and absorption cap

169 The good performance of the interferometer in the low energy range (LER) is demonstr

170 Here we study a new type of interferometer in which the beam splitting and recombina

171 be overcome by using a dual-aperture stellar interferometer in which the starlight is cancelled, or '

172 tes are vital to exploring gravity with atom interferometers in greater detail.

173 FT-IR microimaging employing continuous scan interferometers in which the advantages of fast image co

174 a semiconductor laser using a laser-feedback interferometer, in which the terminal voltage of the las

175 of the end test masses of gravitational wave interferometers, in which the room temperature internal

176 ersion, a carefully optimized linear optical interferometer including beam splitters with variable re

177 the space of Laguerre-Gaussian modes, and an interferometer incorporating such a 'delay' obtains moda

178 t the successful integration of a Talbot-Lau interferometer into a clinical CT gantry and present dar

179 l studies have explained why a Stern-Gerlach interferometer is a formidable challenge.

180 The modulated phase grating (MPG) interferometer is a recently developed grating interfero

181 The interferometer is constructed from a sequence of discret

182 This interferometer is fabricated from a single-crystal silic

183 The interferometer is formed by tunnel-coupling the proximit

184 The interferometer is locked to its quadrature point (QP) fo

185 As the interferometer is naturally operated at cryogenic temper

186 In this condition, conductance through the interferometer is observed to oscillate in a perpendicul

187 A Mach-Zehnder interferometer is used for the homodyne detection.

188 An important advantage of our MCF interferometers is their capability to operate at very h

189 Two-mode interferometers lay the foundations for quantum metrolog

190 in twenty Asian subjects (20 eyes) using an interferometer (LipiView(R) ocular surface interferomete

191 most complex component of a light-pulse atom interferometer (LPAI), controlling frequencies and inten

192 We report the use of in-line incoherent interferometers made from uniaxial birefringent alpha-ba

193 energy gap also emerges, effectively binding interferometer matter-wave packets together to suppress

194 significance of LLT changes measured by this interferometer may be better interpreted.

195 ation of radio frequency time-of-arrival and interferometer measurements, we observed a sequence of l

196 optically encoded inputs using Mach-Zehnder interferometer mesh networks interleaved with nonlineari

197 s of magnitude smaller than state-of-the-art interferometer meshes.

198 The detector is based on a tunable microwave interferometer (MIM) with a vector network analyzer (VNA

199 Here, we present the Mach-Zehnder interferometer-miRNA detection system capable of detecti

200 microring resonator (MRR) and a Mach-Zehnder interferometer (MZI) based on a silicon nitride platform

201 The spectrometer is based on a Mach-Zehnder interferometer (MZI) employing a He-Ne laser, a mini-flo

202 rd tunable photonic coupler-the Mach-Zehnder interferometer (MZI)-cannot be perfectly programmed to t

203 such as resonant modulators and Mach-Zehnder interferometers (MZIs), and are highly sensitive to fabr

204 of mid-infrared (MIR; 3-12 mum) Mach-Zehnder interferometers (MZIs).

205 Using a cesium matter-wave interferometer near a spherical mass in an ultrahigh-vac

206 first report of a Talbot-Lau neutron grating interferometer (nTLI) with inverse geometry.

207 ed using a direct measurement (by an optical interferometer) of its changes in diameter as it pulsate

208 refractometric detection using the Rayleigh interferometer offers a key advantage for providing accu

209 system and the incorporation of the Rayleigh interferometer onto the ultracentrifuge that had the gre

210 different waves and form new types of hybrid interferometers, opening a door for many applications in

211 Current bench-top interferometers operate in the near field with limitatio

212 rgeted in the current literature) using a PS interferometer operating in label-free mode without any

213 Here we present an atom interferometer operating with single trapped atoms, wher

214 modulation (for example, using Mach-Zehnder interferometers or ring resonators).

215 tors use nonreciprocal phase shift (NRPS) in interferometers or ring resonators, but to date NRPS req

216 a recently proposed nanoparticle matter-wave interferometer, originally conceived for tests of the qu

217 provide the correspondence between expected interferometer output signals and gravity models.

218 maging, it enables a polychromatic far-field interferometer (PFI) without absorption gratings.

219 ce model, encompassing the description of an interferometer phase probed with relevant quantum states

220 vertical separation generate megaradians of interferometer phase.

221 Interferometers probe the wave-nature and exchange stati

222 e technique for shot noise suppression, this interferometer promises further improvement in sensitivi

223 The interferometer provided maps 300 kilometers by 1000 kilo

224 It makes use of the fact that an X-ray interferometer provides a conventional absorption as wel

225 Here, we demonstrate that a clock interferometer provides metrological improvement compare

226 Such quantum Hall interferometers (QHIs) can unveil the exchange statistic

227 We numerically study a matter wave interferometer realized by splitting a trapped Bose-Eins

228 rvation of phase jumps in a Fabry-Perot (FP) interferometer revealed anyonic quasiparticle exchange s

229 ell with two embedded channels placed in the interferometer's arms, and a tunable external cavity qua

230 r of the outputs and their dependence on the interferometer's length.

231 -polariton condensate and employ a Michelson interferometer setup to characterize the short- and long

232 The interferometer setup with its lenses is included rigorou

233 onalized prGO film coated on the fiber-optic interferometer shows high sensitivities for the detectio

234 our device is near the quantum limit for the interferometer size and quantum detection efficiency of

235 been enabled by the introduction of grating interferometers so far.

236 d if it is a stellar-mass orbiter, the Laser Interferometer Space Antenna (LISA) should detect its lo

237 The upcoming Laser Interferometer Space Antenna(2) (LISA) is expected to de

238 re derived from Atmospheric Emitted Radiance Interferometer spectra together with ancillary measureme

239 approach employing waveguides and multi-mode interferometer splitters to optically address multiple (

240 In bosonic interferometers, squeezed states(3), number states(4,5)

241 novel technologies and architectures for the interferometer subsystems.

242 Analysis of our velocity interferometer system for any reflector (VISAR) results

243 n interferometer (LipiView(R) ocular surface interferometer, TearScience Inc, Morrisville, NC).

244 , chip-based implementation of a double-beam interferometer that can separate biomolecules based on s

245 urces, these events must be observed with an interferometer that has sufficient spatial resolution fo

246 mentum space, in analogy to an Aharonov-Bohm interferometer that measures magnetic flux in real space

247 The system utilizes a Common-Path-Interferometer to detect X-ray-induced phase shifts of t

248 Here we use a scanning laser interferometer to determine the volume displacement and

249 We realize an atomic interferometer to measure Berry flux in momentum space,

250 We have used a laser-diode interferometer to measure in vivo the distribution along

251 e use a highly tunable graphene-based QHE FP interferometer to observe the connection between interfe

252 We develop an interferometer to prove entanglement of these distinguis

253 scope, which is converted into a Linnik-type interferometer to sequentially acquire both superresolve

254 nsional polarization-sensitive time-scanning interferometer to the laser, multidimensional spatiotemp

255 nique has not been implemented using optical interferometers to date.

256 -to-noise ratio compared with a conventional interferometer under the same operating condition, which

257 The second is a high-resolution Michelson interferometer used as a phase-sensitive reflection-type

258 Implementing this device as a Michelson-type interferometer using the coherent nature of the dynamic

259 hown experimentally to be a robust spin wave interferometer using the forward volume mode, with a lar

260 nstrated improved measurement precision over interferometers using coherent states(6,7).

261 of magnitude DL attained with label-free PS interferometers using conventional effective optical thi

262 ce, it is essential to demonstrate spin wave interferometers using spatially isotropic spin waves wit

263 Electronic interferometers using the chiral, one-dimensional (1D) e

264 Conventional interferometers usually utilize beam splitters for wave

265 icroscopy and image analysis, a Mach-Zehnder interferometer was constructed in which one of two inter

266 The interferometer was developed to operate at two different

267 A three-pulse Mach-Zehnder interferometer was studied to understand the influence o

268 In addition, a packaged MCF interferometer was transferred into field trials to vali

269 use nonlinear processes are involved in this interferometer, we can couple a variety of different wav

270 sing a custom-built heterodyne low-coherence interferometer, we demonstrate in living mouse cochleae

271 the cochlear partition using a custom-built interferometer, we demonstrate that electrical stimulati

272 Depending on the operating point of the interferometer, we demonstrated binary and ternary logic

273 e spatial-light-modulator-based polarization-interferometer, we have constructed a 'Hilbert-space ana

274 nt technique based on a scanning Fabry-Perot interferometer, we observe long-living narrowband compon

275 Using this interferometer, we obtain interference fringes in a Mach

276 For the Michelson interferometer, we perform Bayesian inferencing from a 4

277 ers into subwavelength cavities of plasmonic interferometers, we demonstrate coherent generation of s

278 scopes and a prototype of a lateral shearing interferometer were used for the measurements.

279 Our MCF interferometers were used for sensing strain.

280 o arms comparable to an imbalanced Michelson interferometer, where one arm is significantly longer th

281 le lung imaging system based on a dual-phase interferometer, which allows tuning and direct resolutio

282 s in ballistic trilayer graphene Fabry-Perot interferometers, which result from phase coherent transp

283 Matter-wave interferometers, which split and recombine wave packets

284 This allows us to fabricate simple MCF interferometers whose interrogation is carried out with

285 Here we propose an interferometer with a levitated, optically cooled and th

286 contrast CT setup consisting of a Talbot-Lau interferometer with a rotating anode x-ray tube and a si

287 Employing an interferometer with a Sagnac-like ring design, we succes

288 The system combines Mach-Zehnder interferometer with a spectral imaging system for captur

289 ak value device over a standard Mach-Zehnder interferometer with equal detected optical power, as wel

290 te optical waveguides forming a Mach-Zehnder interferometer with interferometer arms electrically pol

291 e general physical model of the Mach-Zehnder interferometer with photon loss which is a fundamental p

292 The first is an interferometer with recoiling mirrors.

293 were performed by using a Talbot-Lau grating interferometer with the beam direction in anterior-poste

294 tronomy Observatory's Very Large Array radio interferometer with the Very Long Baseline Array antenna

295 tem consists of a cascade of 15 Mach-Zehnder interferometers with 30 thermo-optic phase shifters inte

296 Our approach applies to interferometers with arm cavities, such as the km-long L

297 Recently, interferometers with atoms suspended for 70 s in an opti

298 of a hexagonal mesh of silicon Mach-Zehnder interferometers with phase shifters.

299 EI)-modified nanoporous anodic alumina (NAA) interferometers with reflectometric interference spectro

300 erfect absorber," functions as an absorptive interferometer, with potential practical applications in