ライフサイエンスコーパス: broadband

1 ed terahertz time-domain spectrometer with a broadband (0.3-2.5 THz), rotatable THz polarization stat

2 d and experimentally demonstrated a compact, broadband 1 x 3 power splitter on a silicon photonics pl

3 ond coupling constants, without the need for broadband (13)C decoupling.

4 etween 30 Hz and 80 Hz), and another that is broadband[3].

5 The broadband absorbance of samples (RGB-resolved absorbance

6 obtaining a resonant and dynamically tunable broadband absorber based on vanadium dioxide (VO2) phase

7 Broadband absorbers are essential components of many lig

8 This is not possible with traditional broadband-absorbing inorganic semiconductors without inp

9 and efficient 4f-4f emission with the strong broadband absorption and low-phonon-energy crystalline e

10 stic quasi-random nanostructures improve the broadband absorption by 225% over the unpatterned cell.

11 d metasurface design, enabling efficient and broadband absorption enhancement by direct coupling of i

12 thermal mass while maintaining high infrared broadband absorption in the long wavelength infrared (LW

13 The broadband absorption measures >87% from 1,200 nm to over

14 In experiments a high broadband absorption was maintained even when the fill f

15 display selective, omnidirectional, tunable, broadband absorption when closely packed.

16 esonant structures enable angle-insensitive, broadband absorption.

17 de range of acoustic applications, including broadband acoustic isolation and topologically protected

18 celeration (eventually becoming the 20-50 Hz broadband activity caused by the asynchronous state) and

19 l cortex exhibits two types of gamma rhythm: broadband activity in the 30-90 Hz range and a narrowban

20 ite effects on the two rhythms: it increased broadband activity, but suppressed the narrowband oscill

21 hase of the beta rhythm and the amplitude of broadband activity.

22 , this technique opens the possibilities for broadband, always-ready quantum memories and fast optica

23 ke fMRI, resting-state power fluctuations of broadband and arrhythmic, or scale-free, macaque electro

24 The observed broadband and fast momentum transformation could promote

25 d do not suffer from speckle, but are rather broadband and have a relatively low output power limitin

26 ptical lines in a single device enabling the broadband and high-speed detection required in many appl

27 Using ultra-broadband and highly time-resolved optical spectroscopy,

28 ent metasurfaces can enable small-footprint, broadband and low-loss photonic integrated devices.

29 For broadband and multimode devices, however, more complex s

30 e photoelectrochemical water splitting under broadband and red light (lambda > 590 nm) illumination i

31 d principal component analysis, to realize a broadband and sensitive wavemeter.

32 t electrical stimulation can evoke both fast broadband and slow sharply tuned responses of the reticu

33 d by broadband or stochastic processes, with broadband and stochastic characteristics that are substa

34 e elucidate the general methodology by which broadband and, simultaneously, large wave decelerations,

35 e matching, with the possibility of compact, broadband, and efficient frequency mixing integrated wit

36 Exploiting the sensitive, broadband, and high-resolution capabilities of time-reso

37 ion, which has been a big stumbling block to broadband applications.

38 Broadband asymmetric transmission (BAT) is a highly desi

39 amic responses of the proposed system in the broadband asymmetric transmission bands are explored and

40 halcogenide family as a platform for hybrid, broadband, atomically precise quantum photonics devices.

41 Most remarkably, the broadband behaviors of nondispersive optical activity an

42 nna-coupled tunnel diodes are examined under broadband blackbody and quantum-cascade laser (QCL) illu

43 example in the radiation belts is inherently broadband, but this is a feature hard to mimic with conv

44 Using time-resolved spectroscopy with broadband capability, we clearly demonstrate that CT at

45 T-CARS) spectroscopy technique that achieves broadband CARS measurements at an ultrahigh scan rate of

46 e technique's strength, we use it to perform broadband CARS spectroscopy of the transient mixing dyna

47 We report on the first detailed use of broadband cavity enhanced absorption spectroscopy (BBCEA

48 lyoxal and methylglyoxal were measured using broadband cavity enhanced spectroscopy, which for glyoxa

49 a Criegee intermediate has been measured by broadband cavity enhanced UV absorption.

50 two well-studied features of brain signals, broadband changes in the frequency power spectrum of the

51 pulses is often overlooked because of their broadband characteristics and short pulse durations.

52 nd 3D models to verify the functionality and broadband characteristics of the calculated lens.

53 ar, the unique holographic approach exhibits broadband characteristics.

54 esign and experimental demonstration of a 3D broadband cloak that can effectively manipulate the scat

55 e than 20 times higher than that of previous broadband coherent Raman scattering spectroscopy techniq

56 of fractional nonlinear harmonics leading to broadband coherent white-light generation.

57 atomic clocks enabling satellite navigation, broadband communication and high-speed trading.

58 ations with uncontended, multi-gigabits/user broadband connections.

59 he optical properties provide a platform for broadband control of light-matter interaction.

60 This metadevice enables the broadband conversion of linearly polarized light into an

61 Furthermore, broadband coplanar waveguide (CPW) to planar staggered p

62 eaches 27% in the DC-OPA pumped by a chirped broadband Cr(2+):ZnSe/ZnS laser, enabling the generation

63 sts a simple and general way to flexibly use broadband current sources to produce broad or narrow ban

64 duces the spontaneous, directed formation of broadband, cylindrical waveguides.

65 ( approximately 5-7 Hz) power followed by a broadband decrease in alpha/beta power in the time-frequ

66 the bulk crystals exhibit a highly efficient broadband deep-red emission peaked at 695 nm, with a lar

67 technology will be unable to support future broadband demands.

68 ale electrochemical strain microscopy (ESM), broadband dielectric spectroscopy measurements, and dens

69 that the SMM has the potential for use as a broadband dielectric spectroscopy operating at higher fr

70 Here, we use broadband echo sounders to characterize Arctic thermohal

71 ids produce large numbers of short duration, broadband echolocation clicks which may be useful for sp

72 was strongly correlated with a reduction in broadband EEG power after stimulus presentation.

73 Here we describe instead a broadband effect of enhanced light transmission through

74 spectral element simulations demonstrate the broadband efficacy of the metawedge in mode conversion w

75 perovskites were found to have white-light, broadband emission in the visible range that was attribu

76 raction images in both scattering angles and broadband energy can be utilized to retrieve complementa

77 ted on such nanopatterned substrates possess broadband-enhanced light absorption, high quantum effici

78 oach might be used as a general platform for broadband enhancement of infrared spectroscopy.

79 sentations following an initial induction of broadband events, which were temporally separated and se

80 S signal is optimized for water imaging with broadband excitation.

81 oss of both the Bk(III) luminescence and the broadband feature.

82 ise both frequency-specific oscillations and broadband-features, such as long-range dependence (LRD).

83 f the LH2 electronic structure, we performed broadband femtosecond transient absorption spectroscopy

84 ive field of the cortical site measured with broadband field potentials, and less so with event relat

85 Here we experimentally demonstrate broadband, flexible, conformable, helicity multiplexed m

86 cortex of rats were stimulated in vivo with broadband fluctuating currents applied juxtacellularly.

87 Complementary measurements by ultrafast broadband fluorescence and absorption spectroscopy show

88 Here, we demonstrate broadband four-wave mixing with enhanced nonlinear frequ

89 using silicon microresonators, and realize a broadband frequency comb spanning from 2.1 to 3.5 mum.

90 rthermore, the designed device can work in a broadband frequency range.

91 ptical activity with high transmittance in a broadband frequency range.

92 vity events that showed either narrowband or broadband frequency spans revealing characteristic spect

93 to achieve the required optical effect over broadband, from visible to short-infrared, thus circumve

94 the absorption edge, we find a red-shifted, broadband (full-width at half-maximum of about 0.4 eV),

95 rahertz quantum cascade lasers (QCLs) with a broadband gain medium could play an important role for s

96 l for high internal quantum efficiency and a broadband gain.

97 At rest, broadband gamma (50-200 Hz) power in the primary motor c

98 lating its strength, and its relationship to broadband gamma activity.

99 Narrowband and broadband gamma power were uncorrelated.

100 the way toward implementing high-performance broadband graphene-based photodetectors.

101 desired spatial resolution, the design of a broadband high-contrast nanoprobe for ultrafast temporal

102 cranial (iEEG) work we found that excitatory broadband high-frequency activity transients, driven by

103 ay lead to the development of a new class of broadband high-resolution spectrometers.

104 low dielectric loss and near-dispersionless broadband, high permittivity, is exceedingly demanding.

105 to its unique performance in terms of ultra-broadband, high-speed detection and frequency accuracy,

106 rive reduction of the iron oxide shell under broadband illumination to reversibly blue-shift and sign

107 plications in biomimetic circuitry and ultra-broadband imaging but polycrystalline and amorphous thin

108 design could surpass this limit by providing broadband increase in the local density of states in a s

109 quency adaptation of MT neurons and led to a broadband increase in the power spectrum of local field

110 x molecules requires methods that can record broadband infrared spectra (that is, spanning multiple v

111 and to an intriguing possibilities of ultra-broadband investigations into complex condensed matter s

112 es in the dark to the more stable one, while broadband IR irradiation above 2000 cm(-1) results in an

113 n ultrathin (20 nm) VO2 film, we demonstrate broadband IR light absorption tuning (from ~90% to ~30%

114 o-cis conversions of HOCO is also found upon broadband IR light of the spectrometer, and the ratio of

115 gnitude faster when the sample is exposed to broadband IR radiation.

116 Continuous broadband irradiation (lambda > 220 nm; 130 min) of the

117 Broadband laser sources based on supercontinuum generati

118 relative standard deviation using relatively broadband lasers to mitigate spectroscopic fractionation

119 rectional operation are developed to achieve broadband lasing from the same semiconductor chip.

120 Broadband lasing in the frequency range of 3.1-3.7 THz i

121 the remembered S1 was strongly reflected in broadband LFP activity, with an early sensory-related co

122 s forms an optoelectronic crystal capable of broadband light absorption and efficient funnelling of p

123 ide (GO) thin film material, which exhibited broadband light absorption and excellent stability in hi

124 The experimental results show that broadband light can be controlled and redirected in a vo

125 Assisted by chaotic motions, broadband light can travel between optical modes with di

126 new platforms for spectroscopy, sensing, and broadband light generation, a potential testing ground f

127 he deterministic spatiospectral control of a broadband light source by means of wavefront shaping.

128 Broadband light trapping and field localization is highl

129 crystalline silicon solar cell, in enhancing broadband light trapping capability of the cell and, at

130 We report 'broadband light-sensing' all-polymer phototransistors wi

131 This broadband light-trapping metastructure shows its potenti

132 . Hu and co-workers report highly efficient, broadband lighting from printed hybrid nanocarbon struct

133 perimentally demonstrate a highly efficient, broadband linear polarization converter functioning at t

134 onductor kinetic inductance creates an ultra-broadband linear-dispersion and constant-attenuation reg

135 brication, and characterization of sensitive broadband lithium niobate (LiNbO3) single element ultras

136 apping to produce highly efficient below-gap broadband luminescence, and opens up a new route towards

137 aser-plasma-accelerators to directly produce broadband Maxwellian-type particle flux, akin to conditi

138 The broadband mechanical measurements demonstrated have fund

139 mote applications such as multicolor lasers, broadband memories, and multiwavelength optical networks

140 Finally, a broadband metadiffuser panel of 3 cm thick was designed

141 We demonstrate an infrared broadband metasurface absorber that is suitable for incr

142 Here we report a broadband metasurface design, enabling efficient and bro

143 Here, we report a high-performance broadband metasurface quarter-wave plate made of anisotr

144 de is single mode, providing a sensitive and broadband method for THz power splitting.

145 ons in non-planar ferromagnetic dots using a broadband microwave spectroscopy technique.

146 (H2O)n (n=1-5) adducts have been analyzed by broadband microwave spectroscopy.

147 nvestigated using a combination of ultrafast broadband mid-IR and visible transient absorption and fl

148 rectangular cross section is used to excite broadband Mie resonances across visible and near-IR spec

149 e simplest two-component configurations with broadband mixing are found, as well as the more complex

150 In this report, broadband mixing of the [Formula: see text]-symmetric an

151 ity dispersion was engineered for efficient, broadband mode-locking via four wave mixing.

152 h in thickness and exhibit compact and truly broadband modulation of optical signals using heterostru

153 The broadband momentum transformation enhances the device co

154 We report broadband momentum transformations of light in asymmetri

155 In contrast, images that elicit larger broadband, multiunit, or fMRI responses are much less pr

156 ronic devices, such as electrically tunable, broadband near infrared lighting devices operating at ro

157 In this study, we used broadband near-infrared spectroscopy (NIRS) to measure t

158 ing is achieved by reducing the amplitude of broadband neural oscillations after sensory input, which

159 een variability quenching and suppression of broadband neural oscillations.

160 ults demonstrate the tremendous potential of broadband NIRS as a non-invasive, in vivo means to study

161 We used a broadband NIRS system to measure changes in oxCCO, in ad

162 Stimuli were broadband noise bursts, 10-Hz sinusoidally amplitude-mod

163 We demonstrate that coherent broadband noise enhances signal representation in audito

164 this stimulation protocol to time-dependent broadband noise stimulation in sensory and motor cortice

165 using sinusoidally amplitude modulated (AM) broadband noise stimuli presented in simulated anechoic

166 hway responded selectively to high-intensity broadband noise, but not pure tones.

167 is strongly enhanced in coherently modulated broadband noise, corresponding to the psychoacoustic phe

168 onal time-frequency modes as well as against broadband noise, with performance well exceeding the the

169 ion enables loss-free, compact and extremely broadband non-reciprocity.

170 We report the ultra-broadband nonlinear optical (NLO) response of Bi2TexSe3-

171 applications as they underpin the material's broadband nonlinear optical absorption and ultra-fast ca

172 the Bi2TexSe3-x nanosheets possess an ultra-broadband nonlinear saturable absorption property coveri

173 ions, and good performance is observed for a broadband of frequencies.

174 Furthermore, we observe a broadbanding of the reflectance spectra from the plasmon

175 By tuning the pump wavelength, broadband OFC with the bandwidth of >180 nm and the freq

176 level diffractive microstructures can enable broadband, on-axis transmissive holograms that can proje

177 allowing for large isolation in the bulk and broadband one-way transport along their edges, with topo

178 entations rely on resonance techniques, thus broadband operation at optical frequencies imposes signi

179 c silicon herringbone structures, exhibits a broadband operation in the terahertz regime.

180 ces" with high fidelity, high efficiency and broadband operation that are interchangeable by controll

181 s inside the nanocomposite that enhanced the broadband optical absorption up to 2.3 eV and subsequent

182 electric waveguide with a low-visibility and broadband optical activity represents a transformative w

183 y applications including high-speed imaging, broadband optical communications, and ultrafast laser di

184 A broadband optical diode behavior is observed after optim

185 tion law, we calibrate these SNe using their broadband optical light curves to within ~0.065 to 0.075

186 neous chunks of bulk aerogels with superior, broadband optical transparency across the visible spectr

187 es during transitory periods (in the case of broadband or Alfvenic aurora).

188 lly tailored absorption coatings with either broadband or narrowband characteristics.

189 ation is less at Jupiter than that caused by broadband or stochastic processes, with broadband and st

190 ever, in thermoelectric detectors, achieving broadband or wavelength-selective performance with high

191 st-effective technique for the generation of broadband orbital angular momentum and radially polarize

192 These unidirectional structures are broadband (over 2.5 THz) at 1550 nm, effectively loss-fr

193 on, we demonstrate a miniature, directional, broadband, passive, low-cost approach to detect airflow

194 work provides a feasible approach to realize broadband perfect absorption of elastic waves in ultra-t

195 The broadband phase mixing in the four-channel case is expec

196 is novel microresonator, we demonstrate that broadband phase-locked Kerr frequency combs with flat an

197 The broadband photodetection is attributed to the synergisti

198 Here, we demonstrate a broadband photodetector using a layered black phosphorus

199 uch as non-bandgap-limited hyperspectral and broadband photodetectors.

200 Here, a high-performance p-Si/n-ZnO broadband photodiode working in a wide wavelength range

201 The general performance of the broadband photodiodes can be further improved by the pie

202 verely limit its use in applications such as broadband photodiodes.

203 hypercrystals" (PHCs) that combine the large broadband photonic density of states provided by hyperbo

204 nverse-design method to design ultra-compact broadband photonic devices.

205 It consistently shows broadband photoresponse from the ultraviolet (255 nm) to

206 from 0.36 to 2.62 eV, which are crucial for broadband photoresponse.

207 ally tunable conductance and capacitance and broadband photoresponse.

208 Whereas broadband physiological noise is general to all processe

209 We derive analytic broadband pi/2 and pi pulses that perform exact, or asym

210 plasmons, and open the way to the design of broadband plasmonic devices able to operate at very diff

211 mental and theoretical results on the use of broadband plasmonic nanopatch metasurfaces comprising a

212 cancy centres in diamond and photonic and/or broadband plasmonic nanostructures is crucial for the de

213 lline lattices, one can obtain multi-band or broadband plasmonic resonances which are not possible in

214 the Stokes parameters, indicating excellent broadband polarization conversion between linearly and c

215 We demonstrate a broadband, polarization independent, wide-angle absorber

216 Here, we demonstrate lithography-free, broadband, polarization-independent optical absorbers ba

217 onse for approaching uncooled ultrasensitive broadband polymer PDs in the future study.

218 of global resting-state fMRI activity is the broadband power fluctuation in scale-free population act

219 Results demonstrate that the broadband power fluctuation of scale-free electrophysiol

220 scillations in the local field potential and broadband power increases.

221 across stimuli, the BOLD amplitude and ECoG broadband power were positively correlated, the BOLD amp

222 omatic UV-B, UV-A, and visible radiation and broadband provocation testing showing similar results.

223 ents have been studied using a continuous or broadband-pulsed terahertz source, not using a modulated

224 Designing accurate and high-fidelity broadband pulses is an essential component in conducting

225 However, constructing exact and analytic broadband pulses remains unsolved due to the nonlinearit

226 caded nonlinear processes are enabled by the broadband pump and the coincident phase matching angle o

227 exhibit negligible absorption of free-space broadband pump light.

228 metric chirped pulse amplifier (OPCPA) and a broadband-pumped dual-chirped optical parametric amplifi

229 and paves the way for the optimal design of broadband-pumped high-quality micro-lasers and efficient

230 mbles of solid-state optical emitters enable broadband quantum storage and transduction of photonic q

231 ctroscopy systems increasingly rely on ultra-broadband radiation (extending over more 5 octaves) maki

232 ma-accelerators, we reproduced relativistic, broadband radiation belt flux in the laboratory, and use

233 best when we used a combination of both the broadband response and ERP, suggesting that they capture

234 calculations suggest a promise of MXenes in broadband saturable absorber applications due to metalli

235 d on the unique polarization selectivity and broadband saturable absorption of monolayer graphene.

236 hese structures, we generated a multi-octave broadband SC spectrum ranging from 1.5 um-25 um at a low

237 quake events (DFLEs) in near real-time using broadband seismic records, which can provide timely warn

238 rbations are particularly well observed with broadband seismometers at distances between 1000 and 200

239 recorded by a superconducting gravimeter and broadband seismometers during the 2011 Mw 9.0 Tohoku-Oki

240 High-speed broadband services require optical fibres in access netw

241 synchrony in the local population, while the broadband signal reflects the level of asynchronous neur

242 red changes in noise spectrum deviating from broadband, signal dependent noise.

243 l (3D) acoustic illusions under detection of broadband signals still remains challenging despite the

244 ated circuits, compact high Q-resonators and broadband, slow-light devices in the THz band.

245 ted with element- and site-specificity using broadband soft X-ray pulses produced by high harmonic ge

246 ce has a high porosity (97.3%) and efficient broadband solar absorption (>97%).

247 cues are integrated: cortical ILD tuning to broadband sounds is a composite of separate, frequency-s

248 lar, responses to natural scenes, which have broadband spatiotemporal statistics, are more reliable t

249 re obtained for generating 1.8-4.2 mum super broadband spectra, which can be used to seed both the si

250 th the global hemodynamic change lagging the broadband spectral change of EEG by approximately 5 s.

251 e current established technology, can record broadband spectral data efficiently but requires scannin

252 A rapid, broadband spectral measurement (520 cm(-1)) of methane u

253 er, we demonstrate diffraction-limited ultra-broadband spectroscopy system up to 14.5 THz with a dyna

254 AR Sco's broadband spectrum is characteristic of synchrotron radi

255 that enhance the absorption of light over a broadband spectrum, and permit the reduction of thicknes

256 a wavelength selector, a novel approach to a broadband stimulated Raman spectroscopy is demonstrated.

257 We demonstrate an intense broadband terahertz (THz) source based on the interactio

258 We demonstrate broadband terahertz detection with signal-to-noise ratio

259 e present a powerful technique for realizing broadband terahertz detectors through large-area plasmon

260 z-rate amplitude modulation and switching of broadband terahertz electromagnetic waves.

261 and could lead to commercial development of broadband terahertz laser arrays.

262 highest operating temperatures achieved for broadband terahertz QCLs at the respective emission freq

263 rent that drives the nanoantennas to produce broadband terahertz radiation.

264 regime (0.2-2 THz) were characterized using broadband terahertz time-domain spectroscopy.

265 Highly efficient broadband thermal radiation from reduced graphene oxide

266 lls, and besides for achieving intense ultra-broadband THz electric fields.

267 erve as an ideal channel for transmission of broadband THz pulses.

268 ese needs, the development of an intense and broadband THz source has been a focus of THz research.

269 ity are very promising materials for intense broadband THz wave generation and other nonlinear optica

270 se complex in solution are compared with the broadband time-resolved firefly bioluminescence recorded

271 vskite films, CH3NH3SnI3, were studied using broadband transient absorption and time-resolved fluores

272 Refolding was confirmed by ultrafast broadband transient absorption and two-dimensional elect

273 Herein, we use broadband transient absorption spectroscopy to measure r

274 rystal tetra-n-butylammonium triiodide using broadband transient absorption spectroscopy.

275 CH3NH3PbBr3 perovskite single crystals using broadband transient reflectance spectroscopy.

276 The second method used broadband trapping to collect ions and translationally c

277 Broadband tunability is a central theme in contemporary

278 Broadband tunable absorbers can find applications in abs

279 g of a gallium antimonide cell paired with a broadband tungsten and a radiatively-optimized Drude rad

280 Here, we apply ultrafast broadband two-dimensional infrared (2D IR) spectroscopy

281 , is rather insignificant as demonstrated by broadband two-photon spectroscopy.

282 Blue structures have a well-defined broadband ultra-violet (UV) to blue wavelength distribut

283 interest in the physics and applications of broadband ultraslow waves in nanoscale structures operat

284 e two parameters velocity of sound (VOS) and broadband ultrasound attenuation (BUA), is an alternativ

285 lop new material and structural concepts for broadband vibration mitigation.

286 This combination of strong broadband visible absorption, sharp near-infrared emissi

287 We investigate the origin of the broadband visible emission in layered hybrid lead-halide

288 red to photorelease CO remotely by low-power broadband visible light (<1mWcm(-2)) with the aid of fib

289 Importantly, the broadband wave attenuation capability will be maintained

290 ent method, we numerically demonstrated that broadband wave attenuation zones can be achieved by tail

291 ible to have high cloaking efficiencies in a broadband wavelength range, and we experimentally demons

292 transmission ratio is larger than 2.5 over a broadband wavelength regime.

293 al base for optoelectrical applications with broadband wavelength selectivity from the infrared to th

294 These dual-band pulsed sources with an ultra-broadband wavelength separation of ~360 nm will add new

295 -random geometries can manipulate light over broadband wavelengths and wide ranges of angles.

296 intain the quarter-wave phase retardation in broadband, while the turbine blades consist of multiple

297 on than that of EA4Pb3Br10, which results in broadband white-light emission of EA4Pb3Cl10 in contrast

298 mm(2)) and Luneburg lens (855 mm(2)) in the broadband white-light visible wavelength range using the

299 We present here a broadband, wide-angle, and polarization-independent near

300 Here, we demonstrate a highly-collimated, broadband, wide-diameter beam from a compact source in f