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

3 In a standard broadband 2D MS, the range of precursor ion cyclotron fr

4 namely (i) a high Numerical Aperture (N.A.), broadband aberration rectified spherical lens (0.1 THz-0

5 smonic nanoclusters that either operate as a broadband absorber or with a reconfigurable reflection b

6 ractive index matching or the inclusion of a broadband absorber.

7 absorbers in one-port and two-port systems: broadband absorbers (one-port), broadband sparse absorbe

8 saturable absorbers (SAs) are considered as broadband absorbers and have been used in various studie

9 Broadband absorbers are essential components of many lig

10 Our approach for broadband absorption allows to minimize the number of re

11 zy graphene (NT-3DFG) is flexible due to its broadband absorption and does not generate cellular stre

12 dride reduction substantially attenuated the broadband absorption enhancements with pH, clearly indic

13 ltrathin (lambda/165) metasurface to develop broadband absorption in a frequency range of interest fo

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

15 It combines broadband absorption of all frequencies used by bats wit

16 monic systems, realising the transition from broadband absorption to tunable reflection through deter

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

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

19 Recently, broadband achromatic metalenses in the visible have been

20 ped resonance, we demonstrate three types of broadband acoustic absorbers in one-port and two-port sy

21 tions (<30 Hz) entrain the corticomotor high broadband activity (>40 Hz) during rest, relinquishing t

22 The amplitude of high broadband activity in human cortical field potentials in

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

24 ruption, mediated by slow wave modulation of broadband activity, changes during unconsciousness in hu

25 ) that maximized the ratio between theta and broadband activity.

26 a significant negative relationship between broadband albedo (Moderate Resolution Imaging Spectrorad

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

28 monic Doppler gratings (PDGs), which provide broadband and azimuthal angle dependent grating periodic

29 Specifically, we demonstrate broadband and controllable shift (up to 14.9 THz) in the

30 The observed broadband and fast momentum transformation could promote

31 d correlate these networks with time-varying broadband and frequency-specific functional networks der

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

33 By utilizing the meta-skin insulator with broadband and high throughput, orbital-angular-momentum

34 tense laser-driven proton pulses, inherently broadband and highly divergent, pose a challenge to esta

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

36 These findings indicate that broadband and narrow band functional connections reflect

37 In this proof-of-concept study, we compare broadband and narrowband modulation 2D mass spectra of a

38 and engineering, that can simultaneously be broadband and possessing long storage times, thereby off

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

40 It was observed that a broadband and simultaneous emission involving coumarin c

41 ation about the seen category is encoded via broadband and sub-gamma (<30 Hz) power variations, while

42 We demonstrate broadband and wide-angle antireflective surface nanostru

43 on paper substrates can dramatically enhance broadband and wide-angle light absorption across the ful

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

45 In recent years, broadband- and near-infrared (NIR)-mediated polymerizati

46 ample of a novel photocatalyst for both full broadband- and NIR-mediated CRP in aqueous conditions.

47 odified Luneburg lens antenna by designing a broadband anti-reflective layer along with the modified

48 ading to strong chromatic aberrations of the broadband attosecond pulses.

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

50 Electrical power generation from a broadband blackbody thermal source has been experimental

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

52 We present the first ever broadband, calibrated electrical connection to the insid

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

54 ly above the surface of liquid samples using broadband cavity enhanced absorption spectroscopy.

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

56 ignal enhancement (~10(6)) due to its strong broadband charge-transfer resonance, but also extraordin

57 Here, we present the first broadband chip-scale single-photon spectrometer covering

58 e-water adducts have been observed using two broadband chirped-pulse Fourier-transform microwave (CP-

59 l coloration combined with highly asymmetric broadband circular dichroism and a microfocusing capabil

60 mice showed a large increase in ultrasonic, broadband clicks after sciatic nerve injury, which was r

61 eates chaotic tunneling channels that enable broadband collection of intracavity emission with a sing

62 nd a use in applications, where multiband or broadband compact devices are required.

63 a of the LFPs near stimulus onset revealed a broadband component (1-100 Hz) and two narrowband compon

64 ses revealed that power variations along the broadband component were most sharply tuned and offered

65 hemical transformation first as a whole in a broadband configuration and then immediately switch to t

66 correlated components, and importantly, both broadband correlations and neuronal spiking activity are

67 owband oscillations also exhibit time-locked broadband correlations with a consistent time delay, a r

68 Increases in broadband cortical electroencephalogram (EEG) power in t

69 scopic measurements between high resolution, broadband coverage, and acquisition time.

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

71 or qH{(13)C}NMR: GARP and bilevel adiabatic broadband decoupling.

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

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

74 nd collectively they generate hard-to-attain broadband deep-subwavelength absorption.

75 dramatic optical contrast of GST, we realize broadband (Deltalambda/lambda ~ 15%) mode shifting betwe

76 Broadband dielectric spectroscopy (BDS) measurements bef

77 vant cooling rates (2-10 K/min) by thin film broadband dielectric spectroscopy.

78 lved spectra acquired with a highly-coherent broadband dual-frequency-comb system based on optical su

79 , broadband sparse absorbers (two-port), and broadband duct absorbers (two-port).

80 rimary auditory cortex, using pure tones and broadband dynamic moving ripple stimuli, to examine prop

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

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

83 h the nondeletion genotype as well as excess broadband EEG power (1-32 Hz) peaking in the delta frequ

84 on the dynamical state of the system, these broadband effects can be better predicted by functional

85 ICR cell, using single-shot ejections after broadband ejections and MS/MS based on sustained off-res

86 Broadband Electrical Spectroscopy (BES) demonstrates tha

87 el, polarization insensitive, wide-angle and broadband electromagnetic metamaterial absorber, which c

88 These results demonstrate that the broadband emission decay of (EDBE)PbBr(4) arises from a

89 ing a compact common-path interferometer and broadband excitation, which is implemented as an extensi

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

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

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

93 Broadband femtosecond fluorescence up-conversion spectro

94 combined with scanning electron microscopy, broadband femtosecond transient absorption spectroscopy

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

96 Broadband focusing with composite plano-convex metasurfa

97 batic nanofocusing and imaging, we study the broadband four-wave mixing (FWM) response of graphene wi

98 imaging platforms are implemented including broadband Fourier transform infrared microscopy and disc

99 ave oscillations (0.1-1 Hz) and amplitude of broadband frequencies (8-200 Hz) within the cortex and a

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

101 This paper proposes a compact broadband frequency scanning spoof surface plasmon polar

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

103 he light flowing along a single branch has a broadband frequency stability such that one can even ste

104 Our broadband full Stokes polarimeter is robust, cost-effect

105 ired as the diffuser relies solely on strong broadband (full visible range) lossless multiple light s

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

107 The broadband functional connectivity of LAI was similar to

108 ow beta in the thalamus and the amplitude of broadband gamma (50-200 Hz) in the cortex (P = 0.031, Wi

109 lts support the idea that increased cortical broadband gamma activity leads to impairments in cogniti

110 which involve aberrant increases in cortical broadband gamma activity.

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

112 m-binding protein parvalbumin (PV) increased broadband gamma frequency power, increased locomotor act

113 the mechanisms which can result in increased broadband gamma power and the pathophysiological implica

114 BF-PV neurons partially rescued the elevated broadband gamma power elicited by subanesthetic doses of

115 rousal system bidirectionally tunes cortical broadband gamma power, allowing on-demand tests of the e

116 In contrast, broadband gamma was consistently observed for all presen

117 ral, and functional properties of narrow and broadband gamma.

118 Here, we demonstrate that two broadband (>300 nm) synchronized mode-locked lasers enab

119 ctivity, best captured in the high-frequency broadband (HFB; 70-170 Hz) range.

120 visual narrowband gamma oscillations, unlike broadband high gamma, appears contingent on specific str

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

122 scillations and phase-related modulations in broadband high-frequency activity.

123 20-60 Hz), recent work has emphasized a more broadband "high-gamma" response (~70-150+ Hz).

124 r single quantum correlation method provides broadband homonuclear decoupling along the proton detect

125 at the most important variation patterns are broadband (i.e., distributed across multiple frequencies

126 Therefore, they require broadband illumination and spectrometers.

127 the use of highly responsive materials under broadband illumination.

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

129 For example, broadband impedance matching, accompanied with moderatel

130 ose employing hyperbolic metamaterials for a broadband impedance matching, while a structured layer o

131 ity profile along its thickness, and ensures broadband impedance matching.

132 proposed anti-reflector layer is inherently broadband in nature, has a continuously tapered inhomoge

133 ep, postictal slowing was characterized by a broadband increase of spectral power, and showed a reduc

134 This initiative opens the door to broadband infrared nano-imaging of heterogeneity in ferr

135 ve infrared imaging, mechanical mapping, and broadband infrared spectroscopy capabilities with 6 nm s

136 spectral receptive-field model incorporating broadband inhibition better predicted the neural respons

137 on through nonlinear temporal integration of broadband inputs.

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

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

140 best of our knowledge-not been harnessed in broadband IR measurements to date.

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

142 We generate broadband Kerr frequency combs using a dispersion-engine

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

144 sh the potential for lightweight, ultrathin, broadband lenses for high-quality imaging in the LWIR ba

145 In contrast, broadband LFP power, including gamma, negatively predict

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

147 built-in electric field for high-efficiency broadband light absorption, exciton dissociation, and ca

148 ecently gained attention as highly efficient broadband light emitters.

149 of accurate, visible-range monochromatic and broadband light reconstruction, as well as spectral imag

150 ant device technology that can be applied to broadband light sensing, highly sensitive fluorescence i

151 ng of nanoparticles on a chip using low-cost broadband light sources.

152 Broadband light trapping and field localization is highl

153 This broadband light-trapping metastructure shows its potenti

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

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

156 uency hearing loss by low-pass filtering the broadband masking noise.

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

158 t a single microresonator provides rapid and broadband measurement of optical frequencies with a rela

159 Here we present a broadband measurement of QRPN at room temperature at fre

160 The broadband mechanical measurements demonstrated have fund

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

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

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

164 portunities to achieve highly reconfigurable broadband metasurfaces with large diffraction efficiency

165 r of peaks with greater accuracy compared to broadband methods.

166 ique provides an alternative way to generate broadband microcombs and enables the selective enhanceme

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

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

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

170 Broadband near-infrared spectroscopy was used to record

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

172 on) analyses of single AN fiber responses to broadband noise, for direct comparison to previously pub

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

174 icantly better (P < 0.0001) than those using broadband noise.

175 tem in the presence of a recorded real-world broadband noise.

176 i, differing dramatically from fMRI and ECoG broadband (non-oscillatory) responses.

177 cryoprobe, when compared with a conventional broadband observe (BBO) probe, further sensitivity enhan

178 dimensions of (55 x 30) mm(2) has achieved a broadband of 4 GHz with high peak measured gain of 9.8 d

179 h self-organization, energy distributed in a broadband of frequencies gets condensed into a dominant

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

181 uctural wave cloaking and waveguiding over a broadband operating frequency range.

182 tic metasurfaces capable of an exceptionally broadband operating range.

183 e-matching-free nature and its unprecedented broadband operation range.

184 is adaptive in real time for reconfigurable broadband operation thanks to its programmability.

185 eometry, (iv) high efficiency along with (v) broadband operation, (vi) area scalability and (vii) fab

186 However, chromatic aberration, limiting broadband operation, has remained a challenge for metasu

187 ch showed record conversion efficiencies and broadband operation, the possibility to coherently contr

188 rces that combine resonant upconversion with broadband operation.

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

190 Broadband optical frequency combs are extremely versatil

191 nerating white or black colours due to their broadband optical response and robustness to perturbatio

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

193 and visualized using high-speed imaging and broadband or monochromatic laser light-sheet illuminatio

194 rking bands are reversibly tuned in an ultra-broadband over 1000 nm covering green to telecomm region

195 We demonstrate broadband perfect acoustic absorption by damped resonanc

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

197 An off-resonance broadband photoacoustic spectroscopy (PAS) technique wit

198 dry transfer, demonstrates high-sensitivity, broadband photodetection at room temperature.

199 The broadband photodetection is attributed to the synergisti

200 t, the device can work as a high-performance broadband photodetector with extremely high sensitivity

201 or time-dependent studies indicated that the broadband photoluminescence (PL) from (110) perovskites

202 (LSPR) is, for the first time, exploited for broadband photon harvesting in photo-regulated controlle

203 Owing to the LSPR-enhanced broadband photon harvesting, high monomer conversion (>9

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

205 oach toward future ultrahigh-sensitivity and broadband photonic detectors.

206 rministically embedding GaAs quantum dots in broadband photonic nanostructures that enable Purcell-en

207 sing, nanocellulose can be used to fabricate broadband photonic reflectors, thermally super-insulatin

208 A broadband photoresponse from 532 to 1850 nm with ultrahi

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

210 ally tunable conductance and capacitance and broadband photoresponse.

211 Whereas broadband physiological noise is general to all processe

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

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

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

215 By introducing a tilted THz ultra-broadband polarizer, we split the THz beam in two orthog

216 At sensorimotor cortices, there was a broadband power increase (12-100 Hz), while the power of

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

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

219 tate onsets, surrounded by locally decreased broadband power, suggesting a mechanism synchronizing co

220 Relativistic plasma mirrors generate broadband power-law spectra, that may span the gap betwe

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

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

223 Broadband pump-probe experiments with ~100-fs time resol

224 eviously demonstrated to effectively capture broadband radiation across the ultraviolet to near-infra

225 tremely nonlinear effect generating coherent broadband radiation and pulse durations reaching attosec

226 on spectrum and is therefore well suited for broadband radiation sources.

227 light-excited fluorescence, and mid-infrared broadband radiation.

228 hat are virtually dispersion-free over ultra-broadband ranges of wavelengths from microns up to milli

229 At the core of the approach is a novel broadband relaxation-edited NMR experiment that covers t

230 the tunability of disordered systems with a broadband response has been scarcely explored.

231 Such an imaging device achieves broadband response in 4.2-20 THz and can absorb the norm

232 Achieving the broadband response of metamaterial absorbers has been qu

233 ich cannot be fulfilled by common PDs with a broadband response such as Si-based PDs.

234 Here we present a broadband rotational-spectroscopy study on the stepwise

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

236 alidation data for doublets and a commercial broadband scan lens.

237 the standard FT-IR mode, used for classical broadband scans from 6000 to 650 cm(-1), and the new QCL

238 ommunication infrastructure (dark fiber) for broadband seismic monitoring of both near-surface soil p

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

240 gnetic wave amplitude and exhibits prominent broadband sensing from 5 to 900 MHz.

241 Broadband sensitive photoresponse is realized at room te

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

243 We use a broadband simulation approach to develop a rupture scena

244 n channels, preventing parallel detection of broadband single photons with high spectral resolutions.

245 linear metasurfaces can efficiently generate broadband single-cycle THz pulses.

246 oton pair generation, (ii) deterministic and broadband single-photon spatial conversion relying on a

247 We found that broadband slow-wave modulation enveloped posterior corte

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

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

250 By varying the spectral contrast of broadband sounds around the 6-9 kHz band, which falls wi

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

252 The detection ranges of broadband sounds produced by marine invertebrates are no

253 etal TaAs, which is demonstrated as a unique broadband source of the chiral terahertz wave.

254 Noise and spectral stability of such broadband sources are key parameters that define their t

255 ort systems: broadband absorbers (one-port), broadband sparse absorbers (two-port), and broadband duc

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

257 times allows the creation of highly resolved broadband spectra.

258 We find that the broadband spectral energy distribution is double-peaked,

259 deliver new avenues for chemical imaging and broadband spectroscopy at ~10 nm spatial resolution.

260 A mode-locked laser that can produce a broadband spectrum and ultrashort pulse has been applied

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

262 Relative to a broadband spectrum, the stitched output showed an over 2

263 hibited great potentials with high power and broadband spectrum.

264 electrically tunable over an extremely large broadband spectrum.

265 ons and depolarization ratios measured using broadband SRS agree with the limited number of previousl

266 methanol, water, benzene, and toluene using broadband SRS with femtosecond and picosecond Raman pump

267 Broadband stimulated Raman scattering (SRS) is often obs

268 or outputs, with a color opponent center and broadband surround.

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

270 Here we demonstrate a broadband terahertz photon-type up-conversion imaging de

271 Since random patterns are spatially broadband, they capture more information per image, enab

272 Spectrograms of broadband THz pulses propagated through different length

273 Broadband transient absorption measurements and quantum

274 r cell devices in combination with ultrafast broadband transient absorption spectroscopy, we demonstr

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

276 n the body using low-frequency carrier-less (broadband) transmission, thereby making it extremely dif

277 itter (0.3 THz-0.6 THz) and (iii) an on-axis broadband transmissive hologram (0.3 THz-0.5 THz).

278 Using a leaky-wave antenna with a broadband transmitter, we demonstrate a single-shot appr

279 imized alloy, Ge(2)Sb(2)Se(4)Te(1), combines broadband transparency (1-18.5 mum), large optical contr

280 Broadband tunability is a central theme in contemporary

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

282 ng high-quality focusing while retaining the broadband/ultrashort characteristics of the radiation.

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 ted (P < .01) with calcaneal speed of sound, broadband ultrasound attenuation, and QUS index.

286 , a 255 nm UV-LED, a capillary Z-cell, and a broadband UV photodiode (PD).

287 opments have led to innovative solutions for broadband vibration attenuation, with a multitude of pot

288 here lightweight and tunable properties with broadband vibration suppression and wave attenuation abi

289 oil snapping organ generates substrate-borne broadband vibrations using fast, cyclical abdominal moti

290 al approach, combining electrophysiology and broadband Vis-NIR spectroscopy, to monitor neurodevelopm

291 hase Zero' clinical study platform combining broadband Vis/near-infrared(NIR) spectroscopy and electr

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

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

294 y (OCT) and FAF simultaneously with a single broadband visible light source.

295 d its ability to achieve a fully passive and broadband wave control.

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

297 The ultra-broadband, wavelength-selective pumping may be applied t

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

299 -Evans rats to 2 weeks of moderate-intensity broadband white noise followed by 1 week of 7 kHz tone p

300 crofluidic capillary flow and a microfocused broadband X-ray source at the Advanced Light Source sync