コーパス検索結果 (1語後でソート)
通し番号をクリックするとPubMedの該当ページを表示します
1 om 16 channels sampled at 19.5 KHz (9.7 KHz bandwidth).
2 eme with 2 nm spatial resolution and 150 MHz bandwidth.
3 that falls within the intermediate frequency bandwidth.
4 sustain transmission over a broad frequency bandwidth.
5 ude of the horizontal peak and a doubling in bandwidth.
6 ing low-loss optical interconnects with high bandwidth.
7 with broad ranges of central wavelength and bandwidth.
8 above 3.0 over more than 1,000 nm wavelength bandwidth.
9 the structure is measured with insufficient bandwidth.
10 racterized by a force-dependent strength and bandwidth.
11 capacitance is believed to limit single-cell bandwidth.
12 ted during Cerenkov radiation within a given bandwidth.
13 localization, which improves with increasing bandwidth.
14 field to effectively use the available fibre bandwidth.
15 les, which have inherently narrow absorption bandwidth.
16 eves both high spectral resolution and broad bandwidth.
17 ensate to an optical cavity with ultranarrow bandwidth.
18 transformation over a broad octave-spanning bandwidth.
19 vity of the cells was restricted to a narrow bandwidth.
20 ase and amplitude profiles over a very broad bandwidth.
21 n unprecedented enlargement of the operation bandwidth.
22 ethod to facilitate increasing intracellular bandwidth.
23 le of which is a substantial fraction of the bandwidth.
24 n the resonance frequency and an increase of bandwidth.
25 alanced performance across the whole optical bandwidth.
26 neered to be anomalous over moderately broad bandwidth.
27 with an Eddy current effect in the absorbing bandwidth.
28 noscale, while maintaining a broad operation bandwidth.
29 ma channel, leads to a few percent radiation bandwidth.
30 ated quantum circuits operating at gigahertz bandwidths.
31 he range of 7.4 to 13.9 GHz with a broadened bandwidths.
32 encies occurring in both the gamma and theta bandwidths.
33 ithin 1 to 20Hz, 20 to 70Hz, and 70 to 150Hz bandwidths.
34 iconductors with wide valence and conduction bandwidths.
35 amentally different in their frequencies and bandwidths.
36 nsertion loss, size, and/or narrow operation bandwidths.
37 ollimated (<1 degrees divergence) and narrow bandwidth ( 10% energy spread) proton beamlet of 10(7)
38 quency measurement range limited only by the bandwidth (100 GHz) of current electro-optic modulators.
40 ncy bandwidths, whereas at the low-frequency bandwidth (3-20Hz) significantly more sources localized
41 otransistor with a high current gain (53.6), bandwidth (7 GHz) and responsivity (9.5 A/W) using a sin
42 within the high-frequency oscillation (HFO) bandwidth (70-150Hz) localized primarily to the frontal
43 er (k-space) spectrometer for an ultra-broad bandwidth (760 nm-920 nm) SD-OCT, whereby a combination
45 g with artificial sound sequences matched in bandwidth, amplitude, and duration but differing in spec
47 tive resonant absorption, where the resonant bandwidth and absorption intensity can be engineered by
50 ometer with unprecedented 400 kHz excitation bandwidth and capable of high-throughput acquisition of
53 lization can access more than a gigahertz of bandwidth and creates new possibilities for controlling
54 elling of infrared radiation with fractional bandwidth and efficiency as high as 97% and 48%, respect
56 s a route to spatial control over electronic bandwidth and ferromagnetism through the creation of oct
59 oscopy (CE-DFCS) combines the inherent broad bandwidth and high resolution of an optical frequency co
61 lows for fine tuning of spectral resolution, bandwidth and imaging speed while maintaining full duty
63 n (MTJ)-based STNO, which saves transmission bandwidth and in principle should minimize attenuation f
65 plate, which defies the fundamental limit of bandwidth and incident angles and has the ability of con
66 stantaneous optical transitions, has a broad bandwidth and is enhanced by the presence of resonant tr
67 have hitherto been limited either by narrow bandwidth and long acquisition time, or by low sensitivi
68 dom by dynamically addressing the modulation bandwidth and optical spectral tuning of a probe optical
69 ss short electrical wires is limited by both bandwidth and power density, which creates a performance
74 proach severs the link between the resonance bandwidth and the cavity-photon lifetime, thereby promis
76 linear regression models with a data-driven bandwidth and with the algorithm for selecting the bandw
79 two effective spins for phonons over a broad bandwidth, and strong spin-orbit coupling is realized by
82 e levels increased firing rates and expanded bandwidths, as is usually seen for FRAs obtained without
84 levels reduced firing rates and narrowed FRA bandwidths; at higher SNRs, however, increasing the tone
87 also significant broadening of the resonance bandwidth between laser frequency and that of electron b
89 rtness also increases the temporal frequency bandwidth, but preserves contrast sensitivity, orientati
90 s to the visible range while compressing the bandwidth by a factor of 7.47 under preservation of non-
91 head with high spatial resolution and large bandwidth by coherent control of single electron and nuc
92 ffers the potential to expand communication 'bandwidth' by using biomolecules and providing electroch
93 e of 2 x 10(19) photons/s/mm(2)/mrad(2)/0.1% bandwidth can be made with moderate laser and electron b
95 ; high-frequency ultrasound (156% fractional bandwidth centred around 13.5 MHz) was generated photoac
97 The probes were selectively quenched in the bandwidth closest to the indicator's absorption maximum
98 eneration efficiency with remarkably broader bandwidth compared to standard inorganic 0.5 mm thick Zn
100 rface exists that provides both an efficient bandwidth compression and a substantial frequency transl
103 photoconductive antennas has been limited by bandwidth constraints of their antennas and photoconduct
107 -based GEZIs is their broad spectral profile bandwidths, creating challenges when monitoring multiple
108 ow-bandwidth radiation from a broad spectral bandwidth current source, which takes advantage of the i
109 ther quantum photonic technologies into high bandwidth data communication infrastructures, thereby al
110 ring asserts that any type of system, having bandwidth Deltaomega, can interact with a wave over only
113 nd a dielectric, hold the key to future high-bandwidth, dense on-chip integrated logic circuits overc
114 citation wave patterns are imaged using high-bandwidth detectors, producing large data sets that are
115 rving full measurement characteristics (e.g. bandwidth, determination of capacitive/inductive contrib
116 l resolution much faster than the cantilever bandwidth, determined by the modulation frequency of the
120 ng, but these techniques generally limit the bandwidth, efficiency and active times of the quantum in
121 tems offer significantly improved power- and bandwidth-efficiency, but require fundamental simplifica
123 -electronic localization has a narrow usable bandwidth, electronically controlled optical localizatio
125 regate-like molecular packing, offers narrow-bandwidth emission, and has been successfully applied to
127 al across such a large synaptically relevant bandwidth enhances the response to small-amplitude acidi
132 cy qubits to the ions ( approximately 50 GHz bandwidth) followed by retrieval with 98.7% fidelity.
137 ustic transmitters and receivers have a wide bandwidth, from the audible region (20 approximately 20
139 n laser technology, X-rays with small enough bandwidth have become available, allowing the investigat
145 narrow spectral band ( approximately 900 nm bandwidth in the mid-infrared) with the intensity above
150 s not only limited by the intrinsic detector bandwidth; in addition, bandlimiting due to spatial aver
151 his small but clear and reproducible amide I bandwidth increase is not observed for protein in the so
152 psy and two humans undergoing prolonged wide bandwidth intracranial electroencephalographic monitorin
153 However, although the advantage conferred by bandwidth is clear, we currently know little about how t
156 tem, which is a function of the light source bandwidth, is sufficient to resolve retinal features at
161 s show that the x-rays emerge as nearly time-bandwidth-limited pulse trains of ~100 attoseconds.
162 sting measurement techniques are slow (<1 Hz bandwidth), limiting throughput and preventing use with
163 imultaneously owns high efficiency and broad bandwidth may open a new way for application in imaging,
164 strategies, contributing uncertainty to the bandwidth measurements and leaving important issues unre
169 microscopy techniques that have several kHz bandwidth necessary to reliably capture optically report
170 eadily extended to other systems to increase bandwidth, number of modes, or number of resonators.
172 the pump wavelength, broadband OFC with the bandwidth of >180 nm and the frequency-spacing varying f
177 ave over 30 dB sidelobe suppression and 3-dB bandwidth of 200 MHz, providing good filter selectivity.
179 um reflection loss of -44.7 dB and absorbing bandwidth of 4.7 GHz at -10 dB are achieved in composite
180 r the entire fiber length and operating at a bandwidth of 470 kHz, orders of magnitude larger than an
181 undamental mode direct resonance had a -3 dB bandwidth of 55 Hz, in contrast to the 314 Hz for the fi
182 ricated and measured showing increase in the bandwidth of blazing/specular-reflection-rejection, demo
184 s, we also determined the orientation-tuning bandwidth of correlated activity between pairs of LGN ne
187 sms, of which variability in the orientation bandwidth of linear filtering is the most important.
190 ed in the low-frequency regimes and in their bandwidth of operation because they require impractical
193 ion, with potential functions in setting the bandwidth of postsynaptic responses, sensitivity to mech
196 hitecture robustly achieves high gain over a bandwidth of several gigahertz with sufficient dynamic r
197 monic-antenna array is designed exhibiting a bandwidth of several octaves for use in both multi-band
201 l and experimental results indicate that the bandwidth of the absorption bands can be controlled by c
202 on is always limited by the narrow-frequency bandwidth of the acoustic waves because of the large att
203 he step height is approximately equal to the bandwidth of the auditory filter (critical band), and th
204 ave limitations in terms of peak ion energy, bandwidth of the energy spectrum and beam divergence.
206 the rapid narrowing nature of the frequency bandwidth of the higher instability intervals, making pr
207 Hz did not significantly affect threshold or bandwidth of the IC responses, but rates higher than 50H
209 h decoherence is simulated by broadening the bandwidth of the input illumination, yielding a signific
210 f OCT is limited to about 1 mum, even if the bandwidth of the light covers a wide spectral range.
211 herence is related to the intrinsic spectrum bandwidth of the light source, while spatial coherence c
213 and the thin film emit light within a narrow bandwidth of the visible spectrum and with a high quantu
216 oaden the accumulative operational frequency bandwidth of vibration energy harvesting for enabling se
219 esult from an interplay between the spectral bandwidths of the individual underlying chromophores and
220 t the precise combination of confinement and bandwidth offered by phonon polaritons allows for the ab
223 st photodetectors can enable low power, high bandwidth on-chip optical interconnects for silicon inte
224 eted by changing the filter's dispersion and bandwidth only, while no changes are made to the physica
226 can be continuously acquired at up to 1 kHz bandwidth, or the whole array can be read out rapidly at
227 ariable delay lines with a few THz operation bandwidth, our index-variable OTTDL has an extremely bro
228 n extremely broad spectrum with a fractional bandwidth over 100%, extending to the mid-infrared regim
230 tubes exhibits unique photostability, narrow bandwidth, penetration through biological media, environ
234 iable OTTDL has an extremely broad operation bandwidth practically exceeding several tens of THz, whi
238 e first measurement of excess noise and gain-bandwidth product in III-V nanopillars exhibiting substa
240 as well as the ability to engineer the time-bandwidth product of the signal's envelope to match that
241 of the number of orthogonal modes (the time-bandwidth product) available in the transmission interva
244 phic imaging methods can achieve large space-bandwidth-products by performing pixel super-resolution
246 n of Cerenkov radiation allows for selective bandwidth quenching, in which a band of photons is quenc
247 ntally different method for producing narrow-bandwidth radiation from a broad spectral bandwidth curr
248 hnique that allows high sensitivity and high bandwidth readout of discrete quantum states of metallic
250 three benefits: reduced excitation spectral bandwidth, reduced emission cross-talk between colocaliz
253 heory (DFT) calculations reveals significant bandwidth renormalization and damping effects due to the
258 and parametric, boost the energy, their gain bandwidth restricts the attainable pulse duration, requi
259 ructural building blocks that facilitate the bandwidth-scaled inversion-symmetry breaking are common
260 laminations, analyzed for color content and bandwidth, showed distinctive changes that were coupled
262 The photon energy exceeds the electronic bandwidth, so that completely filled or completely empty
263 how that an effective absorption (above 90%) bandwidth spans from 10.4 GHz to 19.7 GHz, namely a 62%
264 by the relatively high current noise and low bandwidth stemming from the relatively high capacitance
265 rcopallium (RA), controls syllable and trill bandwidth stereotypy, while not significantly affecting
268 oltage pulses, have been employed to achieve bandwidths suitable for applications such as video-frame
271 awake mice revealed that L2 cells had higher bandwidth than L3 cells, consistent with the laminar dif
273 airflow with full fidelity over a frequency bandwidth that easily spans the full range of human hear
275 istence of QKD with data has been limited to bandwidths that are orders of magnitude below those comm
276 ectromagnetic spectrum as a fully-functional bandwidth, the development of a family of efficient THz
277 inimal THz absorption across the measurement bandwidth, the orientations of the eigenmodes of propaga
278 ing solution, owing to their octave spanning bandwidths, the ability to achieve group-velocity disper
279 with different velocities and source wavelet bandwidths, the method is capable to maximise the accura
281 urrounds, thus allowing neurons with limited bandwidth to encode challengingly large input ranges.
283 ron correlations is accessible by tuning the bandwidth under external and/or chemical pressure, enabl
285 orted, which are uniquely able to operate at bandwidths up to 1.5 kHz whilst maintaining internal gai
286 -order modulation formats within the Nyquist bandwidth using coherent detection brings attractive per
287 in the lattice of the [2]2B radical (overall bandwidth, W = 1.4 eV, in the pure compound) leads to ve
289 using different lag times and kernel density bandwidths were tested to establish the consistency of f
290 x similarly for the low- and gamma-frequency bandwidths, whereas at the low-frequency bandwidth (3-20
291 e transmission rate relies on the modulation bandwidth, which is predominantly determined by the mino
292 low-cost THz-TDS scheme with an ultra-broad bandwidth, which may promote the development and the app
293 pound) leads to very strong narrowing of the bandwidth, which reaches a minimum at [2]2Be (W = 0.3 eV
294 such as metaresonator antennas, have narrow bandwidths, which limits their effective range of freque
300 for both high resolution and a large working bandwidth without sacrificing sensitivity, and we antici
WebLSDに未収録の専門用語(用法)は "新規対訳" から投稿できます。