ライフサイエンスコーパス: bandwidth

1 rom 16 channels sampled at 19.5 KHz (9.7 KHz bandwidth).

2 for ultrafast nonlinear optics with scalable bandwidth.

3 rits of high compactness, low loss and broad bandwidth.

4 enhance sensitivity across a wide frequency bandwidth.

5 owing distinct debt accounts consume mental bandwidth.

6 ission (<1 dB loss) maintained over a 200 nm bandwidth.

7 ectron-electron interaction and the miniband bandwidth.

8 se equivalent pressure <100 Pa over a 20 MHz bandwidth.

9 goes hand-in-hand with higher efficiency and bandwidth.

10 is to increase their intensity and frequency bandwidth.

11 with an Eddy current effect in the absorbing bandwidth.

12 localization, which improves with increasing bandwidth.

13 le of which is a substantial fraction of the bandwidth.

14 n the resonance frequency and an increase of bandwidth.

15 alanced performance across the whole optical bandwidth.

16 neered to be anomalous over moderately broad bandwidth.

17 noscale, while maintaining a broad operation bandwidth.

18 ved, with no fundamental limit on the system bandwidth.

19 ma channel, leads to a few percent radiation bandwidth.

20 eme with 2 nm spatial resolution and 150 MHz bandwidth.

21 that falls within the intermediate frequency bandwidth.

22 hod to vastly reduce the required electrical bandwidth.

23 sustain transmission over a broad frequency bandwidth.

24 n terms of the figure of merit and operating bandwidth.

25 e of increased hydraulic pressure and sensor bandwidth.

26 al frequency across hundreds of terahertz of bandwidth.

27 can be stored in the system and the system's bandwidth.

28 esonances and broaden the perfect absorption bandwidth.

29 ion, tuning and stabilization with megahertz bandwidth.

30 th added benefits of enhanced efficiency and bandwidth.

31 proved contrast across the spatial frequency bandwidth.

32 attributed to differences in cochlear filter bandwidths.

33 amentally different in their frequencies and bandwidths.

34 iconductors with wide valence and conduction bandwidths.

35 nsertion loss, size, and/or narrow operation bandwidths.

36 ar responses over broad spatial and temporal bandwidths.

37 ct vibrational frequencies, intensities, and bandwidths.

38 ork for sensing low-power (sub muW) and high-bandwidth (0.1-0.5 kHz) ionic currents.

39 ollimated (<1 degrees divergence) and narrow bandwidth ( 10% energy spread) proton beamlet of 10(7) p

40 conducting qubit frequencies (gigahertz) and bandwidths (10 kilohertz - 1 megahertz) remains a challe

41 quency measurement range limited only by the bandwidth (100 GHz) of current electro-optic modulators.

42 using thermal heaters have limited actuation bandwidths(11,12) of up to 10 kilohertz.

43 m efficiency up to 11% and a narrow emission bandwidth (65 nm fwhm).

44 er (k-space) spectrometer for an ultra-broad bandwidth (760 nm-920 nm) SD-OCT, whereby a combination

45 n the crystal-slab plane, a larger operating bandwidth, a much smaller footprint, compatibility with

46 oss sections are independent of the spectral bandwidth across the range of ~250 to <20 cm(-1).

47 Consequently, megahertz-bandwidth actuation and locking of microcombs have only

48 e selectivity, SF bandwidth, and orientation bandwidth-all of which were found to be topographically

49 ometer with unprecedented 400 kHz excitation bandwidth and capable of high-throughput acquisition of

50 We show a flat, wide, and tunable bandwidth and center frequency by controlling the electr

51 able optical emission filters for tuning the bandwidth and center wavelength.

52 h monochromator-produced light, any spectral bandwidth and centre wavelength from 390 to 730 nm can b

53 services on par with fibre services, both in bandwidth and cost.

54 on, duct deformability extends the frequency bandwidth and enhances the high frequency gain.

55 re enabling for applications requiring broad bandwidth and high efficiency including energy harvestin

56 capable of supporting unprecedentedly large bandwidth and high peak power while maintaining high spe

57 lows for fine tuning of spectral resolution, bandwidth and imaging speed while maintaining full duty

58 n (MTJ)-based STNO, which saves transmission bandwidth and in principle should minimize attenuation f

59 , for widening and/or controlling of blazing bandwidth and incident angle range of operation.

60 The line bandwidth and intensity are defined by the shape and len

61 dom by dynamically addressing the modulation bandwidth and optical spectral tuning of a probe optical

62 the increasing demand for data communication bandwidth and overcome the limits of electrical intercon

63 By investigating the factors limiting their bandwidth and overcoming them, we demonstrate here excep

64 In addition, smaller changes in bandwidth and preferred direction were observed in some

65 the substrates losses that leads to improved bandwidth and radiation properties.

66 rys nuttalli by testing for changes in trill bandwidth and rate-the specific trill structure componen

67 h iron-based magnetic particles improves the bandwidth and S11 of embedded antennas.

68 th the accumulation of massive data, network bandwidth and storage requirements are rapidly increasin

69 proach severs the link between the resonance bandwidth and the cavity-photon lifetime, thereby promis

70 s oscillation frequency linearly over a wide bandwidth and with precise phase-dependent spiking.

71 linear regression models with a data-driven bandwidth and with the algorithm for selecting the bandw

72 trum with topological features and where the bandwidths and bandgaps are dramatically broadened.

73 act, excitation and inversion over a defined bandwidth, and also with bounded amplitude.

74 asure maps of RF size, phase selectivity, SF bandwidth, and orientation bandwidth-all of which were f

75 do so, physical sources of entropy with wide bandwidth are required which are able to provide truly r

76 ll tuning curve attributes (such as gain and bandwidth) are equally useful for evaluating the encodin

77 well described by a Gaussian function with a bandwidth around 25 degrees .

78 e levels increased firing rates and expanded bandwidths, as is usually seen for FRAs obtained without

79 a photon flux of ~ 1.4 x 10(6) photons/s/1% bandwidth at 300 eV.

80 nJ of pulse energy, and a 21.66 nm spectral bandwidth at a peak wavelength of 1899.5 nm.

81 f mathematical functions, operate over broad bandwidths at high speeds, and work equally well at high

82 levels reduced firing rates and narrowed FRA bandwidths; at higher SNRs, however, increasing the tone

83 use of low-cost equipment but diminishes the bandwidth available to end-users.

84 also significant broadening of the resonance bandwidth between laser frequency and that of electron b

85 inuous 180 degrees phase shift across a wide bandwidth, between 35 and 65 GHz.

86 ber of resonances and results in significant bandwidth broadening.

87 irection selectivity, and temporal frequency bandwidth, but other dimensions also showed differences

88 e approach to improving readout fidelity and bandwidth (BW) is cryogenic amplification, where the sig

89 s to the visible range while compressing the bandwidth by a factor of 7.47 under preservation of non-

90 head with high spatial resolution and large bandwidth by coherent control of single electron and nuc

91 ffers the potential to expand communication 'bandwidth' by using biomolecules and providing electroch

92 on a triangular superlattice(5,6) where the bandwidth can be tuned continuously with the vertical di

93 ; high-frequency ultrasound (156% fractional bandwidth centred around 13.5 MHz) was generated photoac

94 dth and with the algorithm for selecting the bandwidth chosen ex ante.

95 eneration efficiency with remarkably broader bandwidth compared to standard inorganic 0.5 mm thick Zn

96 nse amplitudes and narrower voxelwise tuning bandwidths compared with a group of typically sighted in

97 Electronics-bandwidth-compatible (20 GHz) soliton mode locking is ac

98 rface exists that provides both an efficient bandwidth compression and a substantial frequency transl

99 When the bandwidth compression factor alpha is set to 0.8 in FrCT

100 icantly outperforming spectral filtering for bandwidth compression.

101 photoconductive antennas has been limited by bandwidth constraints of their antennas and photoconduct

102 Finally, a bandwidth contour plot depending on the stress and opera

103 hree manipulations of certainty (orientation bandwidth, contrast, and duration).

104 delays as long as 1.8 ps detected across the bandwidth covered by 80-fs laser pulses.

105 and their actuation nonlinearity and limited bandwidth create further challenges for achieving closed

106 ow-bandwidth radiation from a broad spectral bandwidth current source, which takes advantage of the i

107 ring asserts that any type of system, having bandwidth Deltaomega, can interact with a wave over only

108 period Deltat inversely proportional to the bandwidth (Deltat.Deltaomega 2pi).

109 oviders, to satisfy the continuously growing bandwidth demand.

110 le potential to satisfy today's ever-growing bandwidth demands.

111 nd a dielectric, hold the key to future high-bandwidth, dense on-chip integrated logic circuits overc

112 ortantly, optical fibers allow for very high bandwidth densities (in the Tbps/mm(2) range) by carryin

113 rving full measurement characteristics (e.g. bandwidth, determination of capacitive/inductive contrib

114 ic Hamiltonian and an increase in electronic bandwidth due to counterlayer-induced bond-angle changes

115 ve high wavelength resolution for a relevant bandwidth e.g. through a chopper system.

116 ng, but these techniques generally limit the bandwidth, efficiency and active times of the quantum in

117 tems offer significantly improved power- and bandwidth-efficiency, but require fundamental simplifica

118 Ultra-intense, narrow-bandwidth, electromagnetic pulses have become important

119 the detection of a wide range of ultrasound bandwidths enables the distinction of vessels of differi

120 al across such a large synaptically relevant bandwidth enhances the response to small-amplitude acidi

121 perceptually-relevant equivalent rectangular bandwidth (ERB) frequency scale, the ERB(N)-number scale

122 tral frequencies in the extreme UV range and bandwidths exceeding tens of electronvolts.

123 rashort light pulses with the total spectral bandwidth extending over ultraviolet, visible and near-i

124 However, the initial Fixed Bandwidth (FB) implementation is both inefficient and un

125 For example, high-bandwidth feedback control of frequency combs is used in

126 ontinuum laser with a tunable wavelength and bandwidth filter.

127 sed strategies SERS provides narrow spectral bandwidths, fluorescence quenching and multiplexing abil

128 cy qubits to the ions ( approximately 50 GHz bandwidth) followed by retrieval with 98.7% fidelity.

129 munication systems and allows reduced system bandwidth for a given communications specification.

130 The ultranarrow bandwidth for detection results from the helical ribbons

131 s, while maintaining extremely high temporal bandwidth for single-DNA sensing.

132 nd structures as they can greatly impact the bandwidth, frequency resolution, signal-to-noise ratio,

133 ity of 10.79 mV/Pa, a wide working frequency bandwidth from 0 Hz to 40 Hz, good stability, and decent

134 e noise-equivalent power (2 pW Hz(-1/2)) and bandwidth (from 10 kHz up to 1.3 MHz), challenging the s

135 tion of this resonance demonstrates a device bandwidth greater than 83x beyond the conventional Bode-

136 centrated, we show an increase in absorption bandwidths (>100% of the resonance frequency).

137 One song trait (trill bandwidth) had a quadratic relationship with future surv

138 However, the hologram bandwidth has remained too low for any practical use.

139 n laser technology, X-rays with small enough bandwidth have become available, allowing the investigat

140 eased computing efficiency and communication bandwidth have pushed the current semiconductor technolo

141 st promising technologies towards ultra-wide bandwidth, high-brightness, and spatially coherent light

142 ration of the quadrupole with increased mass bandwidth improved the signal-to-noise ratios significan

143 e-photon source with a tunable frequency and bandwidth in a diamond waveguide.

144 Our results reveal that the metallic bandwidth in GNRs can be tuned over a wide range by cont

145 ation regime up to a 10-GHz-scale modulation bandwidth in principle.

146 narrow spectral band ( approximately 900 nm bandwidth in the mid-infrared) with the intensity above

147 er frequencies and the highest (p<0.05) half-bandwidth in the nuasCH2 and nusCH2 bands.

148 , is able to sort three colors over a 100 nm bandwidth in the visible regime, independently of the po

149 monstrate here exceptionally fast OLEDs with bandwidths in the hundreds of MHz range.

150 ow power consumptions and high communication bandwidths in tunnel environments.

151 ear and nonlinear optical effects over broad bandwidths in ultrathin devices.

152 ks promise access to the high speed and high bandwidth inherent to optical systems, thus enabling the

153 However, although the advantage conferred by bandwidth is clear, we currently know little about how t

154 Significant improvement in detection bandwidth is demonstrated by encapsulating the ring reso

155 Although the detection bandwidth is naturally narrow due to the highly resonant

156 Although ULF has very low bandwidth it is very reliable, penetrating and difficult

157 The capping flat bands with bandwidth less than 0.2 eV run through the whole Brillou

158 .6 dB if corrected for detection losses) and bandwidths less, similar90 kHz.

159 lder with an interchangeable narrow-spectral bandwidth light-emitting diode (LED) block that can be u

160 Until recently, this time-bandwidth limit has been considered fundamental, arising

161 s been quite challenging due to the inherent bandwidth limitations.

162 rary 2D spatial/polarisation wavefronts at a bandwidth limited rate of 4.4 THz.

163 ure communication systems, especially in the bandwidth-limited applications.

164 properties (e.g. ultrafast operation, large bandwidths, low cross-talk).

165 imultaneously owns high efficiency and broad bandwidth may open a new way for application in imaging,

166 Four bandwidth methods (reference, normal scale, plug-in and

167 in turn indicates the viability of petahertz-bandwidth metrology with a solid-state device.

168 manufacturable design exhibiting attenuation bandwidths more than two times larger than the equivalen

169 However, due to the limited resonant bandwidth, most periodic plasmonic nanostructures cannot

170 he SNR was 0.93 +/- 0.07 per 1 mV in a 1-kHz bandwidth (n = 42 post-synaptic potentials from 5 cells,

171 Here we show an ultra-high bandwidth nano-electronic interface to the interior of l

172 ) and present an integrated, sensitive, high-bandwidth nanophotonic interface for carbon nanotube res

173 with laser stimulation to improve frequency bandwidth, not requiring attachment to specific vibrator

174 the pump wavelength, broadband OFC with the bandwidth of >180 nm and the frequency-spacing varying f

175 However, the narrow frequency bandwidth of (1)H NMR spectroscopy leads to a severe ove

176 urface that is shown to exhibit a very large bandwidth of 0.350-0.385 THz with an average radiation g

177 while providing 20 dB of protection within a bandwidth of 10 MHz against amplified noise reflected of

178 frequencies upto 21 GHz and with a relative bandwidth of 10(-4) ~ 10(-5).

179 TE or TM polarized incident wave it presents bandwidth of 118% (7.7-29.9 GHz) or 100.5% (9.9-29.9 GHz

180 ency higher than 0.8 for 6.9-29.9 GHz (i.e., bandwidth of 125%) regardless of polarization, while the

181 le the curved absorber for 6.6-29 GHz (i.e., bandwidth of 126%) or for 10.5-29.6 GHz (i.e., bandwidth

182 ncy up to 1.98 GHz V(-1), a broad modulation bandwidth of 17.5 GHz, while with a tiny electro-optic m

183 ption of 99.94% at 4.3 mum and an absorption bandwidth of 170% FWHM on 15.8 mum center wavelength, co

184 con-photonics platform featuring a detection bandwidth of 2.5 THz with a 65 dB dynamical range.

185 l quantum encryption system operating with a bandwidth of 200 Gb/s over a 100 km fibre.

186 The transmitted ultrasound had a -6 dB bandwidth of 31.3 MHz and a peak-to-peak pressure of 1.8

187 um reflection loss of -44.7 dB and absorbing bandwidth of 4.7 GHz at -10 dB are achieved in composite

188 r the entire fiber length and operating at a bandwidth of 470 kHz, orders of magnitude larger than an

189 at contains only 10(5) photons in a spectral bandwidth of 50% full width at half maximum (FWHM).

190 fer a signal/noise ratio of ~10(6) , a large bandwidth of 543 kHz and an ultralow detection limit of

191 ndwidth of 126%) or for 10.5-29.6 GHz (i.e., bandwidth of 95%), depending the polarization.

192 rmining the material quality and operational bandwidth of a broad range of optoelectronic devices.

193 were further improved by increasing the mass bandwidth of a quadrupole mass filter.

194 shifts of resonance frequency and resonance bandwidth of a quartz crystal microbalance (QCM) contact

195 se times on the order of 3 mus, and a signal bandwidth of about 300 kHz.

196 meter, dynamic gain, which characterizes the bandwidth of action potential encoding by a neuron, and

197 ricated and measured showing increase in the bandwidth of blazing/specular-reflection-rejection, demo

198 This broadened bandwidth of Ca(2+) influx is translated by cells into d

199 s, we also determined the orientation-tuning bandwidth of correlated activity between pairs of LGN ne

200 the ratio of the Coulomb interaction to the bandwidth of each individual VHS (U/t) is maximized, whi

201 Reducing the energy bandwidth of electrons in a lattice below the long-range

202 a comparable sensitivity, response time, and bandwidth of existing methods.

203 tures (0-300 Hz) extend beyond the frequency bandwidth of head movements experienced during everyday

204 Hz, beyond the state-of-the-art experimental bandwidth of less than 10 GHz.

205 The limited per-pixel bandwidth of most microscopy methods requires compromise

206 1), referenced to incident illumination, and bandwidth of nearly 3 kHz.

207 AM) of light show promise for increasing the bandwidth of optical communication networks.

208 computational infrastructure and doubled the bandwidth of our connection to the worldwide web.

209 at these repetition rates due to the limited bandwidth of photodiodes and electronics.

210 ion, with potential functions in setting the bandwidth of postsynaptic responses, sensitivity to mech

211 However, operation bandwidth of previously demonstrated plasmonic photocond

212 e new proposed mechanism greatly extends the bandwidth of RCS reduction.

213 ction assumed by the model regardless of the bandwidth of single units.

214 However, the broad radiation bandwidth of such plasma devices limits the source brigh

215 ificant differences in the frequency or half-bandwidth of the 2923 and 2853 cm(-1) infrared bands wer

216 on is always limited by the narrow-frequency bandwidth of the acoustic waves because of the large att

217 Throughout the entire Brillouin zone, the bandwidth of the flat band is suppressed by an order of

218 ugh the whole Brillouin zone, especially the bandwidth of the flat band of out-of-plane orbitals is l

219 f OCT is limited to about 1 mum, even if the bandwidth of the light covers a wide spectral range.

220 herence is related to the intrinsic spectrum bandwidth of the light source, while spatial coherence c

221 Specifically, increasing the mass bandwidth of the quadrupole improved the size detection

222 sation of some model parameters, such as the bandwidth of the spectral filter spectral filtering and

223 r more time, will inevitably also reduce the bandwidth of the system.

224 equency of songs, and duration and frequency bandwidth of trills).

225 With a high dynamic range, a tunable bandwidth of up to 30 MHz and an in situ reconfigurabili

226 Spectral content and bandwidth of vascular electrocorticography were comparab

227 avity programmable filter the dispersion and bandwidth of which can be software configured.

228 ansitions primarily acting by regulating the bandwidth of whitening.

229 ique capability of changing the force with a bandwidth of ~10 kHz.

230 um wavelengths) and can also detect spectral bandwidths of known lineshapes with high sensitivity.

231 Our work also quantified the minimum bandwidths of optical receivers and signal processing de

232 t the precise combination of confinement and bandwidth offered by phonon polaritons allows for the ab

233 st photodetectors can enable low power, high bandwidth on-chip optical interconnects for silicon inte

234 gh signal-to-noise ratio, and broad spectral bandwidth opens up opportunities for precision spectrosc

235 The high-bandwidth optical-stimulation capacity of the device mig

236 ton recuperation are limited by insufficient bandwidth or parasitic absorption, resulting in large ef

237 ch devices have been limited to either small bandwidths or have disregarded the phase of the impingin

238 timated as 10.7 bits per symbol with 500 GHz bandwidth over 2,000 km.

239 mal cost, wide beam scanning angle and broad bandwidth, over phased array antennas and reflector ante

240 nomenon is confined to very narrow frequency bandwidths owing to the mono-resonance characteristics o

241 ssian, with independent center frequency and bandwidth parameters.

242 GPU hardware architectures that support high-bandwidth peer-to-peer memory accesses among multiple GP

243 oping devices with unprecedentedly high time-bandwidth performance.

244 tend to as low as 1/40 of the noninteracting bandwidth, placing our findings in the degenerate regime

245 Good results are obtained in terms of bandwidth, polarization independence and fabrication sim

246 h accompanying numerical simulations, a time-bandwidth product (TBP) exceeding the 'fundamental' limi

247 ding in particular the violation of the time-bandwidth product constraint that should otherwise apply

248 al coherent imaging technique for high space-bandwidth product imaging.

249 can be broadly applied to enhance the space-bandwidth product of coherent imaging systems using imag

250 otonic structures constrained by a low delay-bandwidth product.

251 An optical buffer featuring a large delay-bandwidth-product-a critical component for future all-op

252 Delay-bandwidth products of ~100 for pulses of width ~1 ps are

253 d current sources to produce broad or narrow bandwidth pulses.

254 ntally different method for producing narrow-bandwidth radiation from a broad spectral bandwidth curr

255 The use of high-bandwidth recording and higher acid concentration allows

256 three benefits: reduced excitation spectral bandwidth, reduced emission cross-talk between colocaliz

257 we now demonstrate that they have a reduced bandwidth, reflecting a significant impairment of their

258 heory (DFT) calculations reveals significant bandwidth renormalization and damping effects due to the

259 erived optical conductivity spectra with the bandwidth-renormalization factors obtained by many-body

260 neuron pools is shared across all frequency bandwidths (representing cortical and spinal input) asso

261 -standing issues associated with information bandwidth requirements and power-handling capabilities.

262 its first subharmonic, thus reducing device bandwidth requirements.

263 creased data storage costs and communication bandwidth requirements.

264 Next, in order to increase the frequency bandwidth, resistively loaded traces, printed by convent

265 The combination of the potential bandwidth resource around 2 mum with the soliton molecul

266 SPPs can provide a gate-tunable, broad-bandwidth response, but suffer from high optical losses;

267 ructural building blocks that facilitate the bandwidth-scaled inversion-symmetry breaking are common

268 laminations, analyzed for color content and bandwidth, showed distinctive changes that were coupled

269 In combination with a high bandwidth, single-photon sensitive detector, this enable

270 al unique properties, including the spectral bandwidth, small source size and multi-mode emission.

271 The photon energy exceeds the electronic bandwidth, so that completely filled or completely empty

272 rcopallium (RA), controls syllable and trill bandwidth stereotypy, while not significantly affecting

273 while having no effect on syllable or trill bandwidth stereotypy.

274 oltage pulses, have been employed to achieve bandwidths suitable for applications such as video-frame

275 ntered at 500 Hz and 2500 Hz, with criterion bandwidth tailored for each participant.

276 ld consider addressing mental accounting and bandwidth taxes.

277 awake mice revealed that L2 cells had higher bandwidth than L3 cells, consistent with the laminar dif

278 airflow with full fidelity over a frequency bandwidth that easily spans the full range of human hear

279 istence of QKD with data has been limited to bandwidths that are orders of magnitude below those comm

280 tz-substantially exceeding bulk piezo tuning bandwidth-that is extendable to higher frequencies by ov

281 inimal THz absorption across the measurement bandwidth, the orientations of the eigenmodes of propaga

282 ing solution, owing to their octave spanning bandwidths, the ability to achieve group-velocity disper

283 ta is stored in large files, requiring large bandwidth to download and special purpose data manipulat

284 ments to be strictly phase locked at 0.04 Hz bandwidth to droplets generated at 3.50 Hz.

285 ors can achieve sufficient power density and bandwidth to enable controlled flight, illustrating the

286 sing, spiking sparsity, and high interneuron bandwidth to maximize the energy efficiency of neuromorp

287 one might also use the ratio of the shift in bandwidth to the negative shift in frequency as an indic

288 usable, resource (representing unused Wi-Fi bandwidth) to immediate network neighbors.

289 unted soft electronics that incorporate high-bandwidth triaxial accelerometers can capture broad clas

290 orted, which are uniquely able to operate at bandwidths up to 1.5 kHz whilst maintaining internal gai

291 determined covariates, placebo cut-offs, and bandwidths validated our main conclusion.

292 % tunability for each of the four bands with bandwidth values in the range of 30-70 MHz with over 100

293 using different lag times and kernel density bandwidths were tested to establish the consistency of f

294 such as metaresonator antennas, have narrow bandwidths, which limits their effective range of freque

295 ors can have high modulation speed and broad bandwidth, while being compact.

296 disorder degree below which the attenuation bandwidth widens; for high disorder levels, the band gap

297 ossible to characterize those fields at high bandwidth with arbitrary orientations.

298 eriodic parameters (center frequency, power, bandwidth) with aperiodic ones (offset, exponent), compr

299 e (RMS) noise current (18-21 pA over 100 kHz bandwidth, with 50-150 mV bias) when compared to a silic

300 for both high resolution and a large working bandwidth without sacrificing sensitivity, and we antici