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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.
39                              To date, octave bandwidth (25-50 THz) single-channel links have been dem
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
44 mic range of over 100 dB at a broad spectral bandwidth across the UV-NIR range.
45 g with artificial sound sequences matched in bandwidth, amplitude, and duration but differing in spec
46 (2), and delivers 152 fs pulses with 52.8 nm bandwidth and 0.19 nJ pulse energy.
47 tive resonant absorption, where the resonant bandwidth and absorption intensity can be engineered by
48 ds whose emission exhibits both a very large bandwidth and an extremely large Stokes shift.
49 se Eu(2+) luminescence exhibits a very large bandwidth and an extremely large Stokes shift.
50 ometer with unprecedented 400 kHz excitation bandwidth and capable of high-throughput acquisition of
51            We show a flat, wide, and tunable bandwidth and center frequency by controlling the electr
52 able optical emission filters for tuning the bandwidth and center wavelength.
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
55 on, duct deformability extends the frequency bandwidth and enhances the high frequency gain.
56 s a route to spatial control over electronic bandwidth and ferromagnetism through the creation of oct
57 FCS systems in terms of sensitivity, optical bandwidth and frequency-resolution.
58 onstrated with low threshold voltage, narrow bandwidth and high efficiencies.
59 oscopy (CE-DFCS) combines the inherent broad bandwidth and high resolution of an optical frequency co
60 rage with extreme spatial confinement, broad bandwidth and high tunability.
61 lows for fine tuning of spectral resolution, bandwidth and imaging speed while maintaining full duty
62 ian tails, sub-meV ( approximately 620 mueV) bandwidth and improved momentum resolution.
63 n (MTJ)-based STNO, which saves transmission bandwidth and in principle should minimize attenuation f
64 , for widening and/or controlling of blazing bandwidth and incident angle range of operation.
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
70              In addition, smaller changes in bandwidth and preferred direction were observed in some
71 h iron-based magnetic particles improves the bandwidth and S11 of embedded antennas.
72            Ultrafast fiber lasers with broad bandwidth and short pulse duration have a variety of app
73 local dynamics can be quantified with 50 kHz bandwidth and subnanometre amplitudes.
74 proach severs the link between the resonance bandwidth and the cavity-photon lifetime, thereby promis
75 le, biocompatible and have a narrow emission bandwidth and visible fluorescence properties.
76  linear regression models with a data-driven bandwidth and with the algorithm for selecting the bandw
77 trum with topological features and where the bandwidths and bandgaps are dramatically broadened.
78 act, excitation and inversion over a defined bandwidth, and also with bounded amplitude.
79 two effective spins for phonons over a broad bandwidth, and strong spin-orbit coupling is realized by
80 well described by a Gaussian function with a bandwidth around 25 degrees .
81 mes as short as 3 ps implying photodetection bandwidths as wide as 300 GHz.
82 e levels increased firing rates and expanded bandwidths, as is usually seen for FRAs obtained without
83 o-noise ratio from 7 to 9 in a 1 kHz imaging bandwidth at modest illumination intensity.
84 levels reduced firing rates and narrowed FRA bandwidths; at higher SNRs, however, increasing the tone
85 use of low-cost equipment but diminishes the bandwidth available to end-users.
86 on efficiencies of 80% at 825 nm and a broad bandwidth between 630 nm and 1,050 nm.
87 also significant broadening of the resonance bandwidth between laser frequency and that of electron b
88 ber of resonances and results in significant bandwidth broadening.
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
94 ely 80% absorption for an optimized spectral bandwidth centered around 8.8 mum.
95 ; high-frequency ultrasound (156% fractional bandwidth centred around 13.5 MHz) was generated photoac
96 dth and with the algorithm for selecting the bandwidth chosen ex ante.
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
99                                  Electronics-bandwidth-compatible (20 GHz) soliton mode locking is ac
100 rface exists that provides both an efficient bandwidth compression and a substantial frequency transl
101                                     When the bandwidth compression factor alpha is set to 0.8 in FrCT
102 icantly outperforming spectral filtering for bandwidth compression.
103 photoconductive antennas has been limited by bandwidth constraints of their antennas and photoconduct
104                                   Finally, a bandwidth contour plot depending on the stress and opera
105 hree manipulations of certainty (orientation bandwidth, contrast, and duration).
106 delays as long as 1.8 ps detected across the bandwidth covered by 80-fs laser pulses.
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
111  period Deltat inversely proportional to the bandwidth (Deltat.Deltaomega 2pi).
112 oviders, to satisfy the continuously growing bandwidth demand.
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
117 these devices to demonstrate low-noise, high-bandwidth DNA translocation measurements.
118 n response time and a 25% decrease in system bandwidth due to load.
119 metamaterials are limited in their operation bandwidth due to their resonant nature.
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
122                        Ultra-intense, narrow-bandwidth, electromagnetic pulses have become important
123 -electronic localization has a narrow usable bandwidth, electronically controlled optical localizatio
124 easily recorded with fast detectors and high-bandwidth electronics.
125 regate-like molecular packing, offers narrow-bandwidth emission, and has been successfully applied to
126 als, which imposes excessive requirements on bandwidth, energy and computation capacity.
127 al across such a large synaptically relevant bandwidth enhances the response to small-amplitude acidi
128        The produced peaks show the narrowest bandwidths ever reported for a consumable-free thermal m
129                   However, the initial Fixed Bandwidth (FB) implementation is both inefficient and un
130 m laser source with a tunable wavelength and bandwidth filter.
131 ontinuum laser with a tunable wavelength and bandwidth filter.
132 cy qubits to the ions ( approximately 50 GHz bandwidth) followed by retrieval with 98.7% fidelity.
133                              The ultranarrow bandwidth for detection results from the helical ribbons
134 s, while maintaining extremely high temporal bandwidth for single-DNA sensing.
135 band absorption of 90% with a 28% fractional bandwidth from 125-165 GHz.
136 sistor that is polarization-sensitive over a bandwidth from approximately 400 nm to 3,750 nm.
137 ustic transmitters and receivers have a wide bandwidth, from the audible region (20 approximately 20
138 onstrated their high sensitivity and a -6 dB bandwidth greater than 40%.
139 n laser technology, X-rays with small enough bandwidth have become available, allowing the investigat
140          Our results suggest that the narrow bandwidth, high QY, and large Stokes shift are promising
141               The combination of ultra-broad bandwidth, high responsivities and fast operating speeds
142                    Through the use of a high bandwidth, high signal/noise measurement system, NP impa
143 e-photon source with a tunable frequency and bandwidth in a diamond waveguide.
144 ation regime up to a 10-GHz-scale modulation bandwidth in principle.
145  narrow spectral band ( approximately 900 nm bandwidth in the mid-infrared) with the intensity above
146 er frequencies and the highest (p<0.05) half-bandwidth in the nuasCH2 and nusCH2 bands.
147  Information transmission is demonstrated at bandwidths in the Hz and MHz ranges.
148 ow power consumptions and high communication bandwidths in tunnel environments.
149 ear and nonlinear optical effects over broad bandwidths in ultrathin devices.
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
154         Significant improvement in detection bandwidth is demonstrated by encapsulating the ring reso
155               The consequence of the reduced bandwidth is that openings or shuttings that are shorter
156 tem, which is a function of the light source bandwidth, is sufficient to resolve retinal features at
157 >-2 dB and an extinction ratio >15 dB over a bandwidth larger than 60 nm.
158 exes is measured by merging a tunable narrow-bandwidth laser beam with the ions.
159 .6 dB if corrected for detection losses) and bandwidths less, similar90 kHz.
160 ure communication systems, especially in the bandwidth-limited applications.
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
165           We report shot-noise-limited, high-bandwidth measurements of Brownian motion of micrometer-
166                                         High-bandwidth measurements of the ion current through hafniu
167 in turn indicates the viability of petahertz-bandwidth metrology with a solid-state device.
168         However, due to the limited resonant bandwidth, most periodic plasmonic nanostructures cannot
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.
171 t contains only 10(5) photons in a spectral bandwidth of 50% full width at half maximum (FWHM).
172  the pump wavelength, broadband OFC with the bandwidth of >180 nm and the frequency-spacing varying f
173 tinction ratio as high as 9 dB and operation bandwidth of 0.5 THz.
174                   A maximum -3 dB modulation bandwidth of 1.18 GHz is measured.
175         The integrated noise is 220 fA for a bandwidth of 100 Hz, allowing for detection of pA curren
176 l quantum encryption system operating with a bandwidth of 200 Gb/s over a 100 km fibre.
177 ave over 30 dB sidelobe suppression and 3-dB bandwidth of 200 MHz, providing good filter selectivity.
178                                     The half-bandwidth of 2923 cm(-1) band and area of 3220 cm(-1) ba
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
183 n induce recovery outside the spatiotemporal bandwidth of blindsight.
184 s, we also determined the orientation-tuning bandwidth of correlated activity between pairs of LGN ne
185 ion, thus crucially enhancing the collective bandwidth of endothelial responses to agonists.
186 a comparable sensitivity, response time, and bandwidth of existing methods.
187 sms, of which variability in the orientation bandwidth of linear filtering is the most important.
188 1), referenced to incident illumination, and bandwidth of nearly 3 kHz.
189  a different idea: inhibition can expand the bandwidth of neural coding.
190 ed in the low-frequency regimes and in their bandwidth of operation because they require impractical
191                                    Hence the bandwidth of optical rotation is found to be relatively
192                                   The finite bandwidth of our experimental setup sets the lifetime of
193 ion, with potential functions in setting the bandwidth of postsynaptic responses, sensitivity to mech
194                           However, operation bandwidth of previously demonstrated plasmonic photocond
195 e new proposed mechanism greatly extends the bandwidth of RCS reduction.
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
198 ction assumed by the model regardless of the bandwidth of single units.
199                 However, the broad radiation bandwidth of such plasma devices limits the source brigh
200                         Analyses of the half-bandwidth of the 2923 cm(-1) band and the area of the 32
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.
205 ty was controlled by varying the orientation bandwidth of the filter.
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
208 e Q of the amplifier can be specified by the bandwidth of the injected Raman signal.
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
212                     Fourthly, the modulation bandwidth of the plasmonic light-sources is enhanced to
213 and the thin film emit light within a narrow bandwidth of the visible spectrum and with a high quantu
214         With a high dynamic range, a tunable bandwidth of up to 30 MHz and an in situ reconfigurabili
215                         Spectral content and bandwidth of vascular electrocorticography were comparab
216 oaden the accumulative operational frequency bandwidth of vibration energy harvesting for enabling se
217 avity programmable filter the dispersion and bandwidth of which can be software configured.
218         Our work also quantified the minimum bandwidths of optical receivers and signal processing de
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
221 over electronic methods due to the ultrawide bandwidth offered by the optical carriers.
222  study the effects of filter positioning and bandwidth on a number of three-chemical systems.
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
225 m bins and community sizes that of histogram bandwidths or bin sizes.
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
229 timated as 10.7 bits per symbol with 500 GHz bandwidth over 2,000 km.
230 tubes exhibits unique photostability, narrow bandwidth, penetration through biological media, environ
231  enable further scaling of the communication bandwidth per fibre.
232 oping devices with unprecedentedly high time-bandwidth performance.
233  plasmonic absorber counterparts in terms of bandwidth, polarization and angle independence.
234 iable OTTDL has an extremely broad operation bandwidth practically exceeding several tens of THz, whi
235 tore and process such states with large time-bandwidth product and multimode capacities.
236  a telecom-wavelength (1.53 mum) with a time-bandwidth product approaching 800.
237 al coherent imaging technique for high space-bandwidth product imaging.
238 e first measurement of excess noise and gain-bandwidth product in III-V nanopillars exhibiting substa
239                       The quantum efficiency-bandwidth product of 105 GHz is the highest for photodet
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
242 achieving a competitive resolution and space-bandwidth-product.
243 cess noise factors compared to bulk and gain-bandwidth products greater than 200 GHz.
244 phic imaging methods can achieve large space-bandwidth-products by performing pixel super-resolution
245 d current sources to produce broad or narrow bandwidth pulses.
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
249                              Continuous wide-bandwidth recordings from patients undergoing intracrani
250  three benefits: reduced excitation spectral bandwidth, reduced emission cross-talk between colocaliz
251                                    Only 3.6% bandwidth reduction has been observed comparing to that
252 t make up melanin as Gaussian absorbers with bandwidth related via Frenkel excitons.
253 heory (DFT) calculations reveals significant bandwidth renormalization and damping effects due to the
254 creased data storage costs and communication bandwidth requirements.
255  its first subharmonic, thus reducing device bandwidth requirements.
256             The combination of the potential bandwidth resource around 2 mum with the soliton molecul
257       SPPs can provide a gate-tunable, broad-bandwidth response, but suffer from high optical losses;
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
261                   Because of their extensive bandwidth, single-cycle fields cannot be emitted or ampl
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
266  while having no effect on syllable or trill bandwidth stereotypy.
267 y due to the lack of THz emitters with broad bandwidth suitable for the purpose.
268 oltage pulses, have been employed to achieve bandwidths suitable for applications such as video-frame
269 ntered at 500 Hz and 2500 Hz, with criterion bandwidth tailored for each participant.
270 eyed in received synaptic inputs, at a wider bandwidth than for rodents.
271 awake mice revealed that L2 cells had higher bandwidth than L3 cells, consistent with the laminar dif
272 l microcircuits relay information at a wider bandwidth than rodent microcircuits.
273  airflow with full fidelity over a frequency bandwidth that easily spans the full range of human hear
274 fast transient signals within a user-defined bandwidth that exceeds 500 Hz.
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
280 ments to be strictly phase locked at 0.04 Hz bandwidth to droplets generated at 3.50 Hz.
281 urrounds, thus allowing neurons with limited bandwidth to encode challengingly large input ranges.
282                         We use this enhanced bandwidth to resolve signals from multiple nanoparticles
283 ron correlations is accessible by tuning the bandwidth under external and/or chemical pressure, enabl
284 bels (dB) and a fast photoresponse with 3-dB bandwidth up to 3 MHz.
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
288 ent mass resolution of 27 attograms in 1-kHz bandwidth was previously achieved by Lee et al..
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
295 ors can have high modulation speed and broad bandwidth, while being compact.
296 ossible to characterize those fields at high bandwidth with arbitrary orientations.
297 aved memory and logic for unprecedented data bandwidth with reduced energy consumption.
298 s of each seizure was performed to determine bandwidths with significant power at ictal onset.
299  10.4 GHz to 19.7 GHz, namely a 62% fraction bandwidth, with only 2 mm thickness.
300 for both high resolution and a large working bandwidth without sacrificing sensitivity, and we antici

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