ライフサイエンスコーパス: band

1 size, year, or mean HAZ in the 0-3 month age band).

2 road range of frequencies in terahertz (THz) band.

3 eceded by thickening of the RPE-basal lamina band.

4 jecting holes into the semiconductor valence band.

5 bands of 10 and 16 kDa, and in nine a 16-kDa band.

6 robustly generate oscillations in the gamma band.

7 hythmias (VAs) originating from the parietal band.

8 brational fine structure of the ground state band.

9 (10 Hz) or outside (7.5 or 15 Hz) the alpha band.

10 tes optically coupled to the host conduction band.

11 lt of the decay of deep holes in the valence band.

12 iction (n = 12) with a customized pre-shaped band.

13 ift of the squaraine absorption and emission bands.

14 ity spiral surface modes based on spin-split bands.

15 esolution through the use of specific marker bands.

16 t regions is reflected in distinct frequency bands.

17 shed through the operation of multiple shear bands.

18 low-loss and high permittivities at sub-THz bands.

19 with multiple and broadly tunable absorption bands.

20 in WS2 due to the narrow width of its energy bands.

21 preparation in the alpha and beta frequency bands.

22 05) half-bandwidth in the nuasCH2 and nusCH2 bands.

23 PC) measure for the theta and beta frequency bands.

24 s in the alpha (8-13 Hz) and beta (13-18 Hz) bands.

25 immunolabeling revealed that hyperreflective bands 1 and 2, observed in the OCT, correspond to the ou

26 MEN2B) proto-oncogene located on chromosomal band 10q11.21.

27 shown to increase local activity in the beta band [14] and to modulate long-range connectivity within

28 teins used to count cells by flow cytometry, band 3 (CD233), CD71, CD45, and CD41.

29 ersible reaction inside red blood cells, and band 3 [anion exchanger 1 (AE1)] provides a passage for

30 ty, and that the hyporeflective band between bands 3 and 4 corresponds to the RPE nuclei and melanoso

31 Enokitake protein's band (75kDa) reacted specifically with the patient's IgE

32 es the change in wavenumber of the NO ligand band accompanying the isomerization and associated ISC o

33 have demonstrated an important role of gamma-band activity (40-100 Hz) in the feedforward flow of sen

34 mporal pattern of hippocampal high-frequency band activity in single hippocampal contacts.

35 ut how they interact to orchestrate specific band activity remains largely unknown.

36 onse functions were dominated by 10-Hz alpha-band activity.

37 ssociated specifically with prefrontal theta-band activity.

38 flow of visual information mediated by gamma-band activity.

39 sk preceded subsequent stimulus-driven gamma-band activity.

40 study was to analyze the adjustable gastric banding (AGB) natural history on a national basis.

41 igh as 7.23%, ascribed to the HTL's suitable band alignment and excellent hole extraction/collection

42 rs can be achieved by exploiting the type-II band alignment of vertically stacked WS2 /MoS2 semicondu

43 on layer on top of 2H-MoTe2 due to favorable band-alignment.

44 volution and spectral shape of the continuum band, an unusually broad band extending from 2,300 to we

45 The involvement of central theta-band and occipital alpha-band effects are in line with c

46 by describing the competition between shear banding and diffusive relaxation processes, and is remin

47 l-SERS analysis including origin of spectral bands and experimental parameters for spectral reproduci

48 tering and significantly improved prediction bands and uncertainties.

49 he hippocampus, most pronounced in the gamma band, and not explained by spatial movement or anxiety-l

50 es usually occurs only in a narrow frequency band, and the asymmetric frequencies are always within u

51 The RPE band appeared intact in all eyes.

52 n between 10 Hz flicker and endogenous alpha-band ( approximately 10 Hz) oscillations during a select

53 nvolving the filling of holes in the valence band are thought to make important contributions to the

54 ic fingerprint that contains all vibrational band area ratios.

55 irst-principle simulations confirm that such bands arise from distinct acoustic phonons, connecting d

56 tern of plasticity was specific to the gamma band as lower frequency oscillations were suppressed con

57 hin the RPE led us to characterize the third band as the cone phagosomes located in the top of the RP

58 The intensity ratio of Raman bands associated with the scaffolds and HA with the spat

59 These data support the use of gamma-band ASSR as a translational end point in pro-cognitive

60 ctiveness which exceeds 38.4 or 47.5 dB in X-band at 1.6 mm, while the density is merely 0.0058 or 0.

61 f fluorophores featuring a common excitation band at 500 nm, tunable excitation band in the deep red/

62 nce titration of 1 with CN(-) revealed a new band at 540 nm and the nonlinear curve fitting analysis

63 ctrum of 2 reveals a diatomic Co-O vibration band at 770 cm(-1), which provides the conclusive eviden

64 er weights motion preferentially in a narrow band at approximately one-third the radius of the stimul

65 ral observation of displaced water libration bands at ca. 730 cm(-1) upon solvent replacement by adso

66 tion, which effectively tunes the electrical band bending of TiO2 .

67 tact edges over the same length scale as the band-bending.

68 mmunoreactivity, and that the hyporeflective band between bands 3 and 4 corresponds to the RPE nuclei

69 chronous oscillations in the theta and gamma bands between the BLA and interconnected structures have

70 , the desmin cytoskeleton and the attached Z-band-bound thin filaments are degraded after ubiquitinat

71 d to enhance the analyte response and reduce band broadening and/or solute carryovers.

72 ht to be the only factor that contributes to band broadening in electrophoretic separation systems in

73 y phase information was maintained in one SF band but scrambled elsewhere.

74 zed corrections from disorder and additional bands can be small over a significant range of incident

75 lls were more related at a proteome level to banded cells despite a 2-day difference in maturation ti

76 The strength of theta- and beta-band coherence between ACC and FEF but not variations in

77 Around the 2 mum band, conventional saturable absorbers (SAs) possess sma

78 These superior aspects include band convergence, "phonon-glass electron-crystal", multi

79 teins were also observed; especially, in the bands corresponding with 27kDa and 15-17kDa proteins.

80 Finally, we propose that the fourth band corresponds to the accumulation of mitochondria at

81 Those bands could be two isoforms of peach leaf lipid transfer

82 imetals feature zero-dimensional points, the band crossing of nodal-line semimetals forms a one-dimen

83 d crystal structural blocks in real space or band degeneracy at certain points in reciprocal space.

84 ctral patterns among the canonical frequency bands (delta 0-3 Hz, theta 3-7 Hz, alpha 7-13 Hz, beta 1

85 delocalized CT state with well-preserved ion bands despite the strong coupling.

86 ical oscillatory activity within a frequency band dictated by the rhythm of the stimulation source.

87 The alpha band did not respond in a similar manner.

88 The respective Raman marker bands directly show a decrease in the level of glycogen

89 These results suggest that changes in theta band during the epileptogenic period may serve as a diag

90 ts in the formation of a narrow intermediate band (E- band in BAC model) with the minimum at the Gamm

91 e from three- and two-dimensional electronic bands, each with linear dispersion and the additional Be

92 nd gap is affected by a shift of the valence band edge as a function of the layer number.

93 Band edge positions of semiconductors determine their fu

94 nides such as GeS, which display the largest band edge responsivities reported so far.

95 Our method allows us to express the band edge shift current in terms of a few model paramete

96 Our results reveal that the band-edge carrier lifetime increases when the system ent

97 role of VO4 structural motifs and electronic band-edge character in efficient photoanodes, initiating

98 However, access to more than a single band-edge mode for nanolasing has not been possible beca

99 into microscale arrays-can support multiple band-edge modes capable of multi-modal nanolasing at pro

100 ' gain achievable by completely blocking the band-edge state with two electrons.

101 Single band-edge states can trap light and function as high-qua

102 ufficiently broadly that it prevents valence-band-edge states from being thermally depopulated.

103 are complicated by a non-unity degeneracy of band-edge states, because of which multiexcitons are req

104 owever, the presence of trap states near the band edges of TiO2 arising from defects at grain boundar

105 ion covaried positively with occipital gamma-band EEG, consistent with activation of cortical regions

106 nt of central theta-band and occipital alpha-band effects are in line with compensatory neural mechan

107 ts originating from fairly compensated multi-band electronic structure, in full accordance with our f

108 S 3s leading to a relatively low conduction band energy at the Gamma point.

109 Band-engineering techniques should aim to a full control

110 pression, and target reappearances with beta-band enhancement.

111 identify all angle all mode normalized stop bands exceeding 100%, which is larger than what is possi

112 s a versatile technique sensitive to valence band excitations in quantum materials.

113 pe of the continuum band, an unusually broad band extending from 2,300 to well below 1,700 cm(-1) The

114 ration) or 2-stage repairs (pulmonary artery band followed by arterial switch operation).

115 nbow trapping, by taking advantage of a stop-band for surface waves, but also selective mode conversi

116 ncentration is read as the length of colored band formed on the reaction was also demonstrated.

117 Moreover, 19 protein bands from SDS-PAGE were analyzed and a total of 45 diff

118 ested in these COFs in significantly reduced band gap (1.8-2.2 eV), solid state luminescence and reve

119 The recent surge of interest towards high-band gap absorbers for tandem applications led us to rec

120 lar, there is currently no consensus for the band gap and electronic structure of ST12-Ge (tP12, P432

121 solution-processed quantum wells wherein the band gap can be tuned by varying the perovskite-layer th

122 antum yield at excitation energy above twice band gap could indicate a quantum cutting due to the low

123 We identified the band gap Eg and phonon cut-off frequency omegamax as the

124 in a change of the nature of the fundamental band gap from indirect to direct.

125 unlike silicon, the nature of the transport band gap in CNTs is not fully understood.

126 s at the nanoscale and show in-depth how the band gap is affected by a shift of the valence band edge

127 long-lived photoluminescence, and an optical band gap of 1.6 eV.

128 niques and boasts a relatively large optical band gap of 2.15 eV.

129 rough which the A-site cation influences the band gap of 3D metal halide perovskites.

130 theorem: In generalized KS theory (GKS), the band gap of an extended system equals the fundamental ga

131 iconducting CNTs, and a 32% reduction in the band gap of narrow-gap CNTs.

132 pectively, and form electronic states in the band gap of SrTiO3.

133 ong been predicted to form in proximity to a band gap opening in the underlying band structure.

134 sed photodetectors was observed suggesting a band gap reduction as a result of the BNNSs' collective

135 rier, and In2Se3/WSe2, showing a significant band gap reduction in the combined system.

136 -layer tungsten disulfides (WS2) is a direct band gap semiconductor with a gap of 2.1 eV featuring st

137 tructure calculations indicate that opposite band gap shift directions associated with Sb/In substitu

138 elax one of the photoelectrode criteria, the band gap, a promising strategy involves complementing th

139 Typically, when increasing the band gap, one might assume that a decrease in photoactiv

140 The former effect tends to raise the band gap, while the latter tends to decrease it.

141 d in the conjugated backbone to modulate the band gap.

142 actical performance is hampered by the large band gap.

143 charge-balanced semiconductor with a narrow band gap.

144 ice, leading to progressive reduction of the band gap.

145 which also indicates the presence of a small band-gap and thus non-metallic or molecular-like behavio

146 The lifetime of this sub-band-gap emission exceeds that of the excitonic transiti

147 at both atomic and mesoscale levels with the band-gap evolution through a pressure cycle of 0 <--> 17

148 The limited number of known low-band-gap photoelectrocatalytic materials poses a signifi

149 The all-PSCs with the wide-band-gap polymer PBDB-T as donor and PZ1 as acceptor sho

150 roscopy, we prepared a minimal DQD in a wide band-gap semiconductor matrix.

151 Direct band-gap semiconductors play the central role in optoele

152 Metamaterials with acoustic and elastic band gaps are of great interest to scientists and engine

153 n lower disparity and strong superconducting band gaps in the dominant crystal regions, which lead to

154 ed halide hybrid perovskites possess tunable band gaps, however, under illumination they undergo phas

155 t have the disadvantage of excessively large band gaps.

156 that between 80 and 100% of the deep valence-band holes in graphene are filled via an Auger transitio

157 e dynamical stripe correlations in the three-band Hubbard model, which represents the local electroni

158 formation of a narrow intermediate band (E- band in BAC model) with the minimum at the Gamma point o

159 rain oscillations in the EEG alpha frequency band in posterior cortex can dissociate current from fut

160 xcitation band at 500 nm, tunable excitation band in the deep red/near-infrared window, and tunable e

161 Additionally, we investigate the latitudinal band in which first sightings were recorded, and species

162 e mitochondrial localization to actin-rich I-bands in body wall muscle.

163 erate the elongated cells that build Bungner bands in injured nerves and that such cells can transfor

164 calculations identify the exciton absorption bands in transient absorption spectra measured by our gr

165 Specifically, a 1545 cm(-1) band increased in intensity with the progression and sev

166 has been suggested that different frequency bands index distinct canonical computations.

167 hypothesis, which posits that top-down beta-band influences directly modulate bottom-up gamma band i

168 influences directly modulate bottom-up gamma band influences via cross-frequency interaction.

169 a solution led to the increase in absorption band intensity in diffuse reflectance spectra of the ads

170 used by an energy gap close then reopen with band inverse.

171 ations by considering the temporal record of banded iron formations and marine red beds.

172 The disappearance of banded iron formations at 1.8 billion years ago was tra

173 etween 260-280 Hz; the second, and stronger, band is a broad peak in the 400-500 Hz range (termed ome

174 The valence band is also heavily altered due to oxidation and amorph

175 The intensity of the C-D band is proportional to the extent of deuteration in the

176 cient coupling from visible to near-infrared bands is demonstrated between a nanowaveguide and whispe

177 mitigates this problem and can help achieve band-like transport on a wide range of substrate platfor

178 Aggregated bands located at 1683 and 1616cm(-1) became evident afte

179 atients with and without AF into 5 NT-proBNP bands: <400, 400 to 999 (reference), 1000 to 1999, 2000

180 s different regions (medial septum, diagonal band, magnocellular preoptic area, and substantia innomi

181 mpared the in vivo kinetics and proteomes of banded, mature, and hypersegmented neutrophils to determ

182 nderlies top-down control, whereas the gamma-band mediates bottom-up stimulus processing.

183 nct difference in the location of conduction band minimum between Mg2 Si and the isostructural phase

184 ants changes the character of the conduction band minimum from Ni-oxide in the Ni-only to predominant

185 ation contacts creates a very low conduction band minimum.

186 the condition necessary for the "flat/steep" band model for superconductivity is satisfied in O-doped

187 Together, our results suggest that the beta-band modulation was a top-down signal associated with th

188 This finding indicates that the beta-band modulation was unrelated to the execution of the mo

189 , we present data from an 18-y study of wild banded mongooses, Mungos mungo, showing that females tha

190 reflectivity echoes and associated rainfall bands more efficiently.

191 tion, restored a functional balance of gamma-band network oscillations, and allowed treated eFSE rats

192 at visual flicker entrained endogenous alpha-band networks, which in turn impaired task performance.

193 rum is investigated including the effects of band nonparabolicity and the influence of the continuum

194 the nearby asymmetric-stretch rovibrational band of atmospheric carbon dioxide.

195 The charge transfer between the conduction band of nAu and pi* continuum of polyaromatic sheets is

196 ectron-electron scattering in the unfilled d band of Ni.

197 edge appeared at 1.1 eV below the conduction band of SiC.

198 sharp peak (1675 cm(-1)) within the amide I' band of the spectral region.

199 ed electrons can be stored in the conduction band of TiO2 on an ms-s time scale, and we propose that

200 in the filum terminale (FT), which is a thin band of tissue at the caudal end of the spinal cord.

201 aracteristic surface plasmon resonance (SPR) band of Tyr-Au NPs was red-shifted to 596 and 616nm and

202 tains a ciliary root with a pronounced cross-banding of electron-dense material that should be import

203 a periodicity consistent with the D-periodic banding of higher-order fibers assemblies.

204 tract revealed in six patient sera a pair of bands of 10 and 16 kDa, and in nine a 16-kDa band.

205 d by the superposition of similar absorption bands of carbonyl functional groups summing up to a broa

206 ectron scattering and screening in different bands of different materials with both simple and comple

207 These data reveal discrete bands of E2 and E3 cells that may relay information from

208 clear SERS spectra with characteristic Raman bands of histamine.

209 The nu(CO) bands of the molecules with Ag-Fe(CO)5 bonds show a nota

210 f YFP and the visible-region (QX) absorption bands of the RC allow energy transfer via a Forster mech

211 Several Bi 6p x/y bands of Y2 O2 Bi are raised in energy by oxygen doping

212 om SiC to WSe2, where a reduction of valence band offset was observed.

213 familiarity with sound objects, whereas beta-band oscillation signifies involvement of the action-per

214 Alpha-band oscillations also carried clear information about t

215 ordings, both sustained potentials and alpha-band oscillations are present during the delay period of

216 al excitability.SIGNIFICANCE STATEMENT Alpha-band oscillations are thought to reflect cortical excita

217 iform cortex is an important driver of gamma-band oscillations in the vStr and associated limbic area

218 uced rodent duration MMN (p<0.001) and theta-band (p<0.01) response.

219 n in raw signals and in signals after narrow band-pass filtering at the highest dominant frequency (H

220 actis populations to form programmed spatial band-pass structures that do not require fine-tuning and

221 This bias-selectable dual-band photodetector is compact, with no moving parts, and

222 orption near-edge structure (XANES), valence-band photoemission spectroscopy (VB-PES), X-ray emission

223 ux-en-Y gastric bypass, laparoscopic gastric band placement, or laparoscopic sleeve gastrectomy.

224 We use clock spectroscopy to prepare lattice band populations, internal electronic states and quasi-m

225 zed by pronounced difference in SPR spectral band position (shifting up to 50nm).

226 In addition, changes in theta band power during epileptogenesis were associated with a

227 us we found more power in the high-frequency band prior to high-expected pictures than weakly expecte

228 is drastically reduced following the aortic banding procedure; however the cells are able to compens

229 h the SPR sensorgram, and the detected Raman bands provide chemical insight into the binding event.

230 The first band (psi) is centered between 260-280 Hz; the second, a

231 ar gain was typically 10-30 dB and was broad-band rather than sharply tuned.

232 GNR heterojunction band realignment proceeds over a distance less than 1 nm

233 pore diameter and fraction in terms of broad-band reflectance results in very thin films with excepti

234 faces showed as alpha-band-related and beta-band-related AIS increases in content-specific areas; th

235 of prior knowledge for faces showed as alpha-band-related and beta-band-related AIS increases in cont

236 number of AGBs has decreased and the rate of band removal and revisional surgeries has progressively

237 After band removal, the median time to revisional surgery was

238 ection and quantification were 200 and 400pg/band, respectively.

239 I, 0.08-3.56) for gastric bypass and gastric banding, respectively.

240 Gamma band rhythms may synchronize distributed cell assemblies

241 o shows that the combination of the marginal band rigidity and cortical tension increases the ability

242 Here using band shift assays, fluorescence Job plots, and yeast thr

243 ion than previously accomplished using the G-band shift with charge.

244 hin-film optics, to identify subtle changes (band shifts, deviation from linear approximation, etc.)

245 oftware to automatically detect and annotate band sizes, calculate average TL, as well as the percent

246 An overall band structure at grain boundaries is presented.

247 Band structure calculations indicate that opposite band

248 e differences are governed by changes in the band structure due to quantum confinement and are most p

249 The electronic band structure of phosphorus-rich GaNxPyAs1-x-y alloys (

250 lecule junction transmission and the complex band structure of the infinite 1D material for siloxane,

251 mobility that is due to the character of the band structure that results in the so-called Dirac cone

252 eory calculations of franckeite's electronic band structure to rationalize the experimental results.

253 , we monitor the evolution of the electronic band structure upon doping using the G peak area which i

254 e concentration profiles are then related to band structure which provide a unique insight into grain

255 e report the realization of an AG that has a band structure with vanishing density of states consiste

256 ponds with the two direct-gap valleys of the band structure, which can be optically manipulated.

257 tly on wavefunctions in addition to standard band structure.

258 of ferromagnetism and modulates the surface band structure.

259 ubsequent coherent changes in the electronic band structure.

260 a local bandgap in the (110)-projected bulk band structure.

261 mity to a band gap opening in the underlying band structure.

262 allows for controlled modification of their band structure.

263 ework for identifying topologically distinct band-structures for all 3D space groups.

264 osephson junction arrays, and certain narrow band superconductors.

265 f a salient target were associated with beta-band suppression, and target reappearances with beta-ban

266 rations occurring after laparoscopic gastric band surgery as well as the associated payments in a lon

267 murine hearts subjected to transverse aorta banding surgery.

268 the Fermi surface geometry of the electronic bands surrounding the Gamma = (0, 0) and X = (pi/aFe, 0)

269 es from passenger pigeons and 2 genomes from band-tailed pigeons, which are passenger pigeons' closes

270 an intermediate temporal regime in the alpha band that likely reflects different underlying computati

271 The data shows a number of absorption bands that are assigned to one- and two-phonon and impur

272 es a new interpretation of the outer retinal bands that leads to a more accurate interpretation of OC

273 ologically nontrivial valence and conduction bands that touch at a line near the Fermi level.

274 al ring of microtubules, called the marginal band, that flattens the overall cell morphology by pushi

275 Our electronic band theory sheds new light on known topological insulat

276 spikes, the relative power of five frequency bands (theta, alpha, beta, low gamma, and high gamma) an

277 with optical transitions from the conduction band to lower E- and upper E+ valence subbands has been

278 assign the second component of the continuum band to the proton uptake complex, a cluster with an exc

279 d curve fitting of most relevant vibrational bands to calculate a highly characteristic fingerprint t

280 to validate and apply clinically meaningful bands to the ItchyQuant, an illustrated self-report nume

281 ndence of the joint density of states for AG band transitions.

282 arch indicates that the alpha-beta frequency band underlies top-down control, whereas the gamma-band

283 imulus for vitiligo repigmentation is narrow-band UVB (NBUVB), but how the hair follicle melanocyte p

284 th numerical simulations, simultaneous multi-band valley dependent edge states and the associated val

285 The QRS morphologies of the parietal band VAs were characterized by a left bundle branch bloc

286 is anterior muscle in the 20-40 Hz frequency band was also significantly larger for the 9-25 week age

287 e minimum length of isolated hyperreflective bands was determined based on analysis of 34 eyes with c

288 oth the delta (0.5-5 Hz) and alpha (5-13 Hz) bands was significantly smaller for the surgically reinn

289 This band we identified was a novel enokitake allergen.

290 -such as an imbalance mode between different bands-we show that the resistivity bound becomes [Formul

291 rregularities at the inner segment ellipsoid band were seen.

292 o the scale-free dynamics of delta and theta bands, whereas this property in high-gamma fluctuations

293 xcited at the red edge of the Trp absorption band which allows normalisation of the emission spectra

294 multaneously sustaining stopped light energy bands which contain multiple points of zero group veloci

295 -spanning instabilities (also known as shear bands), which are typical to the mechanical yield.

296 organize to form cellular columns, Bungner's bands, which are indispensable for regeneration.

297 We further find a mixture of light and heavy bands, which results in a high thermoelectric power fact

298 rved linear dispersed feature in the valence band, with a Fermi velocity of comparable to that of gra

299 late the group index of different wavelength bands within the supercontinuum generation process.

300 species display alternating high and low Mg-bands within their shell walls that cannot be explained