ライフサイエンスコーパス: band

1 i level in close proximity to the conduction band.

2 ombination tablets according to their weight-band.

3 oscopically small quantum materials, band by band.

4 rmance of a MIMO antenna array at the 60-GHz band.

5 meandered monopole operating in the 915 MHz band.

6 ecrease the energy of the light hole valence band.

7 radio array(6) in the 1,281-1,468 megahertz band.

8 racteristic frequencies outside the observed band.

9 normalized to the neighboring CH stretching band.

10 fetime of mobile electrons in the conduction band.

11 ng to adapt its length to the width of the I-band.

12 of the absorbance of the nu(as) OH spectral band.

13 f the measured spectra over a wide frequency band.

14 anisotropic Weyl cones and the massive bulk bands.

15 organization was shared across all frequency bands.

16 t the degenerate flat bands into Hubbard sub-bands.

17 uires no a priori specification of frequency bands.

18 recently shown the emergence of flat energy bands.

19 insic in nature) and shared across frequency bands.

20 aberrations within photoreceptor-associated bands.

21 , or IQ, and is not found in other frequency bands.

22 by lateralised networks from fast-frequency bands.

23 'Rashba splitting') occurs in the electronic bands.

24 nd observed in several interacting frequency bands.

25 , the Schmidt-Lanterman incisures, and Cajal bands.

26 nsity distribution observed in locust hopper bands.

27 increased in debanding compared with sham or banding.

28 e chain reaction testing, and no oligoclonal banding.

29 esting-state EEG power in beta and low-gamma bands (10%), and numeracy (2%).

30 This activation was manifested in the beta-band (12-30 Hz), ramping up slowly over 500 ms after sti

31 line correction and normalization to Amide-I band (~ 1650 cm(-1)).

32 ular velocity ratio, E/E': sham, 13.6+/-2.1, banding, 18.5+/-4.1, P=0.014) accompanied by increased o

33 m fluorescence: sham, 1.6x10(8)+/-6.1x10(7), banding, 2.6x10(8)+/-4.5x10(7), P<0.001) and augmented m

34 l increased oscillatory activity in the beta band (~20 Hz) at triplet transitions that indexes learni

35 iated with increases in spiking and in gamma-band (40 to 90 Hz) power/connectivity that fed forward u

36 restimulus oscillatory activity in the alpha band (8-13 Hz), we establish a mechanistic link between

37 Retrospective analyses suggest that banding a sleeve using a silicone ring may decrease weig

38 ive cooling materials reported possess broad-band absorption/emission covering the whole mid-infrared

39 ted to memory and supports the role of theta-band activity in human episodic memory.SIGNIFICANCE STAT

40 Bursts of beta frequency band activity in the basal ganglia of patients with Park

41 Unaveraged beta-band activity is characterized by short-lasting, burst-l

42 Oscillatory alpha-band activity is commonly associated with spatial attent

43 These findings challenge the idea that alpha-band activity is directly involved in tactile-spatial tr

44 lly blurs the temporal relationship of alpha-band activity relative to behavioral indicators of tacti

45 ormal GPe activity, and (6) exaggerated beta band activity was not present in the cortex or GPe-STN n

46 osyncratic biases could be spontaneous alpha band activity, a prominent brain rhythm known to influen

47 erval (CI) 0.86-0.99) and adjustable gastric band (AGB; 33.6%; RR 0.45, CI 0.34-0.60; p < 0.001).

48 onding to half-filling of each of these flat bands, all of which are tunable by the displacement fiel

49 The molecular nature of the conduction band allows us to electronically dope the materials by r

50 Crucially, however, each band also exhibited temporally independent FC dynamics c

51 Furthermore, valence band analysis by X-ray photoelectron spectroscopy and ph

52 ariability of each dose group between weight-band and flat-dosing.

53 ogical hotspots were identified within the A-band and N-terminal I-band that closely correlated with

54 The organic-molecule-based conduction band and the inorganic-ion-based valence band provide an

55 We used bird banding and encounter data for American kestrels (Falco

56 , and orbitals, and reciprocal space, namely bands and Fermi surfaces, via symmetry and topology, cla

57 ivity is less synchronous across heterotopic bands and mutants are less responsive to pharmacological

58 The recently discovered flat electronic bands and strongly correlated and superconducting phases

59 CryptoPS low-titer (T1 band) and high-titer (T2 band) results were compared wit

60 ld potentials and spikes at the theta (8 Hz) band, and that low-frequency electrical microstimulation

61 of angioid streaks (AS) using AO: "crack," "band," and "hypopigmented." The first 2 were very simila

62 nisms are implemented in the theta frequency band; and (2) contextual knowledge can indeed be acquire

63 After 8 to 9 weeks, half of the banding animals underwent overload relief by an aortic d

64 indings demonstrate that kagome-derived flat bands are a promising platform for novel emergent phases

65 neuronal oscillations at different frequency bands are associated with top-down cognitive control; ho

66 Specific protein bands are then visualized by decoration with magnetic be

67 ng the change of the OH (~3390 cm(-1)) Raman band area (3350-3550 cm(-1) spectral region) after being

68 g a hypsochromic shift of another absorption band around 340 nm that is independent of the analyte st

69 It is followed by band assignments, a crucial aspect mostly performed with

70 stand the neural mechanisms underlying gamma-band ASSR network abnormalities in schizophrenia.

71 Previous work noted that a CT band at 726 nm formed when ET-FAD was reduced and Bf-FAD

72 nal quantum Hall effect of a single electron band at low magnetic fields.

73 icipating in the formation of electron-dense band at the base of the parasite infection site.

74 NMDAR engagement measured by gamma-frequency band auditory steady-state response (40 Hz ASSR) and res

75 leaved muscles contract, myosin-containing A-bands become split and adjacent myosin filaments move in

76 o perovskite solar cells, the doping-induced band bending in perovskite effectively facilitates hole

77 ace as a result of significant thermodynamic band bending induced by ligand attachment and Ni(II) bin

78 igm comprises a system wherein the extent of band bending induced by metal ion binding is the primary

79 corresponding to the phosphate and carbonate bands between the benign and malignant groups.

80 ral density values of standard EEG frequency bands between the SS (n = 42) and OSA (n = 129) groups d

81 and an increased separation of the n -> pai* bands between the trans- and cis-conformations, which al

82 onal charge density arising from filled bulk bands, but measurements of such charge distributions hav

83 in microscopically small quantum materials, band by band.

84 at 2D-IR spectroscopy of the protein amide I band can be performed in aqueous (H(2)O) rather than deu

85 We show that this low-energy band can be rationalized in terms of edge states of the

86 , the experimentally observed intermolecular bands can be assigned.

87 upling between Pd and Ag, which lowers the d-band center of Pd and thereby significantly enhances its

88 The FT-IR and FT-Raman band characteristics for guar gum, lecithin, and maltode

89 ine kinase and/or creatine kinase-myocardial band (CK-MB) post-procedure were included.

90 ectron paramagnetic resonance (EPR) at the X-band, combining in-phase and out-of-phase detection sche

91 A light-colored band composed of compressed and distorted tracheids was

92 with U ~ 4 eV, indicates that an electronic band connecting the two Weyl cones is flattened by elect

93 ) obtained with SD-OCT showed that this dark band corresponds with an area of retinal thickening comp

94 xploitable band gaps due to their accidental band-crossing origin.

95 Nodal band crossings with linear dispersion are expected to ha

96 palladium gallium (PdGa) displays multifold band crossings, which are connected by exactly four surf

97 dily infected non-sequestering larvae of the banded cucumber beetle (D. balteata), while infectivity

98 actions occurred in beta and gamma frequency bands depending on the area contributing the spikes, exh

99 pharmacological treatment that thins F-actin bands, depletes E-cadherin, and stimulates proliferation

100 The observed SDS-PAGE bands did not show any evidence of zein crosslinking.

101 patient variability was predicted for weight-band dosing compared to flat-dosing.

102 igher median AUC0-24h compared to the weight-band dosing.

103 e spin polarization occurs in the spin-split bands due to asymmetric spin-flip.

104 scopy is a valuable source of information on band-edge profiles, governed by the distribution of inte

105 The introduction of copper tunes the d-band electron configuration and enhances the adsorption

106 Combined with X-band electron paramagnetic resonance (EPR) spectral anal

107 ighlight the extrinsic origin of their broad band emission.

108 The synergy of favorable band energy alignment and concerted cascade interfacial

109 X-band EPR experiments revealed bis(phosphine)cobalt(II) b

110 Continuous wave and pulsed (HYSCORE) X-band EPR show it has a highly compact g(z) area and smal

111 and controls, with particularly strong theta band event-related connectivity in dystonia.

112 Such intercellular bands extended into a large-scale network of mechanicall

113 stence of Rashba splitting at the electronic band extrema of 35+/-10 meV, and identify the main inver

114 tude of low-frequency fluctuations in slow-4 band (fALFF4).

115 ownsampling data, (3) of different frequency band features.

116 we observe the formation of a coherent, two-band Fermi surface, consisting of both hole pockets cent

117 y analysis shows a low-intensity or absent D band for FG, indicating that FG has among the lowest def

118 lized states for electrons and more disperse bands for holes upon optical or thermal excitation.

119 ) nanoprobe with narrow and tunable emission bands for intracellular in vivo imaging is presented.

120 ivity for both NRR and HER by shifting the d-band from -4.42 to -4.19 eV.

121 romagnetic resonators, we transform a single-band FSS to a dual-band FSS.

122 rs, we transform a single-band FSS to a dual-band FSS.

123 erformance photoelectrode, including a small band gap and favourable cost, optoelectronic properties,

124 aphene, TMDs have the advantage of a sizable band gap and strong spin-orbit coupling.

125 e integrated trap density (D(it)) across the band gap by nearly 1 order of magnitude in Al(2)O(3) (<6

126 Engineering the band gap chemically by organic molecules is a powerful t

127 This 1.7 eV band gap decreases to 0.3 eV at 65 GPa.

128 be suspended for the hybrids containing low band gap emissive metal halide species, such as SbCl(5)

129 1.5 GPa, emission can be triggered by above-band gap laser irradiation, accompanied by a color chang

130 Optically active defects in wide band gap materials, for instance, are critical constitue

131 od mobility have been big challenges in wide band gap materials.

132 tly enhanced for the hybrids containing wide band gap non-emissive ZnCl(4) (2-) .

133 ity (7.75 x 10(-3) S cm(-1)), and an optical band gap of 1.67 eV.

134 omic-layer organic semiconductor with a wide band gap of 3.41 eV.

135 Zn-HAB is shown to have microporosity with a band gap of approximately 1.68 eV, resulting in a modera

136 sults in a bathochromic shift of the optical band gap of CdSe QDs (R = 1.17 nm) of up to 111 meV whil

137 onduction band, substantially decreasing the band gap of the expanded lattice.

138 lity and is a semiconductor with an indirect band gap predicted near 1.3 eV.

139 properties at nanoscale and small adjustable band gap ranges.

140 fact that it is one of the most studied wide band gap semiconductors.

141 ions of the pyrazinium-based orbitals in the band gap transition of A(II) Pb(2) X(6) .

142 on potential, electron affinity, and optical band gap which provides an absorption profile that has s

143 where (3AMP)(FA)Pb(2)Br(7) has the smallest band gap while (4AMP)(MA)Pb(2)Br(7) has the largest band

144 n causes colossal reduction in layered MnBDC band gap while it has no observable effect on bulk MOFs.

145 multi-redox waves with a low electrochemical band gap, which signifies the tuning of highest occupied

146 Coulomb force-independent of its electronic band gap.

147 p while (4AMP)(MA)Pb(2)Br(7) has the largest band gap.

148 Here, we report an associative zinc oxide band-gap excitation and copper plasmonic excitation that

149 d solutions that span the indirect to direct band-gap modification which exhibit tailorable optical p

150 eover, the deformed graphene could exhibit a band-gap, allowing an exponential change in the source-d

151 ally exist in semimetals without exploitable band gaps due to their accidental band-crossing origin.

152 and the electronegativity of the metals, the band gaps of OMCs were varied by 0.83 eV and their condu

153 The indirect band gaps of the Sn and Pb compounds are ~1.7 and 2.0 eV

154 many-electron interactions induce electronic band gaps when graphene is patterned at nanometer length

155 sublattices, leading to materials with small band gaps, large exciton binding energies, and absorptio

156 1993 (n = 8,631; gastric bypass and vertical banded gastroplasty, 49% each) and 98% laparoscopic (n =

157 Our work paves the way for exploring flat-band-generated quantum phenomena in WSMs.

158 emission rather than by the ligand-centered bands, implying that Dy(3+) can be tuned as a single ion

159 analysis of the protein amide I and amide II band in aqueous solutions that achieves a limit of detec

160 significantly reduced at the gamma frequency band in Fmr1-KO rats.

161 to the SWCNTs were found to form a separate band in the density gradient apart from the fluorescent

162 layer and, most ventrally, formed a distinct band in this region.

163 This transformed behaviour suppresses shear-banding in bulk samples in normal uniaxial (tensile or c

164 al features of disordered packings of rubber bands in a cylindrical container.

165 find the magnetic co-representations of all bands in all magnetic space groups, we generate data to

166 is the creation of weakly dispersive, 'flat' bands in bilayer graphene for certain 'magic' angles of

167 formation, shape, and speed of locust hopper bands in our models.

168 d at partial fillings of the flat electronic bands in recent spectroscopic measurements(7-10), and tr

169 tterns in AO-OCT and irregular outer retinal bands in SDOCT.

170 ence of IgG Abs, which appear as oligoclonal bands in the cerebrospinal fluid.

171 Both modified starches reported absorption bands in the IR at 1566 and 1738 cm(-1), proper for thes

172 large bathochromic shifts in the absorption bands, indicating that the electronic properties of dith

173 Echocardiography revealed that banding induced concentric hypertrophy and diastolic dys

174 e currents of 2-dimensional (2D) topological band insulators with broken time-reversal symmetry.

175 nteractions, which split the degenerate flat bands into Hubbard sub-bands.

176 es that under weak spin-orbit interaction, a band inversion occurs.

177 When the surface massive Dirac band is slightly carrier doped by a gate voltage, the ed

178 The associated quantum geometry of the bands is extracted, enabling prediction of the anomalous

179 The double degeneracy of the Dirac bands is protected by a combination of inversion, time-r

180 ent with propranolol/nadolol plus endoscopic band ligation.

181 ation in their phase-of-firing at a 10-25 Hz band-limited beta frequency at which they synchronize ac

182 tional brain integration were assessed using band-limited power envelope correlation, whereas those o

183 Witham MD, Band M, Chong H, et al.

184 and a specific band nature with the valence band maximum and the conduction band minimum mainly domi

185 Since segregation-induced banded microstructures commonly occur in many engineerin

186 the valence band maximum and the conduction band minimum mainly dominated by the halide and DABCO(2+

187 Here, we assessed alpha-band modulation with massive univariate deconvolution, a

188 moarchitecture of the amygdaloid body of the banded mongoose (Mungos mungo) and domestic ferret (Must

189 uclei in the domestic ferret compared to the banded mongoose and other carnivores, although this inve

190 In the banded mongoose the dentate gyrus appears to be comprise

191 est our model using long-term data from wild banded mongooses, a species characterized by frequent in

192 ually large semigap of ~16 eV and a specific band nature with the valence band maximum and the conduc

193 ures in a N(2) matrix, and subsequent narrow-band near-infrared (NIR) laser excitation to give 1cc.

194 ist angles, TBBG shows multiple sets of flat bands near charge neutrality, resulting in numerous corr

195 We wirelessly recorded 192 broad-band neural signals from three cortical sensorimotor are

196 eoptic area, septum, nucleus of the diagonal band of Broca, and main olfactory bulb.

197 he quantum anomalous Hall effect in the flat band of magic-angle twisted bilayer graphene(4-8) has sp

198 n zone, especially the bandwidth of the flat band of out-of-plane orbitals is less than 0.02 eV along

199 ps almost perfectly with the Q(x) absorption band of the BChls.

200 The rise and fall times of the elution band of the temporal component were considered as the in

201 experimental energy of the lower absorption band of these species.

202 Pathological hotspots within the A-band of TTN may be informative in determining variant pa

203 ed full width at half maximum of the elution band of up to 30% in comparison to the calculated value

204 luence of segregation-induced microstructure bands of austenite (gamma) and martensite (alpha' ) phas

205 ating efficiencies for the two main emission bands of CSD-PLNPs, resulting from MI-triggered R-PersL

206 pairs of cells or cell aggregates can induce bands of deformed gel, extending to surprisingly long di

207 nce between the intensities of the two Raman bands of molybdenum disulfide and graphene oxide, we dem

208 Spectral interferences of the molecular bands of PO and NO as well as the iron lines with Se lin

209 simultaneously orchestrating closely spaced bands of resonances along different magnetization trajec

210 degeneracy at the Gamma point of the energy bands of the high-temperature phase is lifted in the low

211 Herein, the excitation bands of ytterbium-based MOFs are extended to 800 nm via

212 e-Sb[Formula: see text]Te[Formula: see text] band offset using X-ray photoemission spectroscopy, and

213 Tractional vitreous bands on imaging correlated with plus disease status (29

214 lated groups of variables, such as frequency bands or regions of interest in electroencephalographic

215 Concomitantly, task-associated gamma band oscillations induced by trains of auditory stimuli,

216 with plus disease status (29% vs. 5% without bands; P = 0.05).

217 Hence, talin operates as a mechanical band-pass filter, able to read and interpret frequency-d

218 otential, it is possible to use high-pass or band-pass filtering to specifically isolate the SKNA.

219 Here we present a new technique based on band-pass filters for uncovering local-scale signals hid

220 fined by field-inversion gel electrophoresis banding pattern), emm types, and emm clusters at visits

221 in-in-sap-in-resin double emulsions, showing banding patterns with differential content of resin-in-s

222 oral host age by quantifying annual skeletal banding patterns, and utilise high-throughput sequencing

223 discover unusual electronic coupling to flat-band phonons in a layered kagome paramagnet, CoSn.

224 igh-energy state with an unusual sequence of band population.

225 ver, the relationship between such a spiking-band power (SBP) and neural activity remains unclear, as

226 of cognitive control-local midfrontal theta-band power changes-that participants show during full al

227 ractions, activity in this excited frequency band propagates to nearby regions.

228 ion band and the inorganic-ion-based valence band provide an unusual electronic platform with localiz

229 otein isolates exhibited complex polypeptide banding ranging from molecular weight of 11-75 kDa.

230 SDS-PAGE profile of PPI revealed major bands ranging from 50 to 7 kDa.

231 volution of one such system, the replication band (RB) in spirotrich ciliates, which is a localized,

232 Their two-photon absorption bands reach into the NIR-II region of the electromagneti

233 onnectivity from previous studies, eBird and band recoveries.

234 ptoPS low-titer (T1 band) and high-titer (T2 band) results were compared with IMMY LFA titers obtaine

235 itivity analysis yields insight into how the band's collective characteristics vary with changes in t

236 non/polar solvents, exhibiting narrow, sharp band shapes in dichloromethane but broad features in tol

237 pha, and even more so, in the beta frequency band significantly compromised the prediction of the lim

238 Narrow-band spectral lines enable researchers to investigate th

239 Different temperature dependent band splitting behaviors are observed at the [Formula: s

240 ment with the sarcomere end, working as an I-band spring that accounts for the rise of passive force

241 gth 2.7-3.1 um, showing the ability of the I-band spring to adapt its length to the width of the I-ba

242 fibres from frog skeletal muscle reveal an I-band spring with an undamped stiffness 100 times larger

243 omains, featuring layer-polarized conduction-band states caused by lack of both inversion and mirror

244 es the peak height in blip transients if the band-stop cutoff frequencies are compatible with the nan

245 electrolyzing ZnO, that model nanoimpacts, a band-stop filter can remove environmental noise within t

246 Furthermore, a Butterworth band-stop filter preserves the peak height in blip trans

247 [BiVO(4)] give rise to compatible electronic band structure alignment at their interfaces to ensure e

248 ichiometry of VO(2) from 1.86 to 2.44 on the band structure and insulator-metal transitions are prese

249 s into the interplay between magnetic field, band structure and many-body interactions in tunable sem

250 nt conduction polarity and their identifying band structure fingerprints.

251 6 electronvolts) and a favourable electronic band structure for efficient electron charge transport.

252 Fermi energy tuning to the nodal web-a flat band structure made of interconnected nodal lines-is the

253 tal interest is whether the chirality of the band structure manifests itself in charge transport prop

254 synergic effect on the resulting electronic band structure need to be explored in a broader material

255 We build up the band structure of BaCuAs using a molecular orbital appro

256 adjusting the interlayer coupling(6) or the band structure of constituent layers(9).

257 the Fermi surface topology and quasiparticle band structure of hole- and electron-doped Sr(2)IrO(4) a

258 of morphological aspects, phase purity, and band structure of photoelectrodes for an enhanced PEC pe

259 ffect of electrical doping on the electronic band structure of twisted bilayer graphene using a back-

260 ayers enables fine control of the electronic band structure, resulting in magic-angle flat-band super

261 as the reflection of the Fermi level in the band structure.

262 y enables super-resolution tomography of key band-structure details in situ.

263 We calculate electronic band structures and find good control of Rashba splittin

264 d inversion symmetries, resulting in complex band structures with Weyl crossings and unique spin text

265 of their triboelectric charge densities and band structures, it is found that the triboelectric outp

266 lying pai* orbitals that form the conduction band, substantially decreasing the band gap of the expan

267 was temporally independent between frequency bands, suggesting a putative mechanism for malleable fre

268 and structure, resulting in magic-angle flat-band superconductivity(1,2), the formation of moire exci

269 alpha-Band suppression following tactile stimulation was later

270 Moreover, alpha-band suppression occurred at the time of, or after, the

271 hey exploit wavefunctions relying on crystal band symmetries, which tunneling interactions are inhere

272 n of electronic correlations in tunable flat-band systems realized in twisted van der Waals heterostr

273 el of hypertrophy induced by thoracic aortic banding (TAB).

274 es, which account for the extended n -> pai* band tails.

275 dentified within the A-band and N-terminal I-band that closely correlated with regions of high percen

276 resent an alternative route to creating flat bands that does not involve fine-tuning.

277 1 degrees, features isolated flat electronic bands that host a rich phase diagram of correlated insul

278 At 1.4, 2.3, 3.4, 4.0, and 5.0 GHz bands the proposed AQGA is on average 75%, 49.2%, 64.9%,

279 apid decay (0.6 ns) of a small spectral side band, the broad emission line shape is constant to 100 n

280 proved by the SRAs for the children's weight band; then switched to 50 mg film-coated tablets once da

281 overy could help create super-intense narrow band thermal light sources and even an infrared emitter

282 ct endogenous oscillatory activity frequency bands: theta (~3-8 Hz) versus beta (~13-30 Hz) respectiv

283 absorber or with a reconfigurable reflection band throughout the visible.

284 igated decoding accuracy: (1) based on delta band time-domain features, (2) when downsampling data, (

285 3-6), a magnetic system in which non-trivial band topology favours long-range order of orbital angula

286 ted network and high density of near-valence band trap states in amorphous GeS.

287 We achieve tuning of individual frequency bands using magnetic reed switches connected in between

288 rial thinning, intraplacental T2-hypointense bands, uterine bulge, serosal hypervascularity, and sign

289 n be attributed to the radical change of the band velocities when the chiral Weyl fermions are excite

290 es showed that the absorbance of the protein bands was linear with the amount of mass deposited on th

291 In addition to a hydrated phyllosilicate band, we detect a ubiquitous 3.4-micrometer absorption f

292 filling of the first hole moire superlattice band, we observe a Mott insulating state with antiferrom

293 Five IMS bands were assigned to the heterogeneous ion mobility pr

294 pectral density values in the beta and delta bands were higher in the OSA group than in the SS group.

295 but more fragments and higher molecular mass bands were observed in the Gd-P gel image.

296 materials have demonstrated attractive broad-band white-light emission properties, they pose a seriou

297 rising splitting of the PL spectrum into two bands with an average energy separation of 80 meV.

298 The capping flat bands with bandwidth less than 0.2 eV run through the wh

299 350 degrees C parallel to the length of the bands within the apparent elastic limit of the phase mix

300 Independent control of spectral bands without significant cross-talk between infrared an