ライフサイエンスコーパス: excitation

1 ivity that hosts Majorana modes (non-Abelian excitation).

2 ough enhancing neuronal TRPV1 expression and excitation.

3 losest to the axon will generate greater CGC excitation.

4 dent switch from GABA-mediated inhibition to excitation.

5 (PNs) produces a long-term enhancement of SC excitation.

6 synaptic cells that show increased levels of excitation.

7 e ion trap using orthogonal double resonance excitation.

8 which again indicates the role of collective excitation.

9 thods for measuring MPI and spread of neural excitation.

10 intact rat, mimicking responses to glutamate excitation.

11 elds green and orange fluorescence upon blue excitation.

12 res spatial information on atrial electrical excitation.

13 s optimized for water imaging with broadband excitation.

14 de of the electronic charge transferred upon excitation.

15 of the emission lines under selective laser excitation.

16 dependent of potential KO actions on network excitation.

17 gated CGRP8-37, prevented sustained neuronal excitation.

18 ike timing, even with physiological rates of excitation.

19 nger enhancement due to the non-linearity in excitation.

20 ons: transient inhibition and longer-lasting excitation.

21 e lifetime can be modulated using pump-probe excitation.

22 h increased inhibition and reduced recurrent excitation.

23 isations promoted unidirectional patterns of excitation.

24 dication was observed less than 1 mus after excitation.

25 by the molecule via propagating patterns of excitation.

26 has the ability to prolong incoming cortical excitation.

27 nd AND-NOT gates via interacting patterns of excitation.

28 ads to the hybridization of light and matter excitations.

29 achieved with a broad range of visible light excitation (400-600 nm).

30 y, we demonstrate that nearest-neighbour RVB excitations account for the bulk of the spectral weight

31 melting of the CDW correlations rather than excitation across an optical gap.

32 Photon excitation also increased significantly above 1.0 MJ m(-

33 , a third ac signal occurring between the ac excitation and ac ejection frequency scans must also be

34 aveguide tapers to improve the efficiency of excitation and collection of fluorescent signals in the

35 ntracellular pH (pHi) is critical to cardiac excitation and contraction; uncompensated changes in pHi

36 erexcitability resulting from an increase in excitation and disinhibition occurring in two respective

37 nditions: (1) in the latter experiment, both excitation and ejection frequencies must be scanned, whe

38 resonance couples to optical fields at both, excitation and emission bands, and increases the spontan

39 hoice of GNR size to overlap the fluorophore excitation and emission wavelengths greater than 600 nm.

40 od incorporates a continuous wave (CW) laser excitation and gold nanoparticles (Au-NPs) to induce kno

41 processing depends on a fine balance between excitation and inhibition and tACS acts on both excitato

42 Recordings suggest that both excitation and inhibition are driven by the ON channel a

43 owing that in the visual system, feedforward excitation and inhibition are driven with equal strength

44 caine exposure disrupted the balance between excitation and inhibition as shown by an increase in the

45 n CN spike trains, while the balance between excitation and inhibition determines spike rate and loca

46 urons are activated by out-of-phase peaks in excitation and inhibition during network activity, where

47 xposure in vivo disrupts the balance between excitation and inhibition in VTA dopamine neurons, while

48 ways in which disturbances in the balance of excitation and inhibition might develop and be expressed

49 inhibition reestablishes the balance between excitation and inhibition through distinct mechanisms.

50 sured parameters, we applied combinations of excitation and inhibition to CbN cells with dynamic clam

51 The balance of excitation and inhibition, from cellular processes to ne

52 ansmission and an imbalance between cortical excitation and inhibition.

53 We find that synaptic excitation and intrinsic excitability are coregulated in

54 that perform exact, or asymptotically exact, excitation and inversion over a defined bandwidth, and a

55 avoids both autofluorescence under infrared excitation and many tedious washing steps, as the free d

56 role astrocytic EAAT2 plays on buffering nTS excitation and overall cardiorespiratory function.

57 , scalable, and well-suited for a variety of excitation and readout mechanisms, among them optomechan

58 n capable of simultaneous optical-electrical excitation and simultaneous optical-electrical response

59 interpret these inputs as dendrite-targeting excitation and soma-targeting inhibition (the latter con

60 ompared with tufted cells, are due to weaker excitation and stronger glomerular-layer-mediated inhibi

61 Here, we use a combination of TIRF excitation and supercritical angle fluorescence emission

62 effects on neuronal excitability, with both excitation and suppression observed in significant propo

63 to calculate ocular dominance separately for excitation and suppression.

64 ntial of this technique in probing molecular excitations and photochemistry.

65 g the metal-film thickness, spacer distance, excitation angle and polarization, and achieved 10-fold

66 These excitations are distinct from spontaneous Ca waves origi

67 the molecular scale, and massive electronic excitations are produced as a result of the field-matter

68 onant coupling between molecular and antenna excitations as well as the spatial extent of the enhance

69 As the energy increased, the spin excitations assumed a diamond shape, and they dispersed

70 optical [Sm-(TC)2](+) complex at 645nm after excitation at 400nm, in borate buffer, pH 9.2.

71 Upon excitation at 407 nm, the composition-optimized NYS:0.10

72 m the following multiple functions under NIR excitation at 800 nm: 1) Light harvesting by the UCNP sh

73 )2Tbx] (x = 1 to 3) complexes that, upon NIR excitation at 980 nm, showed an unprecedented Yb to Tb u

74 ws to determine the conditions for effective excitation at one selected resonance mode with suppressi

75 h pairs are generated by hot-electron impact excitation at temperatures near T = 300 K.

76 ence effects associated with surface plasmon excitations at a single metal-dielectric interface can p

77 a family of fluorophores featuring a common excitation band at 500 nm, tunable excitation band in th

78 a common excitation band at 500 nm, tunable excitation band in the deep red/near-infrared window, an

79 ted light at 180 degrees with respect to the excitation beam.

80 n time, of protons in a magnetic field after excitation by a radiofrequency pulse.

81 Molecular dynamics simulations with reagent excitation by way of selected vibrational normal modes r

82 Neuronal excitation can induce new mRNA transcription, a phenomen

83 Our approach combines charged excitations carried by strings, with topological propert

84 ulty in treating this state to strong double excitation character of the 2(1)Ag state, which prevents

85 ove 200 eV, permit the probing of electronic excitation, chemical state, and atomic structure.

86 nsitions and emission of several photons per excitation comprise a very attractive feature of semicon

87 al d orbitals contribute to the one-electron excitation configurations describing the initially prepa

88 ts, such as alpha-RuCl3, may display a broad excitation continuum inconsistent with conventional magn

89 CT: In atrial myocytes Ca(2+) release during excitation-contraction coupling (ECC) is strikingly diff

90 um Systems Approach to Understanding Cardiac Excitation-Contraction Coupling and Arrhythmias (3-4 Mar

91 is Systems Approach to Understanding Cardiac Excitation-Contraction Coupling and Arrhythmias Symposiu

92 ion through divergent mechanisms that impair excitation-contraction coupling and may be exemplary of

93 +) in normal cardiac function-in particular, excitation-contraction coupling and normal electric rhyt

94 messengers important for modulating cardiac excitation-contraction coupling and pathophysiology.

95 Ca(2+) is central to cardiac excitation-contraction coupling and stimulates mitochond

96 CNMs via defective membrane trafficking and excitation-contraction coupling in muscle.

97 Excitation-contraction coupling is the bridge between ca

98 ould promote T-tubule development and mature excitation-contraction coupling of hiPSC-CM when culture

99 ut it remains unknown whether all SFMs share excitation-contraction coupling pathway adaptations for

100 ultiple functional adaptations that minimize excitation-contraction coupling transduction times.

101 iomyocytes, Ca(2+) is the central element of excitation-contraction coupling, but also impacts divers

102 ic changes orchestrate cardiac architecture, excitation-contraction coupling, mitochondrial biogenesi

103 cell core, ensuring synchronous and uniform excitation-contraction coupling.

104 ases studied, we report the dominant orbital excitations contributing to the optically active excited

105 e orders of magnitude using near-ultraviolet excitation, depending on the substrate, and without degr

106 on to identify and separate out the magnetic excitations derived from nominal Fe(2+) and Fe(3+) state

107 ncies that are not damped by single-particle excitations do reach the near-infrared and even visible

108 In addition, photostimulated excitations, e.g., electron or hole polaronic trap state

109 Furthermore, T-currents increase excitation efficacy onto calbindin-negative cells during

110 loped and tested for measuring of NIR (760nm excitation) emission spectra in the skin.

111 agre de Condado de Huelva", were analyzed by excitation-emission fluorescence spectroscopy.

112 us materials across the visible spectrum via excitation-emission spectroscopy and time-resolved fluor

113 se is the MM1 fluorescence marker (270-365nm excitation-emission) which we show is due to a Leptosper

114 coded in n different ways, the 2-dimensional excitation-emission-matrix (EEM) spectrum is obtained by

115 working memory can be regulated by external excitation, enabling the system to be tuned to the desir

116 tion of free mobile charges is maximized for excitation energies just above the indirect bandgap.

117 iant oxidation potentials and cation radical excitation energies.

118 crease in photoluminescence quantum yield at excitation energy above twice band gap could indicate a

119 rogen bonding to water, where a pH-dependent excitation energy appears to be an intrinsic property.

120 nt and individual leaves to cope with excess excitation energy by following the changes in absorbed l

121 As the excitation energy of the silver island exceeds that of t

122 nthetic organisms regulate the efficiency of excitation energy transfer (EET) to fit light energy sup

123 Here, we investigated excitation energy transfer and charge separation using t

124 creating considerably faster and more robust excitation energy transfer.

125 nergy, depth-dependent, and element-specific excitation energy values are calculated.

126 some Raman features shifts when changing the excitation energy, and first-principle simulations confi

127 By using the concept of an effective excitation energy, depth-dependent, and element-specific

128 th important factors influencing the fate of excitation energy.

129 ronic band structure of the material and the excitation energy.

130 R output pulse are correlated with the laser excitation energy: at higher laser energy, the microwave

131 on of phasic noise generated by out-of-field excitation enhances temporal coding by expanding the ran

132 We show that their optogenetic excitation evokes rapid protective and avoidance behavio

133 veraged intensity less than 0.1% that of the excitation field.

134 ing in the exponentially decaying evanescent excitation field.

135 d be tuned by the parameters of the external excitation field.

136 sion from the CdS arms emerging only at high excitation fluences.

137 unconventional ground states support exotic excitations, for example the magnetic charges in spin ic

138 yclic strain amplitudes of 0.15% for 0.1 Hz excitation frequency, tip displacements greater than nan

139 vastly different output displacements under excitation from different sides, as well as one-way disp

140 by an increasing gradient of direct synaptic excitation from entorhinal cortex.

141 from weanling mice demonstrate that synaptic excitation from mossy fibres becomes more effective at i

142 ocal dendrodendritic inputs with coincidence excitation from olfactory cortex.

143 A key feature in these applications is excitation from the ground state to a charge-transfer st

144 reement with the experiment.Light and matter excitations from host media can hybridize in the strong

145 ine anisotropy, opening up a large spin-wave excitation gap.

146 wever is not related to the estimated neural excitation growth with current level near the behavioral

147 Although myocardial conduction of excitation has been widely described, the electrical pro

148 m remains elusive as the associated magnetic excitations have proven difficult to access with convent

149 HCP3) and another capable of dissipating PBS excitation (HCP4).

150 ts, which emit light long after cessation of excitation, hold promise for ultrasensitive in vivo imag

151 Importantly, sympatho-excitation in CHF exacerbates its progression and is str

152 ngs of our study is the overall shift toward excitation in liver-related hypothalamic neurons in the

153 While odor-evoked excitation in peripheral olfactory cells is known to enc

154 are the optical reflectivity under resonance excitation in samples prepared by oblique angle depositi

155 al code with both odor-evoked inhibition and excitation in single olfactory sensory neurons increases

156 gs are relevant to understanding the flow of excitation in the brain.

157 e olfactory system, 5-HT largely elicited MC excitation in the MOB while it evoked two different kine

158 hancement, and the advantages that come with excitation in the near-infrared.

159 old rate 3 SMS and free-breathing rate 2 SMS excitation in transmural myofiber helix angle, mean diff

160 n scattering can be used to measure magnetic excitations in Cd2Os2O7 and that it exhibits complex spi

161 hereas the discovery of Dirac- and Weyl-type excitations in electronic systems is a major breakthroug

162 Surface plasmon (SP) excitations in metals facilitate confinement of light in

163 ersatile technique sensitive to valence band excitations in quantum materials.

164 RuCl3 and reveals the presence of nontrivial excitations in such materials extending well beyond the

165 through a set of simple equations describing excitations in the PEL.

166 stant, when inhibitory synchrony was higher, excitation increased CbN cell firing rates more effectiv

167 ace oxygen related defects due to electronic excitations induced by ion irradiation determine the wat

168 pendent critical period development, and the excitation-inhibition (E/I) neural circuitry balance.

169 ation may be able to selectively control the excitation-inhibition balance within a cortical network.

170 opamine/serotonin abnormalities and cortical excitation-inhibition imbalances involving loss of parva

171 Hyperexcitability and the imbalance of excitation/inhibition are one of the leading causes of a

172 ibition may have differential effects on the excitation/inhibition balance in adapting and non-adapti

173 cortical circuits and discuss how shifts in excitation/inhibition balance may relate to pathological

174 n imaging depth of more than 5 cm at 1064 nm excitation is achieved with a contrast-agent concentrati

175 intracellular recordings in cats that while excitation is restricted to RF subregions, inhibition sp

176 data suggest that climbing fibre collateral excitation is weak in adult mice, raising the question o

177 nction of the incidence angle of the optical excitation, its wavelength and the gate-tuned chemical p

178 Upon electronic excitation (lambdamax approximately 300 nm), (2,6-aza)In

179 ed was achieved by concurrent innovations in excitation laser source, rotary joint assembly, 1 mm IVP

180 surface plasmon resonance overlaps with the excitation laser.

181 After exposure to excitation light encoded in n different ways, the 2-dime

182 The encoded excitation light is used to irradiate the liquid sample

183 pin liquid state with fractionalized thermal excitations (magnetic monopoles).

184 ntinuous low-level concurrent inhibition and excitation may contribute to irregular firing.SIGNIFICAN

185 in the vicinity of the U L3 edge in the TXRF excitation mode at the microfocus beamline of the Indus-

186 Strong coupling with some collective excitation mode has been indicated by a dispersion "kink

187 ron interactions and screening to low-energy excitations near the Fermi level.

188 eep was exposed to the sinusoidal acoustical excitation of 40-90dB SPL, in the frequency range from 1

189 We report, for the first time, that the excitation of a peripheral nerve can be accomplished by

190 This laser excitation of a quantum state of an atom of antimatter r

191 l donor and a monoquat acceptor triggered by excitation of a Ru(II) sensitizer enable this form of ph

192 The theory of the excitation of acoustic eigenmodes in multilayer ferroele

193 frequencies (</=1 Hz) evoked a short-latency excitation of BA interneurons (INs) that was depressed a

194 For both series of arrays, excitation of BODIPY at 500 nm results in efficient ener

195 excitations; therefore, by demonstrating the excitation of both bulk and surface vibrational modes us

196 ated amygdala plasticity by driving synaptic excitation of CeA neurons.

197 est because longer wavelengths allow optical excitation of cells in deeper layers of organic tissue.

198 namics, (ii) nonequilibrium, long-time-scale excitation of collective/hydrodynamic modes, and (iii) l

199 Brief excitation of CV motoneurons during crawling episodes re

200 n, as did selective inhibition of D1-MSNs or excitation of D2-MSNs.

201 Selective excitation of DAPP(2+) at 505 nm populates a lower excit

202 The 267 nm excitation of dCyd leads to a non-negligible population

203 Post-growth excitation of fully cyclized GNRs induces cleavage of sa

204 complex lipid mixtures using electron impact excitation of ions from organics (EIEIO) mass spectromet

205 ardia via up-regulating TRPV1 expression and excitation of laryngeal C neurons in the nodose/jugular

206 Excitation of left sensorimotor circuits, during an adap

207 ion of the reporting signal by the energy of excitation of light should lead to new technologies in o

208 signals and capable of mediating feedforward excitation of MCs.

209 ation of energetic electrons through plasmon excitation of nanostructures before thermalization has b

210 Optical excitation of nanostructures is known to induce local he

211 CGRP caused sustained excitation of neurons in slices of rat spinal cord.

212 als due to applied electric fields or by the excitation of photocarriers.

213 In contrast, excitation of Ru-qdpq results in the population of a rel

214 After optical excitation of tF2356, one observes an ultrafast ( approx

215 sis of the spectral features showed that the excitation of the analyte occurred in the region near th

216 In vitro analyses reveal that ATP excitation of the preBotC involves P2Y1 receptor-mediate

217 presence of barriers to propagation and the excitation of topological cycles, respectively, and can

218 r the first time that efferent-mediated slow excitation of vestibular afferents is mediated by muscar

219 Efferent-mediated slow excitation of vestibular afferents is of considerable in

220 d inducing strong coupling between light and excitations of the atoms, one can experimentally study p

221 d neutral stimuli whereas VS dopamine showed excitation only to reward or reward-predicting cues.

222 the observed continuum represents incoherent excitations originating from strong magnetic anharmonici

223 pecies for experiments obeying the modulated excitation paradigm and exploiting phase sensitive detec

224 on an optofluidic chip to create multi-spot excitation patterns that depend on both the wavelength a

225 vations for their ability to support optical excitations persisting for nearly 1 billion cycles, and

226 nvestigated by analyzing the temperature and excitation power dependent emission spectra, thermal que

227 The sensitivity values are dependent on the excitation power, and reach two maximum values of 0.0529

228 he Y2O3:1%Er(3+), 0.5%Ho(3+) at 121 mW/mm(2) excitation power, which makes optical temperature measur

229 ation at individual molecular level, and the excitation primarily derives from lone pair electrons on

230 the labeling efficiency f) and reducing the excitation probability of spins (lambda), are compared o

231 py (LSFM) features optical sectioning in the excitation process.

232 the solution on the in situ atomization and excitation processes occurred during operation of the LD

233 Then, we introduce a dynamic two-photon excitation protocol to simultaneously determine the chan

234 simultaneous and time-delayed pump and probe excitation pulses at fluences below the maximum permissi

235 wn of excitation waves at more physiological excitation rates than the wild-type, and the generation

236 of thermoelectric materials in the intrinsic excitation region can be suppressed through the magnetic

237 ulation is used to determine the spectrum of excitations relative to the excitonic state.

238 Functionally, this elevated excitation results in increased firing rates, and abnorm

239 These excitations reveal the energy dependence of the joint de

240 A white LED is used as the common optical excitation source for all the sensors.

241 ee semiconductor lasers were selected as the excitation source to verify the performance of the BF-QE

242 Excitation spectra and time-resolved photoluminescence m

243 ible absorption and multipeaked fluorescence excitation spectra correlate with experimental absorptio

244 ects were observed by combining emission and excitation spectra in two-dimensional representations.

245 Additionally, the infrared excitation spectra of the 1800 nm luminescence, as well

246 1800 nm luminescence, as well as the visible excitation spectra of the 522 nm and 652 nm luminescence

247 The oxyresveratrol emission and excitation spectra were obtained for first time.

248 e glass, with respect to the shapes of their excitation spectral waveforms and peak wavelengths.

249 Using photoluminescence excitation spectroscopy, we identify a sub-bandgap optic

250 The description of quantized collective excitations stands as a landmark in the quantum theory o

251 arameters on the resonance frequency and the excitation strength of toroidal dipolar mode are studied

252 fer can be strongly modulated by vibrational excitation, suggesting a new avenue for active control o

253 is line has such a high critical density for excitation that it is emitted only in very dense gas, an

254 allowing odor-evoked suppression as well as excitation, the responsiveness of piriform neurons is at

255 he formation of mysterious lines of massless excitations- the Fermi arcs.

256 ectively sensitive to either surface or bulk excitations; therefore, by demonstrating the excitation

257 shape further influences parameters such as excitation threshold and fiber selectivity.

258 mulus that depolarizes the membrane above an excitation threshold.

259 42 trapped ions, by tracing a single phonon excitation through interferometric measurements of only

260 the far-field by establishing the mode of de-excitation to be that of photon tunneling to a nearby wa

261 about rewards and punishments by displaying excitation to both (rather than excitation to one and in

262 nd inhibition as shown by an increase in the excitation to inhibition (E/I) ratio.

263 y displaying excitation to both (rather than excitation to one and inhibition to the other).

264 scattering (CARS) imaging via supercontinuum excitation to probe morphological changes that result fr

265 Additionally, TS dopamine showed excitation to several types of stimuli including rewardi

266 wer spins and which require resonant optical excitations to spin-polarize the ensemble.

267 new mRNA transcription, a phenomenon called excitation-transcription (E-T) coupling.

268 tics of failing cardiomyocytes, with several excitation-transcription coupling pathways shown to be c

269 egulation of gene expression, referred to as excitation-transcription coupling.

270 ronal excitability, synaptic plasticity, and excitation-transcription coupling.

271 quantum transport through nano-structures or excitation transfer in a complex biological system.

272 Solitons, particle-like excitations ubiquitous in many fields of physics, have b

273 harge transport may be induced by electronic excitation under friction, and the nanoscale current-vol

274 the atria, generally associated with erratic excitation underlain by re-entrant scroll waves, fibrill

275 population of the states is dictated by the excitation wavelength (and not primarily by temperature)

276 ied by rate constants, and may depend on the excitation wavelength contrary to slower photochemical p

277 egation behavior at higher concentration and excitation wavelength dependent multicolor emission prop

278 Using a single excitation wavelength dual colour FLIM method we are abl

279 ress the influence of antenna morphology and excitation wavelength on polarization conversion efficie

280 Merely by changing the excitation wavelength, we could specifically excite eith

281 strong and consistent fluorescence under an excitation wavelength.

282 ss the entire visible spectrum by tuning the excitation wavelength.

283 ajority of the current CDots to date exhibit excitation-wavelength-dependent emissions with their max

284 We performed an emission scan at 9 excitation wavelengths common to fluorescent microscopy

285 -function mutations facilitated breakdown of excitation waves at more physiological excitation rates

286 nduction patterns and dynamics of re-entrant excitation waves.

287 on of femtosecond laser pulses and microwave excitations, we report the classical analogue of Rabi os

288 tricle with no SMS and rate 2 and rate 3 SMS excitation were qualitatively similar.

289 Dirac semimetals are known to host fermionic excitations which can mimic physics usually found in ult

290 dia through TRPV1 sensitization and neuronal excitation, which may contribute to the pathogenesis of

291 ike/gas therapy without the need of external excitation, which yields a remarkable H2 O2 -NO cooperat

292 s of cell viability was detected under light excitation, while negligible effects in the dark were de

293 ine splits into distinctive spinon and holon excitations whose dispersions exactly follow the energy-

294 approximately 1 mV under 40 Suns equivalent excitation with 405 nm light.

295 mics of electrons and holes in silicon after excitation with a short laser pulse.

296 Systems hybridising collective spin excitations with microwave photons have recently attract

297 lation was compensated by increased feedback excitation within CA1, thus leading to unaltered firing

298 The foot-shock-driven excitation within the LHb requires glutamatergic signali

299 ts provide a measure of the velocity of edge excitations without contacting the sample, and pave the

300 The use of optical excitation would allow for overcoming all these limitati