ライフサイエンスコーパス: excite

1 when well-defined electronic transitions are excited.

2 is emitted when the nanocrystal is optically excited.

3 Thus, the novel multiphoton-excited 3D printing technique produces extracellular mat

4 Here, we used multiphoton-excited 3D printing to generate a native-like extracellu

5 ce we first show that simple light steps can excite a subset of VPM neurons.

6 injection, and activation of mACh receptors excited a majority of LHb neurons in in vitro electrophy

7 Here we show that BomoTx excites a cohort of sensory neurons via ATP release and

8 ns to a high-intensity state of the directly excited acceptor fluorophore on a DNA tether are due to

9 NG, also known as MITA, MPYS, or ERIS) is an exciting adjuvant target due to its role in cyclic dinuc

10 Exciting advancements have been made in the field of fle

11 The last years have also seen exciting advances in the chemical and physical character

12 These exciting advances reveal the complexity of the pathogeni

13 archaeal life and illustrate the unique and exciting advantages that single-cell genomics offers ove

14 and wide-field collection optics are used to excite and collect the fluorescence emission of these pa

15 h respect to the emissive Ru --> dpp (3)MLCT excited and cannot be formed by static electron transfer

16 is intermediate between that of the locally excited and CT states, approximately reflecting the degr

17 potentials of the photocatalyst in both the excited and the ground states is necessary to obtain a p

18 cal issues in order to make the most of this exciting and evolving technology.

19 Protein tyrosine phosphatases (PTP) are exciting and novel targets for cancer drug discovery tha

20 oy unfamiliar or novel technology, it's both exciting and very worthwhile to form collaborations.

21 New strategies are evaluated and novel, exciting applications are shown.

22 aration of a set of appropriate analogs with exciting applications in the area of host-guest organic

23 One of the exciting applications of molecular technology is the dir

24 showed strong fluorescent emission at 450nm excited at 365nm which quenched in presence of Metronida

25 derivatives and argpyrimidine (ArgP) can be excited at the red edge of the Trp absorption band which

26 article-based drug delivery, opening several exciting avenues for selective and prolonged cardiac the

27 y lifestyle, and further probing will answer exciting basic microbiological and clinically relevant q

28 molecules on the nanoscale, leading to many exciting biological discoveries.

29 ing the ultrafast dynamics of electronically excited BODIPY chromophores could lead to further advanc

30 hotocurrent was measured when the sensor was excited by a 405nm 100mW laser light.

31 near-field mode of a dielectric nano-grating excited by a femtosecond laser pulse with an optical per

32 r-coated glass slide with a thin spacer, and excited by a laser-diode from the backside through a gla

33 ese devices, a charge-density plasma wave is excited by an ultra-relativistic bunch of charged partic

34 patially organized, so that the cell is most excited by clutter rather than isolated objects.

35 Furthermore, OND RGCs are excited by light falling far beyond their dendrites.

36 n, indicating that individual neurons can be excited by more than one astrocyte and that individual a

37 ovement, are inhibited by Purkinje cells and excited by mossy fibres.

38 owed NPVF neurons and vRN are suppressed and excited by noxious stimuli, respectively.

39 ncipal cells: Approximately 15% of cells are excited by odor, and another approximately 15% have thei

40 nge neurons in the cuneate nucleus (CN) were excited by peripheral stimulation.

41 Some of them were excited by visible light irradiation and emitted fluores

42 patial patterns and show that many units are excited by visual motion in a direction-selective manner

43 Stimulation of vestibular efferent neurons excites calyx and dimorphic (CD) afferents.

44 Cyano radicals and excited carbon monoxide molecules in particular are reac

45 e ultrafast spatial and temporal dynamics of excited carriers are important to understanding the resp

46 sight into the ultrafast spatial dynamics of excited carriers in materials.

47 avior represents one of the biggest and most exciting challenges of systems neuroscience.

48 organic frameworks (MOFs) have emerged as an exciting class of porous materials that can be structura

49 ne their biology to enable symbiosis, and an exciting coalescence of genome mining, lipid profiling,

50 asing the solvent polarity and stems from an excited complex (i.e., an exciplex).

51 trated an efficient energy transfer from the excited Coumarin 2 to the ground-state Coumarin 343 in t

52 In summary, the treatment of CRS is at an exciting crossroad.

53 generation in crystalline solids1-6 marks an exciting development, with potential applications in hig

54 Here, we review these exciting developments and highlight key remaining challe

55 Finally, recent exciting discoveries within the field of in vivo manipul

56 o whom neuroscientists typically communicate exciting discoveries-that is, those who can provide more

57 excitation wavelength, we could specifically excite either the monomeric species or the fluorescent n

58 ry calculations of the X-ray spectra for the excited electronic singlet and triplet states.

59 uential structural evolution of CNCbl in the excited electronic state.

60 We discuss the generation of excited electronic states and electron-hole pairs (excit

61 Highly excited electronic states are challenging to explore exp

62 We are entering an exciting era where the ancient wisdom distilled into the

63 arkinson's disease are moving into a new and exciting era, with several groups pursuing clinical tria

64 mmentaries meet these claims with a range of exciting extensions and applications, as well as critiqu

65 nd directions for future development in this exciting field are provided.

66 nadequately validated antibodies can lead an exciting field astray.

67 Two-photon excited fluorescence (TPEF) imaging is a non-destructive

68 pering the interpretation of evanescent-wave excited fluorescence intensities is the undetermined cel

69 anti-Stokes Raman scattering and two-photon excited fluorescence microscopy, we show that CDCP1 depl

70 ce charge field in the crystal caused by the excited free carriers.

71 ellent results obtained allow envisioning an exciting future for the development of novel application

72 e using helminth-derived products is also an exciting future prospect.

73 tion attributed to 5-HT2 receptor activation exciting GABAergic interneurons.

74 A resting atom excites if a sum of its excited hard neighbours and a weighted sum of its soft n

75 A resting atom excites if a sum of its excited hard neighbours and a we

76 When electron-hole pairs are excited in a semiconductor, it is a priori not clear if

77 rpreted by the dispersion of surface plasmon excited in the air TiO2 InSb trilayer system.

78 hat a surface plasmon resonance (SPR) can be excited in this case.

79 m APOLT safely has also opened up a range of exciting indications in the setting of NCMLD.

80 lectrons precipitating in the polar regions, exciting intense aurorae, observed simultaneously by the

81 hemisphere in neglect is pathologically over-excited it ought to be suppressed.

82 training prepares scientists for an array of exciting job opportunities, one of which is as a faculty

83 At this exciting juncture, it is timely to review these new meth

84 hat aversive stimuli, including foot-shocks, excite LHb neurons and promote escape behaviors in mice.

85 ies are corroborated with those of thermally excited magnon number and magnon propagation length to s

86 aturation of carrier occupation in optically excited materials is a well-established phenomenon.

87 tional mode specificity in the vibrationally excited methane reactions.

88 after electron injection as compared to the excited MLCT state of the unbound Re catalyst or when im

89 Collectively, these results establish an exciting model of tendon regeneration and uncover a nove

90 Here we demonstrate that laser-excited muon pump-probe spin spectroscopy (photo-muSR) c

91 fer salt concentration, correlating with the excited nanoscale dynamics.

92 ion, reassembly (ADOR) method represents one exciting new approach to obtain solids with targeted str

93 mechanosensitive, these findings open up an exciting new avenue of research into the fundamental mec

94 Taken together, the data open exciting new avenues for structure-based drug design.

95 ersatile E. coli system to be employed as an exciting new carbon capture technology or as a cell fact

96 The cultural intelligence hypothesis is an exciting new development.

97 The latter are exciting new directions for the field that will likely i

98 cal electrically excitable cells could yield exciting new findings.

99 h also serves as a roadmap into the vast and exciting new landscape of questions about the computatio

100 , and force-mapping techniques are providing exciting new opportunities for future research into bran

101 flavin dynamics in this enzyme class offers exciting new opportunities for inhibitor design.

102 Some of the exciting new possibilities offered by 2D crystals are di

103 The 2D monolayer-capping approach opens up exciting new possibilities to enhance the thermal stabil

104 ventional superconductivity in SLG offers an exciting new route for the development of p-wave superco

105 ranscatheter mitral therapy as a potentially exciting new strategy to improve the lives of patients w

106 ug carriers at the 'nano'-scale is providing exciting new therapeutic strategies in clinical manageme

107 Gene therapy is providing exciting new treatment options for patients with PIDs, a

108 Exciting new work on autophagy-modulating proteins that

109 nse laser pulses transforms them into highly-excited non- equilibrium states.

110 ima in the VA potentials associated with the excited OH vibrational states are shifted away from the

111 metal chalcogenide nanocrystals (NCs) offer exciting opportunities as novel materials to be explored

112 ding two bits of data per clock period opens exciting opportunities for data-carrying capacity enhanc

113 Mechanochemistry offers exciting opportunities for molecular-level engineering o

114 genomic properties of human tumors, provides exciting opportunities for non-invasive diagnostics and

115 n the nanosecond time scale, which points to exciting opportunities for ultrafast and novel skyrmioni

116 Metasurfaces offer exciting opportunities that enable precise control of li

117 These rich datasets offer unprecedented and exciting opportunities to address long standing question

118 from a machine learning perspective provides exciting opportunities to improve diagnostic precision a

119 omega-TAms have emerged as an exciting option for their synthesis, offering a potentia

120 nce is subsequently separated from the photo-excited oscillatory resistance using a multi-conduction

121 An exciting paradigm emerging in cancer biology is that onc

122 molecular design possibilities have enabled exciting photophysical attributes including narrower emi

123 The information reported herein provides exciting possibilities for industrial/biotechnological a

124 ght into backbone dynamics in IDPs and opens exciting possibilities for the design of disordered ense

125 erlying molecular mechanisms, and highlights exciting possibilities to exploit gene and genome transf

126 This finding offers the exciting possibility of estimating conditions of formati

127 atterns, and metabolite concentrations, with exciting potential for neurorehabilitation.

128 a in the regulation of tolerance to food has exciting potential for new interventions to treat dietar

129 Thus, Wolbachia represents an exciting potential new form of biocontrol for arboviral

130 yield breakthrough results, and envision the exciting potential of high-performance nanomaterials tha

131 Our research demonstrates the exciting potential of this novel photocatalyst for the d

132 With a dozen antifibrotic agents possessing exciting preclinical potential in the armory, it seems c

133 bstracting a surface O-atom, then forming an excited precursor state, which dissociates to produce O2

134 Recently exciting progress has been made on this problem, but the

135 and Juergen Knoblich begin by discussing the exciting promise of organoid technology and give concret

136 ears poised for breakthroughs, including the exciting prospect of resolving the conformations and ene

137 optimization for VEEV antivirals, and is an exciting prospect to identify inhibitors for the many ot

138 These advances highlight the exciting prospects for future tools based on the continu

139 ignals via climbing fibres, which powerfully excite Purkinje cells, evoking complex spikes and depres

140 ering (SEHRS) is the spontaneous, two-photon excited Raman scattering that occurs for molecules resid

141 ent state-of-play with a particular focus on exciting recent advances in the identification of potent

142 Exciting recent studies highlight the discovery of at le

143 iseases (ID) has always been challenging and exciting, recognition of the value that ID physicians pr

144 or-1,2,3,4-didehydroretinal (MMAR), produced exciting results.

145 Our work opens an exciting route for the exploration of topological physic

146 r electron transfer (ET) between the triplet excited saccharin moiety and sulfur atom.

147 encodes heading and angular velocity, and is excited selectively by turns in either the clockwise or

148 ortho sites on an aromatic ring in its first excited singlet state.

149 to changes in the viologen structure in the excited singlet state.

150 e subsequent reactions of these first formed excited species lead to the production of ground-state p

151 t with an extended pi-electron system on the excited species obtained during the chemiexcitation path

152 Fe(2+) ion, and FeF2 and characterizes their excited spin states.

153 es characteristic of light- or X-ray-induced excited-spin-state trapping.

154 the quinone-containing ligand, affecting the excited state and electron transfer properties of these

155 acilitating electron collection at Rh in the excited state and reductively quenched state.

156 presence of a highly mixed (3)MLCT/(3)pipi* excited state as the lowest triplet state in 2, whereas

157 Excited state behavior follows predicable patterns.

158 ults from intramolecular interactions in the excited state between the electron-rich aniline and the

159 a given MOF that are primed to form such an excited state complex.

160 Here, the synthesis and excited state dynamics of a conjugated tetracene homopol

161 Npi*), does significantly participate in the excited state dynamics.

162 Here, we report an atomistic model of the excited state ensemble of a stabilized mutant of an exte

163 The most striking feature of the resulting excited state ensemble was an unstructured N-terminus st

164 t, or the absence of a sufficiently reducing excited state for electron injection into appropriate se

165 ch confirmed that the mixed (3)MLCT/(3)pipi* excited state in 2 promotes ligand dissociation, represe

166 nstrate that the spin-strain coupling in the excited state is 13.5+/-0.5 times stronger than the grou

167 that a softening of vibrational modes in the excited state is involved in efficient and rapid energy

168 In fluorophores, the excited state lifetime can be modulated using pump-probe

169 fferent strategy that relies on the peculiar excited state lifetime features of the SYBR Green (SG) d

170 The excited state meta effect, also known as the meta-ortho

171 Using density functional theory and excited state methods, we derive the molecular origins o

172 The energy of the triplet excited state of each complex was estimated from energy-

173 lytically dominant pathway proceeds from the excited state of Li(carb), generating a carbazyl radical

174 are consistent with pathways wherein both an excited state of the copper(I) carbazolide complex ([Cu(

175 In the excited state of the E:THF:NADPH product release complex

176 rbazolide complex ([Cu(I)(carb)2](-)) and an excited state of the nucleophile (Li(carb)) can serve as

177 lidene, as well as vibronic coupling with an excited state of vinylidene.

178 The mixed (3)MLCT/(3)pipi* excited state places significant spin density on the qui

179 rovide a complete mechanistic picture of the excited state relaxation of dCyd/5mdCyd in three solvent

180 ultaneously can differentiate strong triplet excited state sensitizers from hydroxylating species suc

181 ctron properties of the ligand stabilize the excited state sufficiently to realize a long charge-tran

182 he presence of a trans-type influence in the excited state that enhances ligand exchange.

183 The most probable excited state that leads to elimination of nitrogen and

184 le dynamics, only the MCA samples a dominant excited state that resembles the TSA, as evidenced by th

185 Photodriven electron transfer from a donor excited state to an assembly of electronically coupled a

186 buting to the optically active excited state-excited state transitions, and suggest a simple rule to

187 modified as a result of the presence of the excited state wavefunction.

188 tion of DAPP(2+) at 505 nm populates a lower excited state where electron transfer is kinetically unf

189 (tau = 19 ns) Ru(dpi) --> qdpq(pi*) (3)MLCT excited state where the promoted electron is delocalized

190 the vibrational cooling of the Franck-Condon excited state, indicative of nonequilibrium dynamics.

191 here the polar CT state is the lowest energy excited state, we observe its population through signifi

192 the resonator through its orbitally-averaged excited state, which has a spin-strain interaction that

193 with both 1) the energy of a low-lying (4) E excited state, which has been postulated to be involved

194 tations contributing to the optically active excited state-excited state transitions, and suggest a s

195 y preparing a long-living wave packet in the excited state.

196 the photoreaction involves an electronically excited state.

197 ex analogue or the apo state as its dominant excited state.

198 f the configurations sampled, on the locally excited state.

199 ated trapping barriers in the electronically excited state.

200 via conrotatory ring closure in the triplet excited state.

201 tational analysis of geometry changes in the excited state.

202 leading to the generation of the luminescent excited state.

203 d light, energy transfer occurs from triplet excited-state (3)PS* to a photolabile triplet state of M

204 is inefficient in the product region so that excited-state (4) Fe(+) is the dominant product.

205 g (ISC) quantum yields (PhiISC), and triplet excited-state (T1) lifetimes on the microseconds time sc

206 We find that the TT excited-state absorption spectral shape correlates with

207 f these alternative (possibly lower barrier) excited-state channels.

208 This new concept of switching of excited-state configuration should pave the way to contr

209 We present a system of excited-state control for truly local delivery of single

210 the favourable band alignment and transient excited-state Coulomb environment, rather than solely on

211 nescent at room temperature, and their rapid excited-state deactivation precludes their use as photos

212 urrents, yet similar yields for nonradiative excited-state decay from the photoacids and the Ru(II) d

213 Here the excited-state dynamics and structural evolution of the p

214 At the forefront of our investigations are excited-state dynamics deduced from femtosecond transien

215 The excited-state dynamics initiated at 266 nm ((1)pipi*, S2

216 Such states are often invoked in the excited-state dynamics of donor-acceptor dyads, but thei

217 tional, long-range charge transport from the excited-state electron donor via a transient C60(*-) tow

218 In 1 N HBr (aq), the photocatalyst undergoes excited-state electron injection and light-driven Br(-)

219 etic quenching by the Co(II) species and (2) excited-state electron transfer to Co(III) species.

220 ysical characterization of their ground- and excited-state features has also been included, paying pa

221 The extent of ground- and excited-state interchromophoric interaction among the pi

222 The exception is amine 4 that undergoes excited-state intramolecular proton transfer (ESIPT) in

223 the mechanism of fluorescence sensing to be excited-state intramolecular proton transfer (ESIPT).

224 Selective excited-state intramolecular proton-transfer (ESIPT) pho

225 s generated via electron transfer between an excited-state iridium photocatalyst and an amine substra

226 cule energy gap, temperature and the triplet-excited-state lifetime of the molecular adsorbate.

227 significant differences are observed in the excited-state lifetimes by transient absorption spectros

228 nsfer from an iridium sensitizer produces an excited-state nickel complex that couples aryl halides w

229 Here, we demonstrate excited-state organometallic catalysis via such an activ

230 the density functional embedding theory, the excited-state potential energy surfaces for dissociation

231 infrared (NIR) spectrum along with favorable excited-state properties for use in solar-energy convers

232 The excited-state quenching of [Ru(TAP)2(HAT)](2+) (TAP = 1,

233 respect to mediator is attributed to triplet excited-state quenching via (1) energy transfer or param

234 with heteroatoms often possess an important excited-state relaxation channel from an optically allow

235 correlation functional (HSE06), treating the excited-state species as excitons with triplet multiplic

236 atter ((3)CDOM*) is a short-lived mixture of excited-state species that plays important roles in aqua

237 cited vibrational dynamics which survive the excited-state structural evolution.

238 that blocks the major deactivation pathway: excited-state trans-to-cis polyene rotation.

239 insic chromophore property, and by improving excited-state trapping, protein interactions enhance the

240 g the initially prepared singlet and triplet excited-state wave functions, we (i) show that the relat

241 nzo[a,e]pentalene modifies the first triplet excited states (T1) of the compounds.

242 tive reactions prevent formation of reactive excited states and photoinhibition.

243 ical model to study the structure of protein excited states and rationally design validating experime

244 Excited states are by definition transient species, and

245 probably due to nonradiative deactivation of excited states by N-H bonds.

246 easurements and recent knowledge of lifetime excited states in MIL-125-type of solids.

247 the adsorbate molecule, and crossing between excited states may effectively lower the dissociation ba

248 Ultrafast spectroscopy was used to probe the excited states of 1-4, which confirmed that the mixed (3

249 facilitated mixing with highly vibrationally excited states of acetylene, leading to broadening and/o

250 rearrangement is one of the highest singlet excited states of diazotetrahydrofuranone.

251 trol the rate of formation (Rf,T) of triplet excited states of dissolved natural organic matter ((3)D

252 uorescence spectra indicate that the singlet excited states of these nanorings are highly delocalized

253 better fine-tuned than others to sustain the excited states of these species.

254 re more typically observed in electronically excited states reached by absorption of ultraviolet or v

255 ents that they undergo, in particular of the excited states that connect chemistry to biological func

256 nfinement with the formation of self-trapped excited states that give efficient bluish white-light em

257 toredox quenching of the carbostyril antenna excited states was observed for all Eu(III)-complexes an

258 al/ligand-to-ligand charge-transfer (ML-LCT) excited states were observed in all four complexes.

259 e to the availability of many electronically excited states with intermediate energies arising from t

260 equilibrium with short-lived low-abundance 'excited states' that form by reshuffling base pairs in a

261 esults from annihilation between high-energy excited states, producing energetically hot states (>6.0

262 haracterize the identity and dynamics of the excited states, where singlet and triplet Rh2/form-to-na

263 ion differs from dynamics occurring on lower excited states, where the timescale required for the wav

264 e state and less-populated intermediates, or excited states, which can play critical roles in both pr

265 emical processes occurring from equilibrated excited states.

266 ing potential applications of their combined excited states.

267 nformations during formation of two distinct excited states.

268 or nonradiative processes occurring in upper excited states.

269 al complexes with long-lived charge-transfer excited states.

270 positions of the lowest singlet and triplet excited states.

271 lly isolated proximal and distal qdppz-based excited states; the former is initially generated and de

272 overning the interplay between the different excited states; unexpectedly, water favors population of

273 ghts into the complex nature of the relevant excited-states.

274 history of organocerium(iv) compounds is an exciting story of ups and downs.

275 Resonantly excited, such metal nanostructures feature collective os

276 highlight how further improvements to these exciting technologies, based on the development of quant

277 c fields produced by thermal fluctuation can excite the near-field optical states, creating the poten

278 sely, urethral flow at high bladder volumes, excites the bladder (micturition reflex) and relaxes the

279 ch stimulation of the receptive field center excites the cell whereas stimulation of the surrounding

280 the circular polarization of the light that excites the electron donor and the imprinted chirality o

281 By exciting the host semiconductor with light that resonate

282 hotoacoustic tomography breaks this limit by exciting the targets with diffused photons and detecting

283 repump laser with an energy above 1.3 eV can excite this charged state and recover the bright neutral

284 These are exciting times and the pace of discovery is remarkable.

285 We are excited to introduce a new design for JEM.

286 igations suggest that IRPL is generated from excited-to-ground state relaxation within the principal

287 make fast changes in the Hamiltonian without exciting transitions.

288 hanisms and target biology, which facilitate exciting translation of this research to many areas of d

289 Excited triplet state chromophoric dissolved organic mat

290 tron spin density distributions of the first excited triplet states are strongly affected by the mole

291 IPY-anthracene dyads (BADs) generate locally excited triplet states by way of photoinduced electron t

292 nstants, and electron-spin structures of the excited triplet states for the metal-free room-temperatu

293 To this end, we excite two FRET donors mTFP1 and LSSmOrange with a 440 n

294 or molecular species, and these species are excited using an external laser source, the radiation li

295 We suggest that METH-activated sacral CPGs excite ventral clusters of sacral VF neurons to deliver

296 Z) media, while they can also be selectively excited via bound eigenmodes.

297 pose that the hot electron and hole carriers excited via Landau damping (during the plasmon decay) ar

298 The decay is accompanied by coherently excited vibrational dynamics which survive the excited-s

299 The orexin neurons excite wake-promoting neurons in the basal forebrain (BF

300 lization, which lifts the scaling ceiling in exciting ways.

301 based on the chlorophyll (Chl) fluorescence excited with red (R) and green (G) light.