ライフサイエンスコーパス: energy level

1 7) on selection of the optimal monochromatic energy level.

2 lar charge transfer and lowering of the LUMO energy level.

3 sists of naphtalene diimides having low LUMO energy level.

4 rphometry is associated with decreased brain energy levels.

5 ransfer on the S1 states and anti-correlated energy levels.

6 onal landscapes of proteins and their rugged energy levels.

7 e substituent effects on their HOMO and LUMO energy levels.

8 ven interactions leading to the splitting of energy levels.

9 nabolic environments in addition to cellular energy levels.

10 s evidence for partial unpinning of the TiO2 energy levels.

11 to a modification of the polymer electronic energy levels.

12 trum, consisting of highly degenerate Landau energy levels.

13 lectronic properties including HOMO and LUMO energy levels.

14 ale heating region is evaluated at different energy levels.

15 respond to glucose during reduced background energy levels.

16 ital and lowest unoccupied molecular orbital energy levels.

17 by transient exposure to hormones signaling energy levels.

18 e to growth factors, nutrients, and cellular energy levels.

19 ls, including growth factors, nutrients, and energy levels.

20 the loop-loop interface in intermediate free-energy levels.

21 p and mixing of the frontier valence orbital energy levels.

22 lar cells was increased by adjusting polymer energy levels.

23 thin film transistors (OTFTs) and molecular energy levels.

24 devices, because of their intrinsic discrete energy levels.

25 hosphorylation, independent of intracellular energy levels.

26 ties, since they possess relatively low LUMO energy levels.

27 increases mitochondrial biogenesis and brain energy levels.

28 d oxidative pathways in response to cellular energy levels.

29 sonance with a particular separation between energy levels.

30 perovskites have a different composition and energy levels.

31 omain wall, displaying discrete quantum-well energy levels.

32 e thermal quenching processes and activation energy levels.

33 able motor activity) and related subjective (energy) levels.

34 in the lowest-sodium model also varied with energy level (~0.5 mg/kcal) and ranged from 500 to 1250

35 ounts in the base model varied directly with energy level (1.0 mg Na/kcal) and ranged from 996 to 317

36 s multiple segments at varying monochromatic energy levels (40-140 keV).

37 rm, allowing application at radiotherapeutic energy levels (50-350 MeV protons, 100-600 Mev/a.m.u car

38 single-energy multi-detector row CT at four energy levels (80, 100, 120, and 140 kVp).

39 ergy multi-detector row CT at four different energy levels (80, 100, 120, and 140 kVp).

40 ze the probability of sustaining appropriate energy levels across the entire foraging trajectory.

41 ectroporation catheter ablation with various energy levels after subxiphoid pericardial puncture.

42 ions play an important role in how molecular energy levels align to the graphene Dirac point, and may

43 R intraribbon heterostructures have a type-I energy level alignment and strongly localized interfacia

44 valent doping on charge-carrier dynamics and energy level alignment at the interface of perovskite NC

45 layers was achieved as a result of favorable energy level alignment at the metal oxide/organic interf

46 The strong electronic coupling and favorable energy level alignment between PbS nanocrystals and bulk

47 The energy level alignment between the highest occupied mole

48 t parameter, the tunneling barrier height or energy level alignment between the molecule and the elec

49 The energy level alignment is found to depend on the molecul

50 ood on the basis of a quantitative interface energy level alignment model, which indicates that bipol

51 geometry in both the contact resistance and energy level alignment of a molecular junction.

52 pectroscopy (CMEAS), for the first time, the energy level alignment of a polymer:fullerene bulk heter

53 that the switch is due to the change in the energy level alignment of the redox states relative to t

54 reveals that, despite the dependence of the energy level alignment on contact geometry, the variatio

55 ing molecular properties like solubility and energy level alignment while maintaining the high fissio

56 IPE spectrum contains information regarding energy level alignment within a complete, working molecu

57 nter to expectations based on more favorable energy level alignment, greater active layer light absor

58 easurably inferior morphology and nonoptimal energy level alignment, resulting in PCEs of 5.34% and 4

59 voltaic characterizations disclosed that the energy level alignment, the molecular orbital profile, a

60 ayer and the substrate acts to influence the energy level alignment.

61 act resistance rather than variations in the energy level alignment.

62 ese systems, such as engineering interfacial energy-level alignment and charge transfer (CT).

63 acteristics of the cell such as respiration, energy level and apoptosis.

64 ross relevant inserts for each monochromatic energy level and iodine concentration.

65 e most probable state with relatively lowest energy level and lowest missing information compared to

66 poorer performance due to its low-lying LUMO energy level and nondisjointed HOMO/LUMO profile.

67 The monochromatic energy level and the lesion iodine concentration had a s

68 f the variance is a function of the selected energy level and the lesion iodine content.

69 a shift toward lower energies of the ligand energy levels and a reduction of the HOMO-LUMO gap.

70 ferences was greatest at lower monochromatic energy levels and at lower iodine concentrations (averag

71 ns are thought to form crucial links between energy levels and cellular metabolism.

72 n was used to identify optimal monochromatic-energy levels and compare them with single-energy CT.

73 In addition to matched energy levels and complementary absorption spectrum with

74 KT and TOR pathways are affected by nutrient/energy levels and endocrine signaling, these data sugges

75 to increase JSC , but also possess suitable energy levels and high mobility to afford high VOC and F

76 ring of phononic heat carriers with magnetic energy levels and increased phonon scattering due to enh

77 We use this method to determine the energy levels and interaction strengths of a fully conne

78 lving competing transitions between multiple energy levels and it has been difficult to precisely det

79 pied or lowest unoccupied) molecular orbital energy levels and optical absorption profiles.

80 The electronic energy levels and optical transitions of a semiconductor

81 Twenty RCTs compared ESWT energy levels and placebo and consistently showed that h

82 -ligand bond length can shift its electronic energy levels and predictably guide electron-transfer re

83 vailability and are required for maintaining energy levels and redox balance as the culture becomes a

84 -withdrawing effect of F, and finally adjust energy levels and reduce bandgap, which is beneficial to

85 which might provide a link between cellular energy levels and regulated secretion.

86 rd, we observe crossing and anti-crossing of energy levels and reveal the non-trivial topological mod

87 porating BAI acceptor possess low-lying LUMO energy levels and small HOMO-LUMO gaps.

88 ve many potential advantages such as tunable energy levels and spectral breadth, but are prone to poo

89 ed devices is attributed to a combination of energy levels and structured surface morphology that cau

90 Given the position of energy levels and the distribution of electronic couplin

91 Electronic properties such as the energy levels and the distribution of HOMOs and LUMOs of

92 lens was enhanced from 7.4 to 11 mm at this energy level, and peak pressure (41 MPa) and maximum cav

93 quantum transition between avoided crossing energy levels, and also results in unexpected magnetic b

94 that promotes growth in response to insulin, energy levels, and amino acids and is deregulated in com

95 omotes growth in response to growth factors, energy levels, and amino acids, and its activity is ofte

96 wide range of signals, including nutrients, energy levels, and growth factors, are known to control

97 wth and metabolism in response to nutrients, energy levels, and growth factors.

98 The extended photoresponse, well-matched energy levels, and high hole mobility from optimized BHJ

99 of the few open quantum systems in which the energy levels, and not just the excited-state lifetimes,

100 ignals, including growth factors, nutrients, energy levels, and various stress conditions, regulates

101 l glycolysis.SIGNIFICANCE STATEMENT Neuronal energy levels are critical for proper CNS function, but

102 hole-transport materials (HTMs) with tunable energy levels are designed and synthesized for efficient

103 erimentally only the electron densities and -energy levels are directly observable.

104 These excitonic energy levels are experimentally found to be robust agai

105 The confined energy levels are highly sensitive to the specific nanos

106 Upon stress, energy levels are maintained by increased mitochondrial

107 While the weakly interacting low-energy levels are used as memory to store classical info

108 g258, the E295K mutant complex has a similar energy level as compared to the wild-type pol beta.

109 l atom through the avoided crossings between energy levels at a fixed frequency.

110 ements and bond distortions that control the energy levels at the valence and conduction band edges,

111 parameters are combined with estimates of 3d energy levels based on the visible-near-IR spectra to yi

112 es contain high protein, low cholesterol and energy levels, being its consumption recommended.

113 Under an excitation at energy levels below 1.3 eV, VSiVC(0) are converted into

114 its allowed for fine control over electronic energy levels both in solution and in the bulk.

115 e these variations by adjusting the electron energy levels, but the more ambitious goal of creating q

116 ivation of interface states and alignment of energy levels by intrinsic molecular polarization, as we

117 f virtual monochromatic images at an optimal energy level can overcome renal cyst pseudoenhancement.

118 , they go through a sequence of states whose energy levels can be computed and arranged into a step-b

119 n of semiconducting polymer frontier orbital energy levels can drive spectral shifts of SWNT hole pol

120 tion that acts as a "dopant," introducing an energy level closer to the electrodes' Fermi level than

121 -Zener formula in the vicinity of an avoided energy-level crossing will cause considerable errors due

122 phase-controlled pulses with up to a 100 muJ energy level, depending on the filling gas, pressure and

123 An energy level diagram for fully decoupled electron- and p

124 ic voltammetry measurements of the ChaMs, an energy level diagram is constructed relating the ChaMs a

125 d Ts as input and generates (i) a nucleosome energy level diagram, (ii) coarse-grained representation

126 thick layer of a single molecule, but if the energy levels differed, the current voltage behavior exh

127 odel agrees well with that of the Fermi/HOMO energy level difference.

128 d lowest unoccupied molecular orbital (LUMO) energy level due to the fluorination of A units.

129 ctric field causes a shift in the electronic energy levels due to the Stark effect, which induces a t

130 the mitochondrial apoptotic pathway and cell energy level during differentiation of mESCs into the ca

131 capture the overpopulation of high internal energy levels during the excitation phase and also the d

132 hase and also the depletion of high internal energy levels during the quasi-steady-state (QSS) dissoc

133 ematically increases the singlet and triplet energy levels (E(S) and E(T)) and blue shifts the absorp

134 a thin polymer interlayer with intermediate energy levels, electrons and holes can effectively shutt

135 o a monoexponential decay, typical of single energy level emitters.

136 nstrate that side-chain conjugation can tune energy levels, enhance absorption, and electron mobility

137 acceptor material, including more favorable energy levels, enhanced light absorption and stronger in

138 We characterize the energy levels, excited state structures, and dynamics of

139 The energy level for the (3)MC state is estimated to lie bet

140 Here we show that, owing to the much higher energy level for the Cu 3d(10) orbitals than for the Ag

141 of these compounds; i.e., (1) the lower HOMO energy levels for BN anthracenes stabilize the molecules

142 Precise energy levels for both the neutral and charged dark exci

143 the smaller splittings between the vibronic energy levels for deuterium, and the KIE increases with

144 rmination of the valence and conduction band energy levels for noncovalently modified (6,5) chirality

145 ns were retrospectively reconstructed at VMI energy levels from 40 to 140 keV in 5-keV increments and

146 CAR amounts in cancer cells altered cellular energy level, glucose uptake, and lactate production.

147 In obesity, fundamental reductions in brain energy levels, gray matter density, and cortical metabol

148 cell growth and proliferation in response to energy levels, growth factors, and nutrients.

149 eeded for an increase in brain energy, brain energy levels have not been directly measured with moder

150 nt method to optimize the hybrid structure's energy levels, here comprising ZnO and a tailored ladder

151 ymers with high molar absorptivity, suitable energy levels, high charge carrier mobility and high sol

152 have deep highest occupied molecular orbital energy levels, high crystallinity, optimal bulk-heteroju

153 ergy difference between the highest occupied energy level (HOMO) of the metal and the lowest unoccupi

154 Cyclic voltammetry was used to determine the energy levels (HOMO and LUMO) in the bistriazines.

155 with adverse events, particularly increased energy level, impulsiveness, decreased concentration, hy

156 lbenzene) based layer, a molecule whose HOMO energy level in a vacuum is close to the Fermi level of

157 ly two-dimensional and its discrete electron energy levels in a magnetic field (the Landau levels) ar

158 he correct ordering of singlet excited-state energy levels in a pentacene molecule (E (S1) < E (D)) f

159 The SnRK1 protein kinase balances cellular energy levels in accordance with extracellular condition

160 not known whether lactate acts by preserving energy levels in axons or in oligodendrocytes, the myeli

161 ergetic offsets between the charge transport energy levels in different morphological phases of polym

162 ported by quantum-chemical simulation of SiV energy levels in small nanodiamonds.

163 tic activity is due to aligning the protonic energy levels in the PCET steps, while improving the act

164 toelectron spectroscopy to characterize hole energy levels in the polymer phases of polymer:fullerene

165 allenge of controlling molecular packing and energy levels in the solid state precludes clear determi

166 e demonstrate voltage tunability of the spin energy-levels in a single quantum dot by modifying how s

167 tunnelling spectroscopy we obtain charge and energy-level information for these boron nitride defect

168 nanocomposite resulted in spatially varying energy levels inside the nanocomposite that enhanced the

169 a higher lowest unoccupied molecular orbital energy level (IOIC2: -3.78 eV vs IHIC2: -3.86 eV), broad

170 w enthalpy of formation, and that the defect energy level is a shallow donor to the conduction band r

171 The measurement and understanding of their energy levels is key to scientific and technological pro

172 An anticrossing of the driven dot energy levels is observed when the Zeeman and valley spl

173 The spin-1/2 system, with two quantum energy levels, is essentially the most nonlinear system

174 anging molecular structure will alter system energy levels leading to a change in the transport barri

175 proach was used to investigate the effect of energy level, lesion size, lesion iodine content, and im

176 HOMO) of the metal and the lowest unoccupied energy level (LUMO) of the molecule.

177 rapamycin prevented the increase in cellular energy levels, lysosomal biogenesis, and endocytic uptak

178 ed highest occupied molecular orbital (HOMO) energy level mainly due to the additional octyl on the D

179 Yet its energy levels manifest the anharmonic structure associat

180 he PBB3 polymer also showed both a favorable energy level match with PCBM (with a LUMO energy level o

181 ures and of the medium can produce transient energy level matching among multiple electronic states.

182 Cs) provides higher carrier mobility, better-energy level matching, and superior stability, as well a

183 enhanced head CT scans at 65-75 keV (optimal energy levels) maximizes image quality compared with sca

184 Brain energy levels may therefore constitute a predictive valu

185 onventional CdSe/ZnS QDs, which have a large energy level mismatch between CdSe and ZnS and thus show

186 Fine energy-level modulations of small-molecule acceptors (SM

187 ed in detecting and interpreting nutrient or energy levels-most notably, the insulin/insulin-like gro

188 , due to fractal nature, generation of newer energy levels never stops.

189 s determined, including COX activity, tissue energy levels, noninvasive and invasive lung function, a

190 ause its modulation in vitro alters cellular energy levels, O consumption, and contractility.

191 plays a critical role in regulating cellular energy levels, observations that have broad implications

192 le energy level match with PCBM (with a LUMO energy level of -3.29 eV) and a favorable film domain mo

193 tic energy of membrane thinning elevates the energy level of interfacial binding with the peptide con

194 motions, is found to depend strongly on the energy level of local mesoscale eddy variability.

195 nique for examining position of the impurity energy level of p-type dopants in nitride semiconductors

196 formation is due to the lowering of the HOMO energy level of the aryl moiety to reduce the process of

197 ngs are shown to dramatically lower the LUMO energy level of the carboxonium electrophile (compared t

198 sor system; it can encode sensitivity to the energy level of the cell and creates independent topolog

199 ture is due to appropriately positioning the energy level of the charge-separated state below the tri

200 efect state that resides below the predicted energy level of the dark excitons.

201 e lowest unoccupied molecular orbital (LUMO) energy level of the porphyrins and, consequently, facili

202 As we correlate each energy level of the resonance band of organic jelly, as

203 ties, since they possess relatively low LUMO energy levels of -3.3 to -3.6 eV (as determined by diffe

204 ced at small negative potentials giving LUMO energy levels of -3.57 to -3.74 eV.

205 l monochromatic images were reconstructed at energy levels of 40-140 keV (in 10-keV increments) in ei

206 resolution, in the vacant space between two energy levels of a given resonance band, a new band appe

207 effect of a dense plasma environment on the energy levels of an embedded ion is usually described in

208 estimated by calculations only involving the energy levels of an isolated neutral atom.

209 (3) modification of g-C3N4 with well-matched energy levels of another semiconductor or a metal as a c

210 off-resonance light can be used to shift the energy levels of atoms, molecules, and solids.

211 es, approaches can be devised to control the energy levels of cation sublattices in semiconductors.

212 vskite solar cells comes from the nonmatched energy levels of charge transport layers.

213 Furthermore, the electronic energy levels of even the same spin are dense on the sca

214 ) and phi of 5-17 and computed HOMO and LUMO energy levels of fragments of 5-17, i.e., 8-vinyl 9-Me-a

215 the confined electronic orbitals and related energy levels of individual semiconductor quantum dots h

216 , we implement a technique for resolving the energy levels of interacting photons.

217 hibited by the difficulty in determining the energy levels of molecules after being perturbed by inte

218 onal theory for calculations of valence band energy levels of nanoscale precipitates of CdS, CdSe, Zn

219 e into the polymer backbone reduced the HOMO energy levels of polymers.

220 e potentiometric valence and conduction band energy levels of semiconducting carbon nanotubes; (ii) p

221 es of the model quartic potential and in the energy levels of the [H, C, N] potential energy surface.

222 etween the donor and acceptor states and the energy levels of the bridging molecule.

223 sis of the DFT calculations of the HOMO-LUMO energy levels of the chiral forms, these compounds can b

224 paring the singly occupied molecular orbital energy levels of the corresponding phosphine radical cat

225 elated to the offset of the frontier orbital energy levels of the donor and acceptor components, whic

226 The energy levels of the donor-acceptor conjugates were fine

227 p to 0.33 A impart remarkable effects on the energy levels of the frontier orbitals of Au25(SR)18(-)

228 ion via Channel I and II pathways, including energy levels of the materials involved, exciton diffusi

229 The structures and energy levels of the molecular layers included donor mol

230 nown to cause broadening and shifting of the energy levels of the molecule; this, in turn, is expecte

231 ffectively impact the optical properties and energy levels of the molecules.

232 Valence and conduction band energy levels of the NaCl-type metal sulfides, MS (M = P

233 vice resistances track with the valence band energy levels of the PM(n) wire, which were modulated vi

234 t the local electric field that broadens the energy levels of the PNA nucleobases.

235 The HOMO energy levels of the polymers can be progressively incre

236 The relative energy levels of the possible transition states of the I

237 ty in fine-tuning the absorption spectra and energy levels of the resultant polymers for achieving hi

238 duce disorder to study the statistics of the energy levels of the system as it undergoes the transiti

239 g, electronic inductive effects modulate the energy levels of the system resulting in compression of

240 A dynamic model based on the energy levels of the two early charge-separated states,

241 When the energy levels of the two molecular layers were similar,

242 nate leads to a splitting of the vibrational energy levels of the umbrella mode.

243 he highest occupied molecular orbital (HOMO) energy levels of their fluorophores.

244 al and electrochemical properties as well as energy levels of this series of donor molecules were tho

245 The model is based on quantized energy levels of transition states and products, and it

246 ded crossings of the quantum mechanical spin energy-levels of radicals formed in cryptochromes.

247 ent obstacle to that end is the unfavourable energy level offset at hybrid inorganic/organic structur

248 at exhibits the smallest donor/acceptor LUMO energy level offset, the photocurrent quantum yield fall

249 The effect of acceptor energy level on electron transfer rate in blends of the

250 Modulation of its energy level on the energy landscape in photosynthetic v

251 they represent physiological states such as energy level or stress in response to environmental and

252 -D structure, donor state density, and Fermi energy level position are critical for maintaining the s

253 s were reconstructed in 10-keV increments at energy levels ranging from 40 to 140 keV.

254 ad an energy fluence of 9 mW/cm(2) and total energy levels ranging from 5.4 J/cm(2) up to 10 J/cm(2)

255 Virtual monochromatic images at energy levels ranging from 80 to 140 keV did not show ps

256 occurred on virtual monochromatic images at energy levels ranging from 90 to 140 keV.

257 alent to a Nernst distribution for one redox energy level, redox site coverage is both underestimated

258 occupied molecular orbital (LUMO) (-3.80 eV) energy levels relative to ITIC1 (HOMO: -5.48 eV; LUMO: -

259 of the gate is simply to shift the molecular energy levels relative to the metal Fermi level.

260 e molecular orbital energies and the contact energy level resulting in a leveling effect that compres

261 We show the analogy between the energy level schemes of the special pair and of the lase

262 The network is also modular, containing energy level sensing proteins that connect to four outpu

263 ments so far have not shown valley-selective energy level shifts in fields accessible in the laborato

264 These energy level shifts may play a major role in PSC perform

265 e, Wigner conjectured that the statistics of energy level spacings would be the same as for the eigen

266 ly observed the discrete, non-equally-spaced energy-level spectrum of LLs, including the hallmark zer

267 hrough a singlet-triplet anticrossing in the energy-level spectrum.

268 The strategy for tailoring the energy level splitting of Ln ions by the highly designab

269 A key finding is that the S(1)-->S(2) energy level splitting, previously used as evidence for

270 aspects of upconversion processes, including energy level splitting, transition probability, line bro

271 ns in the host materials can determine their energy level splitting, which is of vital importance to

272 zed as the host material to embed Eu(3+) and energy-level splitting was achieved for tuning its photo

273 er band gaps are narrowed mainly due to LUMO energy level stabilization.

274 store classical information (bits), the high-energy levels strongly interact with neighboring magnets

275 The energy-level structure of a quantum system, which has a

276 increased visible light absorption, altered energy level structures, and variable cage geometries, w

277 old molecules require a variety of molecular energy-level structures (for example unpaired electronic

278 regulation of GAMT allows cells to maintain energy levels sufficient to undergo apoptosis or surviva

279 the regional and gene-specific responses to energy levels suggest a complex, interactive network whe

280 re generally poorly conducting because their energy levels tend to lie far from the Fermi energy of t

281 For each vascular compartment, the energy level that provided optimal evaluation on virtual

282 m(2) attributable to the proper alignment of energy levels that led to the efficient harvesting of ex

283 core positions, respectively, and gave LUMO energy levels that range from -3.57 to -4.14 eV.

284 PDK1-3 and PDH phosphorylation and decreased energy levels that were significantly ameliorated after

285 sparency, good conductivity, and appropriate energy levels, the solar-cell efficiency and lifetime ar

286 re hydrophobic and have slightly higher LUMO energy levels, thus providing better device performance

287 sor that responds to alterations in cellular energy levels to maintain energy balance.

288 , this dye possesses favorable HOMO and LUMO energy levels to render efficient sensitizing action in

289 Delivery of higher laser energy levels to the RPE/choroid complex resulted in a s

290 favor of the T form, which moves to a higher energy level upon oxygen release.

291 rturbation theory calculations of electronic energy levels, we determined the band edge positions of

292 tenuation for each insert and reconstruction energy level were recorded.

293 the average width and spacing of electronic energy levels: when this dimensionless ratio falls below

294 d renders cleavage sensitive to the cellular energy level, which may be a general feature of CBS-doma

295 However, as we moved into higher free-energy levels, which are farther from the loop-loop inte

296 al estimations of frontier molecular orbital energy levels, which are reported and discussed.

297 We found that the lowest free-energy levels, which are situated in the vicinity of the

298 ers as the dipole layer to tune the relative energy levels, which can potentially maximize the open c

299 onductance reveals peaks indicating discrete energy levels with higher electronic density of states.

300 etry revealed a gradual decrease of the LUMO energy levels with increasing chain length, while absorp