ライフサイエンスコーパス: high energy

1 in a bipolar subcellular pattern in media of high energy.

2 eation of prismatic crystal planes of ice on high-energy (100) surface planes of feldspar.

3 ar approach is also described for generating high-energy 4-12 mum sub-cycle pulses via OPCPA pumped b

4 y can facilitate large crushing strains with high energy absorption, optical bandgaps and mechanicall

5 single ionized outflow, linking the low- and high-energy absorption lines.

6 erators, including the development of staged high-energy accelerators.

7 of glioblastoma with cytotoxic short-range, high-energy alpha-particles would be an effective therap

8 tem combines, for the first time, large FOV, high energy and fast scanning.

9 owing demand for energy storage devices with high energy and high power densities, long-term stabilit

10 erials for use in lithium-ion batteries with high energy and power densities, but they are challengin

11 devices and electric vehicles, due to their high energy and power densities.

12 The symmetric lithium-ion chemistry exhibits high energy and power density and long cycle life, due t

13 tial to achieve the winning combination of a high energy and power density.

14 3.0 V in an aqueous electrolyte, as well as high energy and power performance, nearly 100% coulombic

15 eing herded out of urban spaces that contain high-energy anthropogenic food sources.

16 ng a safe and long-life Li metal battery for high-energy applications.

17 rucial role of multiscale kinetic physics in high-energy astrophysical plasmas.

18 s puckered; the result here was a relatively high energy barrier to N-inversion and a low barrier to

19 ly exploit four-way branch migration, with a high-energy barrier to minimize leakage, and three-way b

20 highly puckered; the result was a relatively high-energy barrier to ring-flip and a low barrier to N-

21 tive materials to enable the next-generation high-energy batteries.

22 ily caloric intake and provide the basis for high-energy bioproducts, chemical feedstocks for countle

23 Conclusion CC fractures are common in high-energy blunt chest trauma and often occur with mult

24 d dietary CV risk factors, and compared with high-energy breakfast, habitual skipping breakfast was a

25 terns of breakfast consumption were studied: high-energy breakfast, when contributing to >20% of tota

26 hemical energy storage devices with not only high energy but also high power densities.

27 cascade, the management and manipulation of high-energy carbocation intermediates that propagate the

28 Productive high-energy charge-transfer (CT) states are populated wi

29 n for increased photon interaction, even for high-energy clinical radiation beams.

30 h present direct solid-state counterparts of high-energy collider experiments on the induced fission

31 the light sources, free electron lasers, and high energy colliders based on laser plasma acceleration

32 tem with fragmentation methodologies such as high-energy collision dissociation (HCD) and collision i

33 identities of separated species validated by high-energy collision dissociation experiments.

34 OS ions were subsequently activated by CID, high-energy collision-induced dissociation (HCD), or UVP

35 ially dissociate disulfide bonds followed by high-energy collisional dissociation (HCD) to determine

36 strategy, encompassing a combination of HCD (high-energy collisional dissociation) multistage mass sp

37 life is dependent on lithogenically sourced high-energy compounds to sustain productivity.

38 ing group as part of the Michael acceptor, a high energy concerted SN2' reaction occurs.

39 of bound ligands SUMO1 transiently samples a high energy conformation, which might be involved in lig

40 on and of 2-oxoglutarate in an unprecedented high-energy conformation that favors ethylene, relative

41 ting the enzyme adenylate kinase in a closed high-energy conformation that is on-pathway for catalysi

42 aching processes which apply toxic acids and high energy-consuming annealing, an interconnected silic

43 Current dogma suggests that high-energy-consuming photoreceptors depend on glucose.

44 While the current methods demand high energy consumptions in concentrating the omega-3, m

45 between two graphene electrodes, to achieve high energy conversion efficiency in the temperature ran

46 levels in the visual cortex during times of high energy demand (photic stimulation).

47 ility to replenish brain ATP during times of high energy demand in BD.

48 preserving the intricate balance between the high energy demand of active neurons and the supply of o

49 II activity is important under conditions of high energy demand, and that specific cell types are uni

50 rated from adenylate kinase during states of high energy demand, the ornithine cycle enzyme argininos

51 Here, we report that COX7AR is expressed in high energy-demanding tissues, such as brain, heart, liv

52 rce-intensive subsector of health care, with high energy demands, consumable throughput, and waste vo

53 nd RPE because photoreceptor cells have very high energy demands, largely satisfied by oxidative meta

54 energy will be better suited to satisfy the high-energy demands of growing urban areas.

55 power sources because of their potential for high energy densities (>200 MWh/kg) and long duration co

56 nide, Nd in this work) can potentially allow high energy densities (100-150 J cm(-3)) and efficiencie

57 redox at high potentials, thereby promising high energy densities for lithium-ion batteries.

58 eous Li-ion/sulfur full cell delivers record-high energy densities up to 200 Wh/(kg of total electrod

59 Enjoying great safety, high power, and high energy densities, all-solid-state batteries play a

60 strophic optical damage (COD) due to locally high energy densities, heliotropic COD growth, solid-liq

61 charge-discharge efficiencies and delivering high energy densities, i.e., 1.2 J cm(-3) , even at a te

62 requires cost-effective battery systems with high energy densities.

63 extremely high specific power densities and high energy densities.

64 ric films of Ba(Zr0.2,Ti0.8)O3 which display high-energy densities (up to 166 J cm(-3)) and efficienc

65 Developing electrode materials with high-energy densities is important for the development o

66 S) battery is of great interest owing to its high energy density (1340 Wh kg(-1) ) and low cost.

67 This offers advantages for high energy density and alleviation of cathode side reac

68 ve units in macrocycles are key to achieving high energy density and long cycle-life electrodes for o

69 derable attention because of their potential high energy density and low cost.

70 ouple is of particular interest owing to its high energy density and low cost.

71 Due to their high energy density and low material cost, lithium-sulfu

72 ate a unique Li-ion/sulfur chemistry of both high energy density and safety.

73 Bendable energy-storage systems with high energy density are demanded for conformal electroni

74 te in particular has the potential to enable high energy density as it can deliver excess capacity be

75 e challenge to achieve both the demands of a high energy density as well as a high power density on t

76 ts in dielectric nanocomposite materials for high energy density capacitor applications.

77 oute to prepare and tailor the properties of high energy density capacitor nanocomposites.

78 There is a growing need for high energy density capacitors in modern electric power

79 creasing demand of emerging technologies for high energy density electrochemical storage has led many

80 favorable attributes including low cost and high energy density for grid energy storage.

81 attractive anode for the next generation of high energy density lithium-ion batteries due to its hig

82 tional design of conductive carbon hosts for high energy density lithium-sulfur batteries requires an

83 ultishelled mesoporous carbon sphere shows a high energy density of 52.6 Wh kg(-1) at a power density

84 To exploit the high energy density of the lithium (Li) metal battery, i

85 renewable lignocellulosic biomass, contains high energy density oligomers in the water-insoluble fra

86 ge systems (ESSs) because they can produce a high energy density or a high power density, but it is a

87 e synthesis of the cubic gauche allotrope of high energy density polymeric nitrogen under near-ambien

88 ers has shown great potential in achieving a high energy density since they can optimize the energy d

89 le, and wearable energy-storage devices with high energy density that can be integrated into textiles

90 that HyLIC, which is capable of achieving a high energy density, a long cycle life and an excellent

91 ased lithium-ion batteries have low cost and high energy density, but their capacity fades rapidly du

92 al that at low current, the HyLIC exhibits a high energy density, while at high current, it demonstra

93 achieve good initial cycling stability with high energy density.

94 large-scale energy applications due to their high energy density.

95 potentially enable Li-S batteries to achieve high energy density.

96 iate temperature of 190 degrees C with ultra-high energy density.

97 toward high safety, high power density, and high energy density.

98 stry, as well as the detonation chemistry of high-energy density materials.

99 hieve morphologically optimal structures for high-energy density materials.

100 ium rechargeable batteries potentially offer high-energy density, safety, and low cost due to the abi

101 ium rechargeable batteries potentially offer high-energy density, safety, and low cost.

102 n are promising as environmentally-friendly, high energy-density materials, but are inherently unstab

103 e implementation of dielectric materials for high-energy-density applications requires the comprehens

104 e material for next-generation lithium-based high-energy-density batteries.

105 for future lithium anode materials design in high-energy-density batteries.

106 development of in situ surface protection on high-energy-density cathode materials in lithium-based b

107 trolyte interactions prevent the use of many high-energy-density cathode materials in practical lithi

108 redox sets a new direction for the design of high-energy-density cathode materials.

109 In an effort to develop high-energy-density cathodes for sodium-ion batteries (S

110 r nanocomposites is crucial to the design of high-energy-density dielectric materials with reliable p

111 t and broaden the possibilities in designing high-energy-density electrodes for the next generation o

112 ch further facilitates future application of high-energy-density Li metal batteries.

113 phosis is essential for realizing stable and high-energy-density Li-S batteries.

114 um is a promising anode candidate for future high-energy-density lithium batteries.

115 The widespread implementation of high-energy-density lithium metal batteries has long bee

116 ions through conversion chemistry to enable high-energy-density lithium-ion batteries.

117 nets and because of the hopes of discovering high-energy-density materials.

118 This is particularly true for laser-produced high-energy-density matter, which often exhibits steep g

119 e the numerous proposed approaches, creating high-energy-density pair plasmas in laboratories is stil

120 material tantalum-an important material for high-energy-density physics owing to its high shock impe

121 en regarded as the future anode material for high-energy-density rechargeable batteries due to its fa

122 research directions in nonlinear optics and high-energy-density science, compact plasma-based accele

123 lithium-sulfur (Li-S) battery is a promising high-energy-density storage system.

124 i velocity, the Fermi surface curvature, and high-energy details.

125 of the wind simultaneously in both low- and high-energy detectors, suggesting a single ionized outfl

126 enopausal phase, exposure to over nutrition, high-energy diet and oestrogen deficiency, are considere

127 the adipocyte number when challenged with a high-energy diet.

128 Previous studies have linked cell damage to high energy dissipation rates (EDR) and have predicted t

129 sine methylation signature ions generated in high-energy-dissociation (HCD) tandem mass spectrometry.

130 Here we report observations of distinct, high-energy, downward, discrete electron acceleration in

131 high E eff value corresponds to the onset of high energy dynamic instabilities in this driven vortex

132 High gradients of energy gain and high energy efficiency are necessary parameters for comp

133 tion (the removal of salts from seawater) at high energy efficiency will likely become a vital source

134 accelerating fields over long distances with high energy efficiency.

135 iated with an O2-evolving anodic reaction in high-energy-efficiency cells are not yet available.

136 lly and through numerical simulations that a high-energy electron beam is produced simultaneously wit

137 rystals investigated with in situ reflection high-energy electron diffraction (RHEED) and ex situ ato

138 to the single-cycle nature of the field, the high-energy electron emission is predicted to be confine

139 By employing high-energy electron-loss signals (of several hundred eV

140 assessment of biological sources of NADPH's high energy electrons.

141 various situations in astrophysics in which high-energy electrons and intense circularly polarized l

142 A Varian Clinac iX is used to simulate the high-energy electrons emitted from (90)Sr, and a high ef

143 By scattering high-energy electrons off a proton we are able to resolv

144 inately fast neutrons generated by impinging high-energy electrons onto a tantalum convertor are mode

145 ir ability to withstand physical stresses in high energy environments relies on their skeletal struct

146 ere, we present a molecular description of a high-energy enzyme state in a conformational selection p

147 scaler with metal tip is less efficient than high-energy Er:YAG irradiation to remove the plaque and

148 Here we investigate the effect of high energy events on a range of starting mixtures repre

149 ned tens of nanometres away from the sample: high-energy excitations are suppressed, while vibrationa

150 However, electron beams typically create high-energy excitations that severely accelerate sample

151 t lifetime results from annihilation between high-energy excited states, producing energetically hot

152 cases, these reactions proceed directly from high-energy excited states.

153 tion metal dichalcogenides region supporting high-energy exciton resonance to a different transition

154 hirped pulse amplifier (OPCPA) for achieving high-energy few-cycle mid-infrared pulses.

155 py to the generation and self-compression of high-energy few-cycle pulses.

156 tivation of O2 due to the presence of both a high-energy, filled O2(-) pi* orbital and an empty low-l

157 Furthermore, high energy flux appeared to prevent fat gain in part be

158 s no sheet bending, and random patterns with high-energy folding, in which the sheet bends as much as

159 ered with a decrease in subjective appeal of high-energy food pictures and reduced energy intake duri

160 pecifically by a lowering of the response to high-energy food.

161 as a fragmentation technique offers prompt, high-energy fragmentation, which can potentially lead to

162 izing this otherwise squandered high-volume, high-energy gas.

163 star often show x-ray emission extending to high energies (>10 kilo--electron volts), which is ascri

164 This type of high-energy harvesting dyad is expected to open new rese

165 with a workflow that included initial fast, high-energy HCD (Orbitrap, FT) scans, which produced int

166 y disk equilibration model, but supports the high-energy, high-angular-momentum giant impact model fo

167 xing during the giant impact and therefore a high-energy, high-angular-momentum impact.

168 ted included donor molecules with relatively high energy HOMO, molecules with high HOMO-LUMO gaps and

169 f UV-active photocatalysts for the requisite high-energy hydrogen atom abstraction event.

170 ally produces nanosized particles because of high-energy impacts.

171 ials in ammonia or hydrocarbon gas under the high-energy impacts; in other milling atmospheres such a

172 It is known that high-energy implosion due to cavitation collapse is resp

173 52), diabetes (OR, 1.40; 95% CI, 1.21-1.61), high-energy injury (OR, 1.38; 95% CI, 1.27-1.49), antico

174 lines' counterpart, which typically requires high energy input such as photo or thermal activation to

175 organic solvent, a secondary emulsifier, or high-energy input.

176 his study suggests that in children with MS, high energy intake from fat, especially saturated fat, m

177 no study has evaluated the relation between high energy intakes at lunch compared with at dinner on

178 d to act as a 2D surfactant and is spread at high-energy interfaces.

179 een both components promote the formation of high-energy interfacial Mn-O-Co species and high oxidati

180 Engineering high-energy interfacial structures for high-performance

181 The use of N-glycan oxazolines, high energy intermediates on the hydrolytic pathway, as

182 ort that vinyl cations are not exceptionally high energy intermediates, and that high intrinsic barri

183 lectrophiles to the intermittently generated high energy intermediates.

184 cally favored alkene epoxidation by trapping high-energy intermediates and catalyzing an oxo transfer

185 or both photochemical excitation to generate high-energy intermediates and heat to drive important th

186 is light-dependent and probably proceeds via high-energy intermediates but is independent of the Glu-

187 he stable ground-state structures and in the high-energy intermediates, was accomplished using the an

188 e transformations involving deprotonation of high-energy intermediates.

189 localization effects in crystalline GeTe via high-energy ion irradiation, we show tremendous improvem

190 rated using heat, pH, high salt mediums, and high energy ionising radiation.

191 ed to the tendril size, so the nature of the high energy irradiation must enable faster growth with l

192 The high-energy landscape is dominated by an energy ladder o

193 Photoexcitation of nitro groups by a high-energy laser is not required; the energy can be del

194 ement fusion depends upon the interaction of high-energy lasers and hydrogen isotopes, contained with

195 it-eating bats (Uroderma bilobatum) manage a high-energy lifestyle fueled primarily by fig juice.

196 High-energy lithium-metal batteries are among the most p

197 e of artificial kagome dipolar spin ices and high-energy, low-entropy 'monopole-chain' states that ex

198 [TAGs], sterylesters, etc.) are reserves of high-energy metabolites and other constituents for futur

199 num alloy powder was extensively deformed by high energy milling, so to refine the bcc iron domain si

200 table reaction intermediates prepared with a high-energy molecular beam in the STM can be readily ext

201 ability to eventually produce high-quality, high energy multi-particle bunches has remained a subjec

202 ochondrial trafficking is crucial because of high energy needs and calcium ion buffering along axons

203 ion have low nitrogen usage efficiencies and high energy needs.

204 l atoms and demonstrate the feasibility of a high energy neutral atom accelerator that could signific

205 sage generation of high-flux, low-emittance, high energy neutral atom beams in length scales of less

206 t equilibration and preserve highly ordered, high energy non-equilibrium states.

207 but the challenging task of describing their high-energy nonlinear properties has long remained elusi

208 is and those fuelled indirectly by living on high energy nutrition represent preserved non-equilibriu

209 ers included donor molecules with relatively high energy occupied orbitals and acceptors with low ene

210 s of HS(EG)nCH3 using interactions among the high-energy, occupied orbitals associated with the lone-

211 ydrocarbons (PHs) is challenging because the high energy of their highest occupied molecular orbital

212 by shifting low-energy moisture reactions to high-energy ones due to As.

213 d-occluded and a new nucleotide-bound state, high-energy outward-occluded intermediate state, with a

214 king on nearest-neighbour bonds describe the high-energy part of the excitation spectrum in YbMgGaO4,

215 aromatic subunits, which can only absorb the high-energy part of the visible spectrum.

216 High energy particle radiations induce severe microstruc

217 y parameters for compact, cost-efficient and high-energy particle colliders.

218 icking the massless relativistic dynamics of high-energy particle physics, and they can twist the qua

219 High-energy phase-stable sub-cycle mid-infrared pulses c

220 METHODS AND Resting SM high-energy phosphate concentrations and ATP flux rates

221 e mechanistic in vivo relationships among SM high-energy phosphate concentrations, mitochondrial func

222 gnificantly faster rates of exercise-induced high-energy phosphate decline than did HFrEF patients wi

223 exhibited severe EI, the most rapid rates of high-energy phosphate depletion during exercise, and imp

224 This finding suggests alterations in high-energy phosphate metabolism and regulation of oxida

225 kinase expression falls, possibly impairing high-energy phosphate transfer from the mitochondria to

226 early, rapid exercise-induced declines in SM high-energy phosphates and reduced oxidative capacity co

227 cation of bioenergetic molecules, containing high-energy phosphates, over the whole brain as well as

228 linear chains of phosphate groups linked by high-energy phosphoanhydride bonds.

229 We discuss how the chemical features of the high-energy phosphorus-nitrogen bond shape the dominant

230 High energy photoelectrons are shown to be a powerful to

231 results also show that screening influences high-energy photoelectrons ( approximately 20 eV) signif

232 As a result, high-energy photoelectrons can serve as a direct probe o

233 nt detection of the reaction fragments after high energy photofragmentation.

234 hotonic properties can be manipulated by the high energy photons.

235 res able to interact with the aforementioned high energy photons.

236 imitations in ultraviolet absorption because high-energy photons are absorbed at the surface of the s

237 a well-known radiation process that produces high-energy photons both in nature and in the laboratory

238 ) enhance the damaging absorbance effects of high-energy photons in radiation therapy by increasing t

239 ging of the 3D fields, which is difficult in high-energy physics and cosmology.

240 future generations of both light sources and high-energy physics experiments.

241 r realizations of many important concepts in high-energy physics, leading to wide-ranging protected p

242 the dynamical mass generation of nucleons in high-energy physics.

243 ature batteries with well-controlled safety, high energy/power density, and operation over a wide tem

244 The nanocomposite exhibits a record-high energy product (28 MGOe) for this class of bulk mat

245 Their high-energy, promiscuous reactivity profiles have hamper

246 tes are novel signaling molecules possessing high-energy pyrophosphate bonds and involved in a number

247 far-from-equilibrium conditions produced by high-energy radiation) consists of a local orthorhombic

248 'tissue-independent' activation of TAL2 upon high-energy radiation, and thus qualifies TAL2 as a pote

249 Pericyclic reactions bypass high-energy reactive intermediates by synchronizing bond

250 les, generating these intermediates requires high-energy reagents (such as highly reducing metals or

251 promising high-capacity cathode material for high-energy rechargeable lithium batteries.

252 the transfer of the spectral weight from the high-energy region to the gap region with electron dopin

253 revealing the formation of quite remarkable high energy remanence states and a change in the dynamic

254 awbacks including hazardous byproducts and a high-energy requirement for regeneration; therefore, res

255 on the proximal tubule that by virtue of the high energy requirements and reliance on aerobic metabol

256 er repeated transitions, possibly due to the high energy requirements of regulation.

257 ntalization, length of axonal processes, and high-energy requirements (reviewed in [3]).

258 It is demonstrated that the U M4 high energy resolution X-ray absorption near edge struct

259 ruction have enabled one to use the CCD as a high energy resolution X-ray detector.

260 Spin resonance provides the high-energy resolution needed to determine biological an

261 Kalpha high-energy-resolution fluorescence detected X-ray absor

262 Inositol pyrophosphates are high energy signaling molecules involved in cellular pro

263 High-energy spectral features allow rapid identification

264 provides a considerable opportunity to probe high-energy spin excitations.

265 In addition, we found that the trapped high-energy state displayed improved ligand binding affi

266 demonstrating that substrate binding to the high-energy state is not occluded by steric hindrance.

267 odel, a protein samples a scarcely populated high-energy state that resembles a target-bound conforma

268 ic interconversion between ground states and high-energy states can constitute the rate-limiting step

269 In enzymatic catalysis, such high-energy states have been identified as crucial entit

270 ding energy to stabilize their substrates in high-energy states that are otherwise inaccessible at am

271 the electrode materials, toward devices with high energy-storage performance.

272 Existing dielectrics for high-energy-storage capacitors and potential new capacit

273 The optimization of high-energy-storage dielectrics will have far-reaching i

274 Here we report a high-energy sub-cycle pulse synthesiser based on a mid-i

275 dislocations and may provide a way to create high-energy surfaces for catalysis that are kinetically

276 el are investigated in situ with high-speed, high-energy synchrotron X-ray radiography.

277 zz grain boundaries tended to be high angle; high energy tendril grain boundaries were not observed.

278 gy tendrils are finer ( 22 nm diameter) than high-energy tendrils ( 176 nm diameter), and low-energy

279 The high-energy tendrils consisted of very large (>100 nm) g

280 energy tendrils have a smoother surface than high-energy tendrils.

281 high uncertainty, or a low duty cycle and a high energy threshold.

282 , from low wave and tidal energy lagoons, to high energy tidal reef flats, but remain dependent upon

283 be a safe alternative to the currently used high-energy tissue ablation technology, which uses X-ray

284 ed the motion of photoexcited electrons from high-energy to low-energy states in a type-II 2D InSe/Ga

285 and the long lifetime is not cut short upon high energy-transfer efficiency.

286 ergoes ultrafast iSF in solution, generating high-energy triplets on a sub-picosecond time scale.

287 The produced protons are characterized by high-energies (with a broad spectrum), are emitted in a

288 ten sodium carbonate (Na2CO3) which combines high energy X-ray diffraction, containerless techniques

289 Using time-resolved monochromatic high energy X-ray diffraction, we present an in situ stu

290 In situ high energy X-ray pair distribution function (PDF) measu

291 rough a combination of time-resolved in situ high-energy X-ray diffraction and absorption spectroscop

292 Through high-energy x-ray diffraction and atomic pair density fu

293 c and noninonic interactions were studied by High-Energy X-ray Diffraction and Pair Distribution Func

294 Here, using synchrotron-based high-energy x-ray diffraction and time-domain Mossbauer

295 structure of SiO2 glass up to 172 GPa using high-energy X-ray diffraction.

296 Operando high-energy X-ray reflectivity measurements demonstrate

297 ated by combining density functional theory, high-energy X-ray scattering (HEXS), and extended X-ray

298 X-ray absorption spectroscopy and high-energy X-ray scattering demonstrate a correlation b

299 High-energy X-rays (HEX-rays) with photon energies on or

300 The high-energy X-rays of the synchrotron permit the recordi