ライフサイエンスコーパス: high energy

1 s affording favorable safety, long life, and high energy.

2 nabled rechargeable metallic Li battery with high energy (178 Wh kg(-1) ) and power (2877 W kg(-1) )

3 However, the origins of such high-energy (above one gigaelectronvolt) photons and the

4 s of LCEs and can inspire the development of high-energy-absorbing device applications.

5 cture, accomplishing both high stiffness and high energy absorption.

6 panchromatic absorptivity via redistributing high-energy absorptive oscillator strength throughout th

7 presented by disarticulated individuals from high energy accretion deposits in Laurasia, thus greatly

8 zyme efficiency by making transitions to the high energy active conformation more probable, rather th

9 principle opens a new opportunity to develop high-energy all-solid-state Li metal batteries.

10 The emitted high-energy alpha particles induce DNA double-strand bre

11 However, the deposition of high-energy alpha-emitters to tumor markers adjacent to

12 Such high energy and complex manufacturing processes make it

13 ectrons, therefore chamber response to these high energy and high dose-per-pulse beams must be well u

14 , high Coulombic efficiency up to 99.9%, and high energy and power density of ~ 420 Wh kg(-1) and ~ 1

15 endrites impedes the service of Li anodes in high energy and safety batteries.

16 applications and fundamental bridge between high-energy and condensed-matter physics.

17 ining DAPH-TFP COF were able to deliver both high-energy and high-power densities, validating the pro

18 pens new venues for the development of novel high-energy and high-stability cathodes.

19 renders it a promising cathode material for high-energy and long-cycle-life LSBs.

20 ective platforms that simultaneously support high-energy and safe electrochemical energy storage.

21 led global conformational changes, including high-energy backbone rearrangements, that cooperatively

22 linear configuration of CO(2) and reduce the high energy barrier by stabilizing the reaction intermed

23 -plane chalcogen atoms but restricted by the high energy barrier to break the in-plane TM-X (X = chal

24 insertion needs to overcome a prohibitively high energy barrier.

25 cts is a challenging reaction because of the high energy barriers for CO(2) activation and C-C coupli

26 YfdC-alpha, were found to be responsible for high energy barriers for the anions to enter EcYfdC.

27 rod-like counterparts (which exhibited very high energy barriers of unfolding and refolding).

28 iable multi-electron transfer electrodes for high energy batteries.

29 The need for high-energy batteries has driven the development of bind

30 r active study for their potential to enable high-energy batteries.

31 d rational design of stable electrolytes for high-energy batteries.

32 ding new perspectives for the development of high-energy battery systems.

33 plans of intensity-modulated proton therapy, high-energy beams are usually assigned larger weights th

34 w-linear-energy-transfer (LET) properties of high-energy beta-particles.

35 ronous global expansion of alluvial fans and high-energy braided streams is a response to abrupt clim

36 lectrochemical oxidation is used to liberate high-energy carbocations from simple carboxylic acids.

37 , also known as inositol pyrophosphates, are high-energy cellular signaling codes involved in nutrien

38 storing metabolic homeostasis in response to high energy charge.

39 henylamine-tetracyanobutadiene (TPA-TCBD), a high-energy charge-transfer species, are linked to a nea

40 h proton transfer (PT) in order to avoid the high-energy, charged intermediates resulting from the st

41 wo visible-light photons to affect a single, high-energy chemical transformation.

42 on yield and the improved focusability using high-energy cluster beams, imaging in the 1 mum spatial

43 ode material development for next-generation high-energy, cobalt-free Li-ion batteries.

44 However, current approaches for predicting high-energy collisional dissociation (HCD) spectra are l

45 des the electron anisotropy into a low and a high energy components which excite the upper-band and l

46 ing dynamics, including a transient burst of high-energy configurations during association, biphasic

47 Here we show that in many of the high energy consuming states, such as California and Tex

48 ver, conventional synthesis of SACs involves high energy consumption at high temperature, complicated

49 However, high energy consumption of vapor generation fundamentall

50 rocesses suffer from poor reproducibility or high energy consumption, respectively.

51 n effects, resulting in large footprints and high energy consumption.

52 ter treatment and seawater desalination with high energy conversion and utilization efficiency.

53 ewable electricity as an electron source and high energy conversion efficiency.

54 routinely conduct intraspecific combat where high energy cranial impacts are experienced.

55 sful in demonstrating efficient CS upon both high-energy CT and low-energy near-IR excitations, signi

56 sue vulnerability, the number of intolerable high-energy cycles applied in unit time (mechanical powe

57 tabolic phenotypes to meet the challenges of high energy demand and macromolecular synthesis.

58 ondrial function is required in tissues with high energy demand such as the heart, and mitochondrial

59 ability at the neuromuscular junction during high energy demand.

60 tochondrial clusters are found at regions of high-energy demand, allowing cells to meet local metabol

61 e neuron allows for clustering at regions of high-energy demand.

62 beta-oxidation, the process required to fuel high energy-demanding pathways (e.g., gluconeogenesis an

63 Eukaryotic ribosomal biogenesis is a high-energy-demanding and complex process that requires

64 e pathway by which photoreceptors meet their high energy demands is not fully understood.

65 However, due to their high energy demands, cardiac cells are disproportionatel

66 uency activity of PV(+) interneurons imposes high-energy demands on their metabolism that must be sup

67 Safety risks associated with modern high energy-dense rechargeable cells highlight the need

68 attracted special attention because of their high energy densities and efficiencies.

69 state lithium-sulfur batteries (SSLSBs) with high energy densities and high safety have been consider

70 ed on the pseudocapacitive mechanism combine high energy densities with high power densities and rate

71 Sodium metal batteries have potentially high energy densities, but severe sodium-dendrite growth

72 ies are a proposed route to safely achieving high energy densities, yet this architecture faces chall

73 ions due to extended period of operation and high energy densities.

74 xtreme high-density plasma mixtures at super-high energy densities.

75 th to develop inherently safe batteries with high energy density (>1000 Wh L(-1)).

76 ingle micro-supercapacitor exhibits an ultra-high energy density (0.23 Wh cm(-3)), an ultra-small tim

77 energy storage applications because of their high energy density and low-cost advantages.

78 e attracted attention owing to the potential high energy density and safety; however, little success

79 have attracted much attention owing to their high energy density and use of greenhouse CO(2) waste as

80 ytes recently spurred resurgent interest for high energy density aqueous lithium-ion batteries.

81 ttery cycling at a fast-charging rate with a high energy density beyond those of a commercial standar

82 In the search for high energy density cathodes for next-generation lithium

83 1.5)O(4) (LNMO) is a promising candidate for high energy density cathodes in lithium-ion batteries (L

84 Rechargeable sodium metal batteries with high energy density could be important to a wide range o

85 ive route towards lithium-ion batteries with high energy density for a broad range of applications.

86 Advanced battery systems with high energy density have attracted enormous research ent

87 The experiment was performed at the high energy density instrument at the European XFEL GmbH

88 ditions currently only accessible at nuclear high energy density laser facilities.

89 The highly reversible Zn anode brings a high energy density of 210 Wh kg(-1) (of cathode and ano

90 acity ratio of Zn:MnO(2) at 2:1 to deliver a high energy density of 212 Wh/kg (based on both cathode

91 In particular, it achieves an extremely high energy density of 27.5 W h kg(-1), which is among t

92 cific capacity of 467 mAh g(-1) and a record high energy density of 481 Wh kg(-1).

93 elivering an average voltage of 1.74 V and a high energy density of 71 Wh kg(-1) with a capacity rete

94 More importantly, a high energy density of 779 Wh kg(-1) and power density o

95 n electrolyte conditions, corresponding to a high energy density of 974 Wh.kg(-1) The superior electr

96 Despite the exceptionally high energy density of lithium metal anodes, the practic

97 confirm magnetization-related effects in the high energy density regime.

98 The high energy density results from the conversion mechanis

99 ch may guide the design and manufacturing of high energy density solid-state batteries.

100 Thermodynamic calculations allow selecting high energy density systems, but experimental findings i

101 Rechargeable lithium-ion batteries with high energy density that can be safely charged and disch

102 -solid-state asymmetric supercapacitors show high energy density up to 13.1 mWh cm(-3) via pseudocapa

103 ectronics due to its long discharge plateau, high energy density, and environmental friendliness.

104 next generation energy storage devices with high energy density, but face challenges in achieving hi

105 and mechanical robustness, which can support high energy density, fast charging and discharging capab

106 gy density, but face challenges in achieving high energy density, high safety, and long cycle life.

107 Due to their exceptional high energy density, lithium-ion batteries are of centra

108 h requires advanced micro power sources with high energy density, long lifetime and good biocompatibi

109 rial to assemble rechargeable batteries with high energy density.

110 nsive attention due to their high safety and high energy density.

111 es on realizing safe Na metal batteries with high energy density.

112 that can provide simultaneous high power and high energy density.

113 rage system that is both safe and features a high energy density.

114 ted extensive research interest due to their high energy density.

115 o their advantages in safety and potentially high energy density.

116 rge-scale energy-storage due to low cost and high energy density.

117 es for reducing ("stabilizing") RT growth in high-energy density (HED) settings on the National Ignit

118 ms, enabled by the design and development of high-energy density electrode materials.

119 um is the most attractive anode material for high-energy density rechargeable batteries, but its cycl

120 cal energy and therefore offers a system for high-energy density storage and for chemical up-conversi

121 tteries with desirable advantages, including high-energy density, wide temperature tolerance, and few

122 thium metal is necessary for the adoption of high energy-density rechargeable lithium metal batteries

123 materials are crucial for the development of high-energy-density all-solid-state batteries (ASSB) usi

124 aterials have been considered as potentially high-energy-density alternatives to commercially dominan

125 t feature microscale dimensions and a unique high-energy-density and a nonequilibrium reactive enviro

126 Fabrication of high-energy-density and high-power-density packaged long

127 the surest and best studied paths to enable high-energy-density batteries and high-efficiency solar

128 High-energy-density batteries with a LiCoO(2) (LCO) cath

129 rate capability of lithium metal anodes for high-energy-density batteries, one fundamental challenge

130 dox with cationic redox chemistry to achieve high-energy-density batteries.

131 While lithium metal represents the ultimate high-energy-density battery anode material, its use is l

132 ium batteries are a potentially sustainable, high-energy-density battery technology beyond Li ion bat

133 ducts, however, the selectivity to desirable high-energy-density C(3) products remains relatively low

134 ckel (>90 %) layered oxides and their use as high-energy-density cathodes for lithium-ion batteries.

135 es, including the inhomogeneous reactions of high-energy-density cathodes, the development of safe an

136 batteries constitute a safe and sustainable high-energy-density electrochemical energy-storage solut

137 The electroreduction of C(1) feedgas to high-energy-density fuels provides an attractive avenue

138 utions toward the goals of a low-cost and/or high-energy-density future, are discussed in detail for

139 free and sustainable fuel, ammonia serves as high-energy-density hydrogen-storage material.

140 OR, which broadens the horizon for designing high-energy-density Li-rich cathode oxides with stable l

141 sulfide and are key to full exertion of the high-energy-density Li-S system.

142 ical applications of lithium metal anodes in high-energy-density lithium metal batteries have been hi

143 gen compounds of interest for development of high-energy-density materials, including explosives for

144 Electrochemical reduction of CO(2) to high-energy-density oxygenates and hydrocarbons beyond C

145 ode materials to control oxygen activity for high-energy-density rechargeable batteries.

146 and the high-voltage cathode for long-life, high-energy-density rechargeable Li metal batteries (LMB

147 al is a promising candidate as the anode for high-energy-density solid-state batteries.

148 However, the high-energy-density states that exist in white dwarfs ar

149 iolet photodissociation (UVPD), an alternate high-energy deposition method that offers extensive frag

150 roduction from decay of (9)Li, formed by the high-energy deuteron bombardment of the beryllium conver

151 It has recently been demonstrated that high-energy diagnostic transthoracic ultrasound and intr

152 cro-computed tomography (muCT) and far-field high-energy diffraction microscopy (ff-HEDM), are now ca

153 Hurricanes are recurring high-energy disturbances in coastal regions that change

154 by a disulfide bond that is constrained in a high-energy eclipsed conformation.

155 y with the combined advantages of low costs, high energy efficiencies, abundant elements, and good en

156 g the last two decades due to its promise of high energy efficiency combined with non-volatility.

157 felt-CoS(2)/CoS heterojunction can deliver a high energy efficiency of 84.5% at a current density of

158 tentials of 80 and 270 mV, respectively, and high energy efficiency of 90.2% in the first cycle is de

159 hieves a low charge potential below 3.4 V, a high energy efficiency of ~80%, and can be reversibly di

160 Li-CO(2) battery with low overpotential and high energy efficiency, by employing ultrafine Mo(2) C n

161 hat can operate in extreme temperatures with high energy efficiency.

162 mentally benign, highly compact, and of very high energy efficiency.

163 Here, we use a picosecond pulse of a high energy electron beam to generate electrons in liqui

164 High energy electron beams consisting of a long train of

165 structural transition probed via Reflection High Energy Electron Diffraction (RHEED) for the first t

166 Here we use high-energy electron scattering measurements that isolat

167 Moreover, Very High Energy Electrons (VHEEs) provide more favourable do

168 Radiotherapy with very high energy electrons has been investigated for a couple

169 They play an essential role in accelerating high-energy electrons forming the hazardous radiation be

170 Unfortunately, the high-energy electrons that carry this important informat

171 pton up-scattering of synchrotron photons by high-energy electrons.

172 Here we report observations of very-high-energy emission in the bright GRB 180720B deep in t

173 acked small sediment particles compared with high-energy environments.

174 nd were characterized by U-shapes suggesting high energy expenditure.

175 The high energy footprint of commodity gas purification and

176 er multiplication (CM) is a process in which high-energy free carriers relax by generation of additio

177 nificantly older compared to patients in the high-energy group (72.2 vs. 53.8 years; p = 0.030).

178 ors were able to assuage the requirement for high energy (> 40 keV) large-area X-ray imaging applicat

179 shwater surface layer (the neuston) occupy a high energy habitat that is threatened by human activiti

180 It offers the high-energy harvesting functionality of micro-PMFCs with

181 air without reliance on bulky equipment and high energy has been a substantial challenge and has att

182 High-energy heavy ions can deliver high radiation doses

183 tive approach to sodium metal batteries with high energy/high power density, long cycle life and high

184 y lead survival for the 4 most commonly used high-energy ICD leads.

185 os between the interband-transition peaks at high energies in the experimental and single-particle-ca

186 s iodine buttressing approach for generating high-energy in-plane HOMOs is anticipated to be highly g

187 investigate a simple strategy for achieving high-energy in-plane orbitals for aromatics simply by po

188 e pair orbitals on the iodines mix to give a high-energy in-plane sigma-antibonding orbital as the hi

189 obesity in orthopaedic trauma patients with high-energy injuries and to investigate their impact on

190 esity among orthopaedic trauma patients with high-energy injuries.

191 model in which SF2312 acts as an analog of a high energy intermediate formed during the catalytic pro

192 The X-ray crystal structure of FLuc with a high-energy intermediate analogue, 5'-O-[N-(dehydroinfra

193 These mediated pathways introduce a high-energy intermediate, cap the driving force for subs

194 the participation of a plethora of activated high energy intermediates such as the alpha- and beta-gl

195 However, these high-energy intermediates can often require directing gr

196 We show that high-energy ion bombardment improves the energy storage

197 Thus, a deeper understanding of subsequent high energy ions generated from various mechanisms and t

198 rein, for the first time, we utilize in situ high-energy Kr ion irradiation with transmission electro

199 no meaningful differences in the rate of ICD high-energy lead survival for the 4 most commonly used h

200 ety end point of lead failure for any of the high energy leads studied.

201 5 years ranged from 97.7% to 98.9% for the 4 high-energy leads of interest.

202 ctical implementation of Li metal anodes for high-energy Li-ion batteries.

203 High-energy Li-rich layered cathode materials (~900 Wh k

204 ) (NMC811)/graphite cells, which are typical high-energy LIBs.

205 e as a consequence of the potential of these high energy light sources to damage living cells.

206 Lipids in HH tissues were comprised of high energy lipid classes, while HD and DD tissues conta

207 ytes remain challenges to the development of high-energy lithium ion batteries containing lithium met

208 hode materials of choice for next-generation high-energy lithium-ion batteries.

209 ursued as a key parameter to build realistic high-energy lithium-sulfur batteries, less attention has

210 tive skins on the surface of Li metal toward high-energy, long-life, and safe Li metal batteries.

211 trated CM, but are not satisfactory owing to high-energy-loss and inherent difficulties with carrier

212 An investigation into the prospects of high energy micro-computed-tomography (Micro-CT) as a no

213 Here we report reproducible generation of high-energy (microjoule level) attosecond waveforms usin

214 High-energy milling (HEM) was used to produce nixtamaliz

215 often requires large amounts of solvent with high-energy mixing, shearing, sonication or electrochemi

216 ectronvolt) photons and the presence of very-high-energy (more than 100 gigaelectronvolts) emission h

217 High-energy nickel (Ni)-rich cathode will play a key rol

218 emale Wistar rats ate chow (controls (C)) or high energy, obesogenic diet to induce MO from weaning t

219 electron-hole pairs is only efficient in the high energy offset blend with fullerene domains.

220 ensity functional theory calculations that a high energy orbital (lO(2p')) at under-coordinated surfa

221 e changes once considered only possible with high energy, our work reveals a potential pathway exempl

222 The intrinsic cycle stability and high-energy output systems that would incur damage under

223 izing radiation in cosmic chemistry includes high-energy particles (e.g., cosmic rays) and high-energ

224 ticles beyond those mimicking the elementary high-energy particles such as Dirac and Weyl fermions ha

225 roach that could be strategically coupled to high-energy PFAS-destructive treatment technologies.

226 gauss, the decay of which powers a range of high-energy phenomena(5).

227 modes and a strong decrease in the number of high-energy phonon modes in comparison to the bulk Sn PD

228 ectroscopy is a noninvasive method to detect high-energy phosphate metabolites, such as ATP.

229 eks after tendon release, when the levels of high-energy phosphates and glycerophospholipids were low

230 ely affect the intracellular availability of high-energy phosphates and ultimately, cellular metaboli

231 e, but did not prevent the level decrease in high-energy phosphates or protein constituents of mitoch

232 chains of orthophosphate residues, linked by high-energy phosphoanhydride bonds.

233 uantum systems, atoms or molecules, absorb a high-energy photon, electrons are emitted with a well-de

234 igh-energy particles (e.g., cosmic rays) and high-energy photons (e.g., extreme-UV).

235 ture is particularly effective at harnessing high-energy photons and is compatible with ionic-dopant-

236 nventional photophysical process that yields high-energy photons from low-energy incident light and o

237 an recombine radiatively, thereby converting high-energy photons to pairs of low-energy photons, whic

238 UVPD energizes ions via absorption of high-energy photons, which allows access to new dissocia

239 omponents in noble liquid detectors used for high energy physics (HEP) experiments and dark matter se

240 ical imaging to security, non-proliferation, high-energy physics and astrophysics.

241 in the diverse areas of physics ranging from high-energy physics, cosmology and astrophysics to biolo

242 ymmetry-a theoretical framework developed in high-energy physics-can be strategically used in optics

243 he molecule-by-molecule lateral growth along high-energy planes.

244 trate (LSCO/STO) is investigated, and also a high-energy plasmon is observed.

245 iform charge system eventually generates the high-energy plasmon.

246 ydrolysis correlates with stabilization of a high-energy, post-ATP hydrolysis state characterized by

247 The centre of the Milky Way hosts several high-energy processes that have strongly affected the in

248 -R155C consumes excess ATP, which can hinder high-energy processes.

249 In mammary tumours, high-energy radiation is associated with induction of fo

250 imited to facilities capable of working with high-energy radioisotopes.

251 Lithium metal is an ideal anode for high-energy rechargeable batteries at low temperature, y

252 High-energy rechargeable lithium (Li) metal batteries (L

253 ds that require stoichiometric quantities of high-energy reductants.

254 tion, different dynamics in both the low and high energy regime, and for developing a wide range of q

255 momentum dependence of the power law in the high-energy region matches the theoretical predictions,

256 The consumption of fuel allows the high-energy replicators to persist at a steady state, mu

257 ge-coupled-device (pnCCD) detector, enabling high energy resolution detection of X-rays differentiate

258 Using U L(3) high energy resolution fluorescence detection (HERFD) X-

259 nteractions can be directly interrogated via high-energy resolution fluorescence detected X-ray absor

260 We have used high energy-resolution neutron scattering to probe nanos

261 sociated Hg-S(3)/S(4) species, as studied by high energy-resolution X-ray absorption near edge struct

262 culate beta-HgS in the DOM, as quantified by high energy-resolution XANES (HR-XANES) spectroscopy, in

263 atomic-scale, spatially resolved images, and high-energy-resolution electron-loss near-edge structure

264 nalyses, including luminescence, U M(4)-edge high-energy resolved fluorescence detection-X-ray absorp

265 design of cation transport requirements for high-energy reversible cathodes in aqueous electrochemic

266 , intact transition epitope mapping-targeted high-energy rupture of extracted epitopes (ITEM-THREE),

267 d by insufficient tissue penetration despite high energy settings.

268 r resulted in wider lesions at both low- and high-energy settings (18.7+/-3.3 versus 12.2+/-1.7 mm, P

269 e posterior and lateral walls using low- and high-energy settings, respectively.

270 y indicates a linear correlation between the high energy shift in NH stretching frequency and the ele

271 disorder is nucleated at low co-ordination, high energy sites of the nanoparticle where cationic vac

272 ube IM-MS (DTIM-MS) platform, which combines high-energy source optics for improved collision induced

273 hat these correlated phases originate from a high-energy state with an unusual sequence of band popul

274 hat hybridization of the emissive state with high-energy states can, in analogy with the intensity bo

275 gy surface that increases the populations of high-energy states prone to aggregation.

276 output systems that would incur damage under high-energy stimuli could particularly benefit from this

277 m wall thickness, ~10 nm crystallinity) show high energy storage capability, hierarchical porous stru

278 are being extensively studied for their very high energy storage capacity. Mn-based disordered rock s

279 n poly(vinylidene fluoride), as required for high energy storage density, is a major challenge.

280 One promising candidate for high-energy storage systems is the nonaqueous redox flow

281 gy is potentially promising for low-cost and high-energy storage systems.

282 eries (RFBs) have great potential to achieve high-energy storage systems.

283 tu/operando time-resolved studies, including high-energy synchrotron X-ray diffraction and diffuse re

284 ernally supplied electrons with sufficiently high energy to drive H(2) production.

285 the absorption of radiation of sufficiently high energy to produce ionization." Ionizing radiation i

286 sation because of their breeding strategy of high energy transfer while fasting, but we anticipate th

287 This approach enables catalysis of high-energy transformations through several opaque barri

288 we provide insight into the structure of the high-energy transition state of Glt(Ph) that limits the

289 h low-energy trauma, patients suffering from high-energy trauma showed significantly lower scores in

290 gy trauma and 11 patients (64.7%) suffered a high-energy trauma.

291 In addition, the model based on high-energy triplet reactivity found that ~30-60% of (3)

292 risation of the luminescence properties of a high-energy, twisted conformation of the previously well

293 approach has the drawback of requiring very high energy, up to the multi-GeV-scale, electron beams,

294 ions however generally require activation by high energy UV or short wavelength blue light, which can

295 "direct" process could also be mediated by a high-energy, virtual charge-transfer state.

296 embryonic; post-hatch; and post-larval, to a high energy water accommodated fraction (HEWAF) of oil,

297 eld X-ray microscopy was spatially linked to high energy X-ray diffraction microscopy and X-ray diffr

298 High energy X-ray phase contrast tomography is tremendou

299 We use high energy X-ray scattering and electro-static levitati

300 using Monte-Carlo simulations constrained by high energy x-ray scattering data.