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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

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