ライフサイエンスコーパス: ballistic

1 he induction of novel states of matter(1-3), ballistic acceleration of electrons(4-7) and coherent fl

2 h aim to lock on specific photons (coherent, ballistic, acoustically modulated, etc.), this framework

3 coustically levitated drop with simultaneous ballistic addition of reactant.

4 We observe ballistic and anisotropic energy flow through the protei

5 ive equation also reveals previously unknown ballistic and diffusive limits for magnetophoresis where

6 icoseconds, revealing the transition between ballistic and diffusive motion.

7 a homogeneous environment, a combination of ballistic and diffusive steps is considered optimal; in

8 flexural phonons, whose flow is known to be ballistic and distance-independent up to relatively long

9 ters the optimal search strategy toward less ballistic and more Brownian strategies.

10 out-of-focus background can arise from both ballistic and nonballistic excitation.

11 One is ballistic and temperature independent; the other is ther

12 Modern war ballistics and blast injuries inflict devastating extrem

13 lization, tunnelling with exponential decay, ballistic, and diffusion behaviours due to dynamical mul

14 have predicted a related phenomenon known as ballistic anisotropic magnetoresistance (BAMR).

15 ted in a growing number of applications from ballistic armour to nanoelectronics.

16 Using a novel ballistics assay in primary human myotubes, we show it i

17 e probabilities when live prey interact with ballistic attacking predators, and find this diversion e

18 Here we report the observation of ballistic avalanche phenomena in sub-mean free path (MFP

19 suggest that the breakdown originates from a ballistic avalanche phenomenon, where the sub-MFP BP cha

20 The collisionless (or ballistic) behavior of a polypeptide undergoing Brownian

21 ossible orientations (the XX model), we find ballistic behaviour of spin dynamics, whereas for isotro

22 topathological consequences of a penetrating ballistic brain injury is the formation of a permanent c

23 ecular self-assembled monolayer (SAM), and a ballistic carrier emitter.

24 f waves in resonant structures as well as in ballistic, chaotic or in Anderson localized systems.

25 erials typically exhibit either diffusive or ballistic charge transport.

26 among states, is found to support coherent (ballistic) charge transfer.

27 (FIB) micro-machining, defining crystalline ballistic circuits with features as small as 250 nm.

28 The quantum of thermal conductance of ballistic (collisionless) one-dimensional channels is a

29 issues causes exponential attenuation of the ballistic component of a light wave.

30 AMR by observing a stepwise variation in the ballistic conductance of cobalt nanocontacts as the dire

31 typically originates from chiral edge states-ballistic conducting channels that emerge when two-dimen

32 tum transport calculations, we find that the ballistic conduction across this intermetallic interface

33 to their superior specific surface area and ballistic conductivity.

34 he electrical conductance of one-dimensional ballistic conductors has long been experimentally establ

35 carbide are single-channel room-temperature ballistic conductors on a length scale greater than ten

36 ths, from a very weak (tunnel) to a perfect (ballistic) contact.

37 elative humidity (RH) and temperature on the ballistic delivery of particles to the skin.

38 dence of these parameters to support a quasi-ballistic description of our devices.

39 d dynamically controlled disorder to observe ballistic, diffusive, and arrested atomic transport.

40 ation and delamination, photosalient effect (ballistic disintegration and motion), and photoinduced b

41 The ballistic dispersion is universal, yet it has been overl

42 e to the transition from an oscillatory to a ballistic dynamic regimes of motion is presented and sup

43 vements' of chromosomal loci exhibiting near-ballistic dynamics.

44 diameter crater and evidence of a high-angle ballistic ejecta plume still in the process of returning

45 Graphene is a room temperature ballistic electron conductor and also a very good therma

46 We observe a ballistic electron resonance that corresponds to the rou

47 We observe ballistic electron transfer (~30 fs) along a reaction co

48 cy transistors because they demonstrate near-ballistic electron transport and are expected to have hi

49 ctrons, the absence of scattering results in ballistic electron transport and the conductance becomes

50 allic atom-scale junctions (ASJs) exhibiting ballistic electron transport is studied using fluctuatio

51 Moreover, graphene exhibits ballistic electron transport on the submicrometre scale,

52 esence of adsorbates through their impact on ballistic electron transport.

53 These results suggest a novel class of ballistic electronic devices exploiting the unique trans

54 rection through specular reflection of quasi-ballistic electrons at the nanowire surface.

55 ent experiments have shown that collision of ballistic electrons in semiconductors can be used to pro

56 Ballistic electrons in solids can have mean free paths f

57 re comparatively thinner and display greater ballistic emplacement than the central faculae because t

58 device is based on asymmetric scattering of ballistic energy carriers by pyramidal reflectors.

59 Many species execute ballistic escape reactions to avoid imminent danger.

60 hile we understand how stimuli evoke sudden, ballistic escape responses, like fish fast-starts, a pre

61 is 1D system, and suggests that transport is ballistic even at room temperature.

62 edictions corresponded closely with previous ballistic experimental results, adding intraocular detai

63 rings targets of interest into the fovea via ballistic eye movements (saccades).

64 GNIFICANCE STATEMENT Saccades are the rapid, ballistic eye movements that we make approximately three

65 Small ballistic eye movements, so called microsaccades, occur

66 affect the characteristics of saccadic (fast ballistic) eye movements in nonsurgical scenarios.

67 We found no relationship between ballistic eyewear use or severity level of TBI and prese

68 of in-service soft-body armor containing the ballistic fiber poly[(benzo-[1,2-d:5,4-d']-benzoxazole-2

69 We image the transition from flat, ballistic field profiles at low temperatures into parabo

70 e lobula plates of robber flies, typified by ballistic flight behavior, all differ from other taxa in

71 ell as a visualization of its evolution from ballistic flow.

72 s of intrinsically nonlocal transport, as in ballistic flows, which are not easily resolvable via exi

73 Random scattering causes the ballistic focus, which is conventionally used for image

74 n of performance by training rats to execute ballistic forelimb movements for reward.

75 Ballistic fragmentation of proteins induced by a gas clu

76 s a key physical quantity for distinguishing ballistic from hydrodynamic flow.

77 tasks and discriminates intermittent (serial ballistic) from continuous control.

78 esent the subcutaneous tissue, and a type of ballistic gelatine, Perma-Gel(R), as a muscle mimic.

79 ells of green maize leaves when delivered by ballistic gene transfer methods.

80 ved a crossover from the FP to QH regimes in ballistic graphene QPC under a magnetic field with varyi

81 ify different SMF threshold values regarding ballistic hazards - e.g. 3 mT (directive 2004/40/EC, EN

82 ) produced by scanner magnet - the so-called ballistic hazards classified among indirect electromagne

83 Distances from scanner magnet cover, where ballistic hazards might occur are: up to 0.5 m for 0.2-0

84 r to experimentally verify SMF threshold for ballistic hazards near MRI scanners used in Poland.

85 density should be taken as the threshold for ballistic hazards.

86 Decays were also collected during ballistic heating to assess the sensitivity of riboflavi

87 etration and globe deformation measured from ballistic high-speed videos.

88 in a device that operates by spin-dependent ballistic hot-electron filtering through ferromagnetic t

89 her refractoriness and the associated serial ballistic hypothesis generalises to sustained control ta

90 pact histopathology obtained during previous ballistic impact experiments on fresh porcine eyes impac

91 endent of the web using laser vibrometry and ballistic impact providing insights into Nature's design

92 Ballistic impact studies and supercomputer modeling were

93 Five additional eyes not subjected to ballistic impact were also evaluated as controls.

94 ble for applications requiring resistance to ballistic impact.

95 Ballistics in microscopic dimensions are very different,

96 s needed to suppress (NOGO) or initiate (GO) ballistic index finger isometric voluntary contractions.

97 combined particle-tracking microrheology and ballistic injection as the first method able to probe th

98 Ballistic injection lasts <1 min and is followed by over

99 High-throughput ballistic injection nanorheology is a method for the qua

100 particle tracking microrheology coupled with ballistic injection of nanoparticles to measure the loca

101 Cell mechanics are measured by ballistic injection of submicron particles into the cyto

102 A ballistic insertion strategy observed in both environmen

103 Investigations using ballistic intracellular nanorheology reveal that lamin A

104 cts to provide a direct demonstration of the ballistic intrinsic spin Hall effect and to demonstrate

105 Computer-controlled ballistic introduction of reactant droplets into the lev

106 ting gap detection in symmetric, planar, and ballistic Josephson junctions.

107 We now demonstrate functional gears in the ballistic jumping movements of the flightless planthoppe

108 h characteristic temperature dependence of a ballistic junction has been observed across 0.6 mum, a r

109 the electronic distribution impinging on the ballistic junction.

110 We employed fluorescent dye ballistic labeling ("DiOlistics") alone, or in conjuncti

111 Using a ballistic labelling method to load cells with Ca(2+) ind

112 valley-polarized conducting channels with a ballistic length of about 400 nanometres at 4 kelvin.

113 s is considered optimal; in particular, more ballistic Levy flights with exponent [Formula: see text]

114 urface state and deduce a quantum coherence (ballistic) lifetime of approximately 10 fs.

115 ues, deviating from the power requirement of ballistic light excitation and thus significantly reduci

116 constant repetition of a neurally generated ballistic-like biphasic pattern of torque which can cont

117 In a previous study using the penetrating ballistic-like brain injury (PBBI) model, engrafted huma

118 ximal offset of the spring-like element in a ballistic-like manner.

119 uency discharge (burst) for saccades and for ballistic limb movements.

120 uctance to exceed the fundamental Landauer's ballistic limit [Formula: see text] The effect is partic

121 n length to exhibit conductance close to the ballistic limit of 4e(2)/h at 8 T.

122 We observe, when approaching the ballistic limit, that charge quantization is destroyed b

123 have been fabricated that work close to the ballistic limit.

124 ent theoretical work has predicted that this ballistic mechanism also requires a nonlinearity in orde

125 From 2D-EV spectra, we elucidate a ballistic mechanism on the excited state potential energ

126 anotubes can behave like ohmically contacted ballistic metallic tubes, exhibiting room-temperature co

127 rbulence, estimated from times of coalescing ballistic microdroplets, suggest that complete mixing oc

128 xin for biological warfare; 200 bombs and 25 ballistic missiles laden with biological agents were dep

129 ncrease abruptly at a particular length--the ballistic mode at 16 micrometres and the other at 160 na

130 Paintball impact provides a robust ballistic model for isolating and quantifying the role o

131 rning and meandering motility, as opposed to ballistic motility, is enhanced by Myo1g.

132 beads, that maintain a consistent pattern of ballistic motion in the liquid.

133 these noncentrosymmetric nanofibers undergo ballistic motion in the presence of H(2)O(2) and thus co

134 th a generalized model that accounts for the ballistic motion of electrons in the metal, indicating t

135 square displacement (MSD) analysis separates ballistic motion phases, which we exclude here, from dif

136 on of the excitons dominates, with transient ballistic motion within a coherence length of up to 40 n

137 s is indeed indistinguishable from classical ballistic motion, we do find a notable exception.

138 e intervals, and intermediate time -interval-ballistic motion.

139 fficiencies of some Levy walks above that of ballistic motion.

140 The ballistic motor task induced an increase in corticospina

141 ers after a model-free learning task, i.e. a ballistic motor task, compared with model-based learning

142 he long standing and widely held belief that ballistic movements (i.e. straight-lines movements) outp

143 nnovative structural mechanisms that produce ballistic movements by amplifying power [1-6].

144 Nevertheless, we show that Levy walks and ballistic movements can be equally or almost equally eff

145 Ballistic movements in biology are powered by muscle con

146 Ballistic movements like saccades require the brain to g

147 We propose that ballistic movements that are powered by recoil of elasti

148 arge, fast motor neurons control high force, ballistic movements while small, slow motor neurons cont

149 Predictive control is crucial for fast and ballistic movements, but impaired prediction can also af

150 mes also improved for isometric and isotonic ballistic movements.

151 es often lead to quick fatigue and unnatural ballistic movements.

152 Here we demonstrate a ballistic nano-rectifier fabricated by creating an asymm

153 In order to test recently predicted ballistic nanofriction (ultra-low drag and enhanced lubr

154 o be even higher than that predicted for the ballistic nanofriction, confirming the enhanced lubricit

155 High-performance ballistic nanotube field-effect transistors with zero or

156 etermine the mechanisms underlying empirical ballistic observations.

157 ation using trained throwers to evaluate the ballistics of thrown spears during flight and at impact

158 nt processes and individual loci can undergo ballistic off-equilibrium movements.

159 emented in solids when electron transport is ballistic on the length scale of a device.

160 t with predictions for phonon transport in a ballistic, one-dimensional channel: at low temperatures,

161 that bridges the traditional depth limits of ballistic optical imaging and the resolution limits of d

162 e, the atomic resistance is analogous to the ballistic, or Sharvin resistance, and the atomic inducta

163 sport phenomena, whether purely diffusive or ballistic, our intermittent kICS approach allows an exha

164 arison between experiments and the theory of ballistic pai-Josephson junctions gives excellent quanti

165 at scales far smaller than believed and the ballistic pair dispersion holds over much longer distanc

166 The effectiveness of ballistic particle delivery to the skin is often depende

167 However, when joining two semi-infinite ballistic parts, such as the XX and XXZ spin-1/2 models,

168 ately 1 eV) electrons have surprisingly long ballistic path lengths in noble metals, allowing a large

169 ions before and after impacts delivered by a ballistic pendulum (30 to 300 g accelerations).

170 , the formation of interstellar dust clouds, ballistic penetrators, spacecraft shielding and ductilit

171 constraints on power output, making extreme ballistic performance noteworthy.

172 h a phenomenon has significant effect on the ballistic performance of B4C.

173 t not previously understood, decrease in the ballistic performance of boron carbide at high impact ra

174 and physical activity may plausibly predict ballistic performance, whereas tactical experience posit

175 benzoxazole ring resulting in a reduction of ballistic performance.

176 2.5 mum exceed those for graphene, and allow ballistic phonon transport along micron-length carbon ch

177 his high temporal resolution, we demonstrate ballistic photon transport in silicon ring resonators.

178 ploiting, for example, coherence properties, ballistic photons or penetrating wavelengths.

179 Here, we report ballistic plasmonic Au nanoparticle (NP) swimmers with u

180 ound that neural control of torques leads to ballistic, possibly more naturalistic movements than pos

181 ar surpassing the speeds of other documented ballistic predatory appendages in the animal kingdom.

182 set the stage for the parallel evolution of ballistic predatory strikes.

183 arrower, and transmission matching classical ballistic predictions.

184 size effects, pronounced nonlinearities, and ballistic processes produce behavior that diverges from

185 ingle-layer and bilayer graphene, we observe ballistic propagation and quantum interference of multip

186 mpared to the expected values in the case of ballistic propagation of light in a waveguide.

187 y that is intermediate between diffusion and ballistic propagation), by combining an analytical anoma

188 ogen, and boron nanostructures are promising ballistic protection materials due to their low density

189 der to a one-dimensional lattice, we observe ballistic quantum spreading.

190 bes are attached to the central section of a ballistic quantum wire to measure the inherent resistanc

191 ng four-terminal resistance in a single-mode ballistic quantum wire.

192 to test since the development of a source of ballistic R- rotons.

193 s identifies a thermophoretic regime that is ballistic rather than diffusive, persisting up to and be

194 w that the thermal radiation produced by the ballistic re-entry of ejecta condensed from the vapour p

195 e we present fluorescence imaging beyond the ballistic regime by combining single cycle pulsed ultras

196 Optical imaging beyond the ballistic regime has been demonstrated by hybrid techniq

197 itching of the polariton polarization in the ballistic regime has been demonstrated.

198 We probe this directional ballistic regime in a single crystal of PdCoO(2) by use

199 For short times, the ballistic regime of Brownian motion was observed, in con

200 monstrate fluorescence microscopy beyond the ballistic regime of light with a threefold improved reso

201 Access to the ballistic regime provides verification of the equipartit

202 whose conductivity can be modulated near the ballistic regime through the number of Fc units able to

203 aging of thick biological samples beyond the ballistic regime.

204 (30-300 microm) movements provide impulsive, ballistic regulation of CoM movement.

205 e system is enabled by parallel pathways for ballistic responses and flexible delayed actions and def

206 creases, this carrier transport becomes less ballistic, resulting in a considerable reduction in effi

207 Participants performed a ballistic right wrist extension task in four different t

208 to superdiffusive rotation and further to a ballistic rotation was observed with increasing asymmetr

209 ronic ground state are shown to be driven by ballistic S-C bond extension and to be complete within 3

210 By spatially filtering the ballistic scattering of an entangled photon, we find tha

211 Using ballistic self-consistent quantum simulations, it is sho

212 Electrons transmitted across a ballistic semiconductor junction are expected to undergo

213 Ballistic semiconductor structures have allowed the real

214 ovide conclusive experimental evidence that 'ballistic' separation prevails in the dynamics of pairs

215 Our experiments show that the ballistic spin Hall effect can be used for efficient inj

216 tic anisotropy and trigger a large-amplitude ballistic spin motion.

217 Deformation mechanisms at ballistic strain rates were characterized by grain rotat

218 rthest from their head milliseconds before a ballistic strike is initiated.

219 ntball impact velocities in both the porcine ballistic studies and CTH models, consistent with predic

220 Ballistic studies were conducted using gelatin-embedded

221 h quality InSb 2DEGs and provide evidence of ballistic superconductivity over micron-scale lengths.

222 anning from pure Brownian diffusion to (sub-)ballistic superdiffusion, are revealed by temporal and s

223 Here we report transport measurements on ballistic suspended graphene-Niobium Josephson weak link

224 available from slow temperature ramps versus ballistic temperature jumps is presented.

225 Here we use a microscopic ballistic test to report the responses of periodic glass

226 m 10 to 100 nanometers by using miniaturized ballistic tests.

227 ere we report an experimental observation of ballistic (that is, with no scattering of electrons) con

228 er-micron graphene samples reach ~35% of the ballistic thermal conductance limit up to room temperatu

229 Further, we demonstrate that this ballistic thermal injection mechanism can be utilized as

230 For pristine graphene, highly ballistic thermal transport is observed.

231 The resulting distance-independent ballistic thermophoretic force is not unlikely to posses

232 By fabricating quasi-ballistic three-dimensional topological insulator nanowi

233 and (2) how well the same subjects learned a ballistic thumb abduction task using the APB muscle.

234 the extent of the initial coherent (that is, ballistic) time-dependent evolution of the injected char

235 intervals, cell movement transitions from a ballistic to a diffusive regime.

236 using on the very short time dynamics of the ballistic to caged transition.

237 of organic molecules due to the switch from ballistic to diffusive propagation of light through a ch

238 observe a crossover in the time domain from ballistic to diffusive transport.

239 eak links that demonstrate a transition from ballistic to pseudo-diffusive like evanescent transport

240 We develop a theory of the ballistic-to-viscous crossover using an approach based o

241 gest that albanerpetontids were sit-and-wait ballistic tongue feeders, extending the record of this s

242 found that an elastically powered movement, ballistic tongue projection in chameleons, maintains hig

243 The evolution of ballistic tongue projection in plethodontid salamanders-

244 eon species outperform larger species during ballistic tongue projection, performance was examined du

245 emonstrate a motor control process of serial ballistic trajectories limited to an optimum rate of 2 s

246 eling elements, we quantify and simulate the ballistic trajectories of seeds, which are dispersed ove

247 the beginning of each step so the resulting ballistic trajectory of the walker's center-of-mass will

248 e artificial intelligence (AI) continues its ballistic trajectory, everything from text to audio, ima

249 port electron tunneling or even some form of ballistic transfer or a pathway transfer for an electron

250 Third, we used the cbr-unc-119 mutant in ballistic transformation and generated fluorescently lab

251 implementing nanoelectronic devices, such as ballistic transistors.

252 Electronic structure properties such as ballistic transmission and band structure computed using

253 cellular transport is a complex interplay of ballistic transport along filaments and of diffusive mot

254 Cavity exciton-polaritons exhibit ballistic transport and can achieve 100 mum in one picos

255 Here we show ballistic transport and quantized conductance of size-co

256 as remarkable electronic properties, such as ballistic transport and quantum Hall effects, and has al

257 nstriction exhibiting the quantum mechanical ballistic transport at [Formula: see text] but governed

258 of electrons in moire minibands by measuring ballistic transport between adjacent local contacts in a

259 However, it is difficult to achieve ballistic transport in a solid-state medium because the

260 cillations effectively demonstrate coherent, ballistic transport in mesoscopic rings and tubes.

261 is the standard theoretical tool to examine ballistic transport in nano- and meso-scale junctions, b

262 biting room-temperature conductance near the ballistic transport limit of 4e(2)/h, high current-carry

263 bulk, providing input to the question of how ballistic transport may be limited in the edge channels.

264 ding only two fitting parameters to a purely ballistic transport model, we can accurately characteriz

265 this spectral distribution by probing quasi-ballistic transport near nanostructured heaters down to

266 er is the Drude weight, which quantifies the ballistic transport of charge carriers.

267 n interacting integrable models, can support ballistic transport of conserved quantities including en

268 vealed that some quantum spin chains support ballistic transport of excitations at all energies.

269 cal insulator nanoribbons that exhibit quasi-ballistic transport over approximately 2 mum.

270 ronic performance, including low-temperature ballistic transport over distances longer than 15 microm

271 bit excellent electrical properties, such as ballistic transport over several hundred nanometers at r

272 which can make use of their room-temperature ballistic transport properties.

273 so that low diffusivity species experience a ballistic transport regime and are advected through the

274 Ideally, the carriers enter into a ballistic transport regime in which they are not scatter

275 zation at low temperatures, corresponding to ballistic transport through 1D subbands, where the measu

276 e oxide interface emits into air and makes a ballistic transport toward the suspended graphene.

277 -graphene coupling length, leading to nearly ballistic transport with a transfer efficiency of ~75%.

278 rees excellently with the Landauer theory of ballistic transport without any adjustable parameter.

279 Vacuum is an ideal medium for ballistic transport, but vacuum electronic devices commo

280 our Josephson junctions are consistent with ballistic transport, with a linear dependence on the Fer

281 m temperature, well beyond that required for ballistic transport.

282 own of Fourier's law through observations of ballistic transport.

283 ional discrete-time quantum walk model shows ballistic transport.

284 thermalization, and an outer one supporting ballistic transport.

285 of PdCoO(2) gives rise to highly directional ballistic transport.

286 njured by either weight drop or low-velocity ballistic trauma and assessed by clinical examination, e

287 s due to neurofibromatosis, severe burns, or ballistic trauma and had no relevant comorbidity.

288 Low-velocity ballistic trauma to the inferior sclera created a reprod

289 ed posterior scleral perforation in a severe ballistic trauma without previous instrumental signs of

290 to realize giant conductance oscillations in ballistic trilayer graphene Fabry-Perot interferometers,

291 The observations reveal a ballistic-type motion, and we provide a model that accou

292 he way to the realization of gate-controlled ballistic valley transport and the development of valley

293 Ballistic virtual reality (VR) can measure shooting perf

294 At low grid velocities, ballistic vortex rings are produced.

295 During ballistic wrist flexion movements, the latency of the se

296 ques: the triphasic EMG pattern accompanying ballistic wrist flexion movements; and reciprocal inhibi

297 DWI) scans were undertaken before unilateral ballistic wrist flexion training.

298 structed-delay task requiring them to make a ballistic wrist movement to a target in response to an a

299 roup A also had less co-contraction in their ballistic wrist movements between the first agonist and

300 rovide evidence that the release of targeted ballistic wrist movements by SAS is mediated, in part, b