ライフサイエンスコーパス: ballistic

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

2 coustically levitated drop with simultaneous ballistic addition of reactant.

3 We observe ballistic and anisotropic energy flow through the protei

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

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

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

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

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

9 Modern war ballistics and blast injuries inflict devastating extrem

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

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

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

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

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

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

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

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

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

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

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

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

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

23 to their superior specific surface area and ballistic conductivity.

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

41 Ballistic electrons in solids can have mean free paths f

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

66 Ballistic impact studies and supercomputer modeling were

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

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

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

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

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

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

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

74 Investigations using ballistic intracellular nanorheology reveal that lamin A

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

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

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

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

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

80 the electronic distribution impinging on the ballistic junction.

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

111 Ballistic movements like saccades require the brain to g

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

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

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

115 mes also improved for isometric and isotonic ballistic movements.

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

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

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

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

120 etermine the mechanisms underlying empirical ballistic observations.

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

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

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

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

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

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

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

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

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

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

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

132 benzoxazole ring resulting in a reduction of ballistic performance.

133 2.5 mum exceed those for graphene, and allow ballistic phonon transport along micron-length carbon ch

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

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

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

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

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

139 arrower, and transmission matching classical ballistic predictions.

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

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

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

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

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

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

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

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

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

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

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

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

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

153 aging of thick biological samples beyond the ballistic regime.

154 (30-300 microm) movements provide impulsive, ballistic regulation of CoM movement.

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

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

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

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

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

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

161 Ballistic semiconductor structures have allowed the real

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

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

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

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

166 Ballistic studies were conducted using gelatin-embedded

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

188 implementing nanoelectronic devices, such as ballistic transistors.

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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