ライフサイエンスコーパス: collision

1 f the collision (i.e., head-on vs off-center collision).

2 approximately 1200 mus for highly off-center collisions).

3 nt quality control are triggered by ribosome collision.

4 n exposure to the risk of pedestrian-vehicle collision.

5 rogen from oceanic subduction to continental collision.

6 activity was consistently terminated by wave collision.

7 can also be oxidized during single-particle collision.

8 he southern Tibetan Plateau after India-Asia collision.

9 cific processes or transitions that occur on collision.

10 es and includes irreversibility arising from collisions.

11 omic displacements following neutron-nucleus collisions.

12 olar wind-surface interactions and gas-phase collisions.

13 a detailed treatment of strong ion-electron collisions.

14 ensitizes cells to transcription-replication collisions.

15 n better understanding of the NP capture and collisions.

16 ctive-landing for the peptide-H(+) + surface collisions.

17 acting at sites of replication-transcription collisions.

18 because its parent body has been consumed by collisions.

19 facilitates electron transfer in the droplet collisions.

20 ile minimizing interference from vapor-phase collisions.

21 .47 pM(-1) s(-1)) of single Escherichia coli collisions.

22 o by non-nebular processes like planetesimal collisions.

23 to a fall (<2 m 34%, >2 m 24%), road traffic collision (25%), and other (17%).

24 0 kilometres in diameter during a shattering collision 7.5 million years ago.

25 However, challenges still exist for collision activated dissociation (CAD) MS/MS based quant

26 The collision-activated dissociation (CAD) fragmentation pat

27 the accessibility of a regime where elastic collisions also become relevant for suspensions of micro

28 In particular, random collisions among crowded proteins generate substantial p

29 ubules through frequent catastrophe-inducing collisions among microtubules.

30 ctrodes using stochastic single-nanoparticle collision amperometry.

31 egime with strong stimulation of spontaneous collisions analogous to superradiance has proved elusive

32 building significantly post-date Indo-Asian collision and challenge the suggestion that the extent o

33 reported behaviors suggest that nanoparticle collision and electro-dissolution is a highly dynamic pr

34 nstrates that omnipolar EGMs can account for collision and fractionation and record EGM voltages unaf

35 in solution and that is released upon their collision and fusion with the fluid interface.

36 ets ( approximately 350 x g), mitigating the collision and lowering the impalement probability by app

37 results demonstrate that silver nanoparticle collision and oxidation is highly dynamic and likely con

38 The highly dynamic process of nanoparticle collision and oxidation is imaged by single-particle flu

39 lectrochemical nanocell to image the dynamic collision and oxidation process of single silver nanopar

40 double-strand breaks (DSBs) at sites of fork collisions and causes genomic damage, including repeat i

41 e conditions required for runaway stimulated collisions and reveal the quantum nature of matter-wave

42 pid dissociation of the holoenzyme is always collision, and no unique characteristics need to be assi

43 e antibody sequence relative to conventional collision- and electron-based fragmentation methods.

44 addition processes and by particle-particle collision-and-fusion events.

45 For most collision angles, the interaction energy is weak because

46 e show that all NPs on the UME surface after collision are attached and electrochemically active.

47 individual Pt nanoparticles (NPs) undergoing collisions at a Au ultramicroelectrode (UME) (5 mum radi

48 al steps, produced through the nanoparticles collisions at the CFUME surface, are respectively propor

49 ort a new experimental setup for studying NP collisions based on the use of carbon nanopipettes to en

50 often less well characterized by traditional collision-based activation methods.

51 for why different cell types have different collision behavior and the effect of interventions that

52 The dynamic collision behavior of the electro-oxidation of single Ag

53 regime occurs when particles undergo binary collisions beneath the surface apexes.

54 f replicative life span (RLS), prevention of collision between replication and transcription, and cel

55 monstrate a controlled and coherent exchange collision between two photons that is accompanied by a p

56 ended the model to include multiple parallel collisions between long dsDNA molecules, and find that t

57 under shock loading is critical for modeling collisions between planetary bodies, interpreting the si

58 In these assays, collisions between polarized cells occur frequently with

59 low because it is gated by diffusion-limited collisions between sensitizer and catalyst.

60 ing the partition of energy in above-thermal collisions between the translational and rotational degr

61 orphologies after experiencing high velocity collisions, but materials science regarding the extreme

62 of stereodynamics in inelastic atom-molecule collisions can often be understood from classical consid

63 and quantitatively) an important role of the collision cascade density in dynamic radiation defect pr

64 Effects of the collision cascade density on radiation damage in SiC rem

65 Results show that, for both Si and SiC, collision cascades are mass fractals with fractal dimens

66 eneral method by which the fractal nature of collision cascades can be used to explain experimental o

67 Although collision cascades have previously been described as fra

68 dment with heavier ions, which create denser collision cascades, results in a decrease in the dynamic

69 distribution of atomic displacements within collision cascades.

70 ion which accounts for the fractal nature of collision cascades.

71 on and migration mechanisms during and after collision cascades.

72 es not manifest itself until long after head collisions cease.

73 10+) by either increasing the source lens or collision cell (or HCD) voltages.

74 n-induced dissociation (CID) at 1.5 keV in a collision cell filled with argon gas, for confident iden

75 Helium collision cell gases and reactive ammonia gas are invest

76 -ICR instrument in place of the standard gas collision cell.

77 g a chaotic distribution for the short-range collision complex that plays a key role in governing the

78 These collision complexes are generally not thought to react c

79 termolecular reactions mediated by ephemeral collision complexes are probably of significance in vari

80 ulations, we reveal that reactions of H + O2 collision complexes with other radicals constitute major

81 ular association reactions involve ephemeral collision complexes-formed from the collision of two mol

82 ilicon (Si) with silane (SiH4 ) under single-collision conditions in crossed molecular beam experimen

83 (C7 H8 ) on the triplet surface under single-collision conditions.

84 was performed by correlating the ion-neutral collision cross section (CCS) and charge state with the

85 resolving power (Rp), resolution (Rpp), and collision cross section (CCS) for compounds analyzed in

86 Collision cross section (CCS) measurement of lipids usin

87 nstrument suitable for rotationally averaged collision cross section (CCS) measurements at low E/N ra

88 Collision cross section (CCS) measurements resulting fro

89 Ion mobility collision cross section (CCS) measurements show that ubi

90 on technique, which relies on differences in collision cross section (CCS) of ions.

91 parison between theoretical and experimental collision cross section (CCS) values to support the iden

92 Diastereomers exhibited differences in their collision cross section (CCS), but were unresolvable in

93 rovide orthogonal information, i.e., m/z and collision cross section (CCS), for the identification of

94 ectrometry allows for the measurement of the collision cross section (CCS), which provides informatio

95 , linear dynamic range, resolving power, and collision cross section (Omega) are reported for each st

96 lity spectrometry (IMS) was impeded by small collision cross section differences (commonly approximat

97 The measured collision cross section in helium for the Naph(+*)(Pyr)

98 However, the collision cross section increases by approximately 2% be

99 and toluene, a reduction in the ion-neutral collision cross section of the isotopically replaced spe

100 ns were monomodal and were used to determine collision cross section values that are within 3% of tho

101 Inspection of the [m/z; chemical formula; collision cross section] data sets shows that the WAF co

102 ic complexity (e.g., [m/z; chemical formula; collision cross section] data sets) for a better evaluat

103 Collision cross sections (CCS) are usually discussed bas

104 Calculated collision cross sections (CCS) for SP(3+) ions at variou

105 Collision cross sections (CCS) were calculated and plott

106 exhibit very distinctive IM drift times and collision cross sections (CCS).

107 tification by measurement of their gas phase collision cross sections (CCSs).

108 ormation content of IM separations, absolute collision cross sections (Omega) with He, N2, Ar, CO2, a

109 Comparison of measured collision cross sections (Omega) with values calculated

110 ly isomerize to structures that have smaller collision cross sections (Omega).

111 Several effects of temperature on collision cross sections and resolution are observed.

112 s further information on the distribution of collision cross sections of each conformational ensemble

113 tion technique that is used to determine the collision cross sections of native-like ions of proteins

114 For delays ranging from 16 to 33 231 ms, the collision cross sections of native-like, 7+ cytochrome c

115 ch as diagnostic ions, isotopic matches, and collision cross sections were applied for metabolites id

116 phase mainly based on differing ion-neutral collision cross sections, enabling powerful analysis of

117 ity spectrometry allows one to determine ion collision cross sections, which are related to ion size

118 k width in the time domain, is irrelevant to collision cross sections.

119 Moreover, by enabling determination of a collision cross-section (CCS) value-a parameter related

120 The use of collision cross-section (CCS) values obtained by ion mob

121 The CAPTR products all have collision cross-section (Omega) values that are within 5

122 buffer-gas allows us to measure the absolute collision cross-section for conformational relaxation.

123 Collision cross-section measurements and molecular model

124 Collision cross-section measurements showed that the aur

125 mass spectrometry are used to determine the Collision Cross-Sections (CCS) of ions.

126 void unnecessary calculation, especially for collision detection, allowing it to be simultaneously ru

127 (ETcaD), and electron-transfer/higher-energy collision dissociation (EThcD) fragmentation methods whe

128 fer dissociation combined with higher energy collision dissociation (EThcD) provides exceptional data

129 lectron-transfer combined with higher-energy collision dissociation (EThcD), for characterization of

130 gmentation methodologies such as high-energy collision dissociation (HCD) and collision induced disso

131 entation techniques, including higher-energy collision dissociation (HCD), electron-transfer dissocia

132 cally compared the efficacy of higher-energy collision dissociation (HCD), electron-transfer dissocia

133 f separated species validated by high-energy collision dissociation experiments.

134 Here, we show that local collision-driven nematic alignment interactions among fi

135 ption factor residence time and non-specific collisions during sampling for DNA targets.

136 In this work, collision dynamics and nonlinear material characteristic

137 ts of various experimental conditions on the collision dynamics.

138 rate and comprehensive datasets for electron collisions enable complex modeling of plasma-using techn

139 recursor selection, alternating high and low collision energies to analyze product and precursor ions

140 ribrid mass spectrometer and optimized their collision energies with regard to optimal sequence cover

141 n mass spectrometry instruments with several collision energies, we proved the method's platform inde

142 High collision energies, which are required for fragmentation

143 atoms were previously carried out near zero collision energies.

144 ical reactions is how reactions proceed at a collision energy close to absolute zero.

145 ns of the reaction kinetics as a function of collision energy over the range 0.005 kelvin (K) to 30 K

146 sulting data-dependent decision tree against collision energy-optimized single methods on two samples

147 riment (all ion fragmentation) applying high collision energy.

148 ter have so far relied exclusively on higher collision-energy dissociation (HCD) fragmentation for pe

149 The method involves collisions entirely between first order solitons in opti

150 cies 1,2,4,7-cyclooctatetraenyl via a single-collision event and opens up a versatile, unconventional

151 d is based on measurements of the individual collision events between ssDNA aptamer-functionalized Ag

152 The number of collision events involving the bacterial cells indicated

153 n nanopipettes to enable monitoring multiple collision events involving the same NP captured inside t

154 trode orientation and from fractionation and collision events.

155 Thus, collision experiments can be used to prepare small NP en

156 This approach enables collision experiments with various complex quasiparticle

157 kinetics of the initial event of microtubule collision followed by ADP release for KIF3AC is not equi

158 magnetic Feshbach resonance in ultracold Rb collisions for above-threshold energies and their method

159 storical probabilities of pedestrian-vehicle collisions for intersections and midblock segments withi

160 higher density gas regime toward a very cold collision-free cluster regime that is dominated by produ

161 experimentally validated, demonstrating both collision frequency (beta) and background particle conce

162 d from chronopotentiograms, is closer to the collision frequency calculated by using the theoretical

163 fic binding events of target analyte induced collision frequency changes enabling ultrasensitive dete

164 These contribute to the larger NP collision frequency observed experimentally.

165 ent between the theoretical and experimental collision frequency of individual Pt nanoparticles (NPs)

166 t the ac heating leads to an increase in the collision frequency of studied nanoparticles with workin

167 Interestingly, the collision frequency resulted from the chronoamperograms,

168 r of collisions is achievable and, thus, the collision frequency, f, increases and the limit of detec

169 n values, which are directly proportional to collision frequency.

170 as if the system has turned into a diffusive collision-full classical system.

171 However, we observe that the collisions give rise to shifts in the center-of-mass pos

172 roplets collide but also the geometry of the collision (i.e., head-on vs off-center collision).

173 Mean risk of pedestrian-vehicle collision in specific walking locations was assessed acc

174 Furthermore, promoting global ribosome collision in vivo resulted in ubiquitination of ribosoma

175 n products result from reactive ion-molecule collisions in a comparatively higher pressure and temper

176 Here we find that runaway stimulated collisions in Bose-Einstein condensates with periodicall

177 article-in-cell simulations with Monte Carlo collisions included have revealed formation dynamics of

178 conditions and time after desolvation using collision induced activation (CIA), time-resolved hydrog

179 s of tandem mass spectra (MS/MS) obtained by collision induced dissociation (CID) and 351 nm ultravio

180 The adjusted collision induced dissociation (CID) conditions generate

181 f dityrosine cross-linked Abeta(1-16), using collision induced dissociation (CID), higher-energy coll

182 high-energy collision dissociation (HCD) and collision induced dissociation (CID), provided the compl

183 The use of FAIMS-selected in source collision induced dissociation (FISCID) yields fragmenta

184 on induced dissociation (CID), higher-energy collision induced dissociation (HCD), electron transfer

185 Collision induced dissociation experiments and Kendrick

186 inct signature fragmentation patterns during collision induced dissociation.

187 [4-(trimethylammonio)phenyl]acetic acid upon collision induced dissociation.

188 Structural confirmation was achieved by collision induced fragmentation following liquid extract

189 eral inferences regarding the sensitivity of collision induced unfolding to changes in protein primar

190 and ionization of peptide-ligand adducts and collision-induced adduct loss hinder the acquisition of

191 ified in MS2-based database searches because collision-induced adduct loss was the dominant feature o

192 imilar for each protein and may be caused by collision-induced changes in the ion trajectory.

193 culosis (Mtb) CYP142A1 were assessed through collision-induced dissociation (CID) and collision-induc

194 ng a 1 Da mass isolation window, followed by collision-induced dissociation (CID) at 1.5 keV in a col

195 ces to create a local database against which collision-induced dissociation (CID) data of modified ol

196 a therapeutic cyclic peptide, exhibits poor collision-induced dissociation (CID) efficiency for mult

197 the advantages of online mobility separated collision-induced dissociation (CID) followed by high re

198 uced adduct loss was the dominant feature of collision-induced dissociation (CID) fragmentation, but

199 Collision-induced dissociation (CID) of these cationic m

200 charged ions, we show the advantage of using collision-induced dissociation (CID) post-UVPD: radical

201 havior of pyrophosphorylated peptides during collision-induced dissociation (CID), a data dependent n

202 fragmentation methods and two combinations: collision-induced dissociation (CID), beam-type CID (HCD

203 ors using the five fragmentation techniques: collision-induced dissociation (CID), beam-type CID (HCD

204 in analysis by electrospray ionization (ESI)-collision-induced dissociation (CID)-FTICR MS was applie

205 peptide backbone information was provided by collision-induced dissociation (CID)-MS3 fragmentation.

206 ent ion deuterium incorporation pattern upon collision-induced dissociation (CID).

207 confirmed via tandem mass spectrometry using collision-induced dissociation and supported by exact ma

208 y high, such that collisional scattering and collision-induced dissociation are expected to underlie

209 nteraction, as determined by energy-resolved collision-induced dissociation cross-section experiments

210 , ion mobility separation arrival times, and collision-induced dissociation fingerprints of HMO anion

211 Collision-induced dissociation mass spectrometry of the

212 re of a given glycopeptide was determined by collision-induced dissociation MS/MS fragmentation, and

213 product and neutral loss signals obtained by collision-induced dissociation to a user-defined white l

214 rmative product ions arising from ozone- and collision-induced dissociation.

215 n mobility-mass spectrometry (ESI-IM-MS) and collision-induced unfolding (CIU) analysis of four diUbq

216 ugh collision-induced dissociation (CID) and collision-induced unfolding (CIU) as monitored by nanoel

217 Here, we show using collision-induced unfolding (CIU) ion mobility-mass spec

218 h two leaders extending toward each other to collision inside the CSZ.

219 In a quantum picture, however, the collision is described in terms of matter waves, which c

220 ation of ribosomal proteins, suggesting that collision is sensed by the cell to initiate downstream q

221 me that, within experimental error, every NP collision is successful and occurs through a sticking me

222 ern and the risk of pedestrian-motor vehicle collision is unknown.

223 ntal chronopotentiograms, a higher number of collisions is achievable and, thus, the collision freque

224 romoted the formation of metal oxides during collision leading to a unique core-shell type nanostruct

225 ated origin firing increase the number of HO collisions leading to genome-destabilizing R-loops.

226 The number of collision lesions from 0.07% to 1.07%.

227 0) cm(3) s(-1) at 294 K exceed estimates for collision-limited values, suggesting rate enhancement by

228 For high-velocity (i.e., > 1 m/s) off-center collisions, mixing times increased by as much as a facto

229 For low-velocity (<1 m/s) off-center collisions, mixing times were consistent with the head-o

230 Upon collision, multiple topological edge solitons emerge und

231 43/50 [86%]) occurring in areas of wavefront collision (n=21; median 0.5; quartiles 0-2 per map) or a

232 cates that each spike is associated with the collision of a single sub-picoliter droplet.

233 phemeral collision complexes-formed from the collision of two molecules-that collide with a third and

234 anism for directional reversal through which collisions of Cut7 motor domains with their neighbors in

235 ed for low velocity ( approximately 0.1 m/s) collisions of droplets with <40 mum diameters.

236 which permits direct O2 formation in single collisions of energetic water ions with oxidized cometar

237 Investigating the collisions of individual metal nanoparticles (NPs) with

238 ocity distributions for a series of reactive collisions of the type X(-) + RY with X and Y denoting t

239 ciated DNA/RNA hybrid formation, and promote collisions of transcription complexes with replisomes.

240 visual looming motion created by an imminent collision or approaching predator.

241 h are not influenced by directional factors, collision or fractionation, compared with contemporary b

242 tion, CIL and cell-cell adhesion governs the collision outcome.

243 nd the effect of interventions that modulate collision outcomes.

244 Results show that an Ag nanoparticle collision/oxidation event typically consists of a series

245 ak because only a few binding sites near the collision point contribute significantly to the binding

246 or understanding complex dependencies in the collision probabilities of multiple random walks.

247 the strong anisotropic forces present in the collision process.

248 xperiment is obtained for each of these four collision properties.

249 mass dependence due to the acceleration and collision properties.

250 In this regime, the collisions rapidly produce highly correlated states with

251 m (WASP) was updated to incorporate particle collision rate and particle attachment efficiency to sim

252 in agreement with inductively coupled plasma collision/reaction interface mass spectrometry (ICP-CRI-

253 a stabilizing Pol delta-CMG interaction, the collision release process is triggered, ejecting Pol del

254 delta, like bacterial replicases, undergoes collision release upon completing replication, and we pr

255 of the Tibetan plateau during the India-Asia collision remains an outstanding issue.

256 Each collision results in a detectable current transient.

257 ndings may suggest that pedestrians moderate collision risk by using lower-risk routes.

258 Males walked in areas with higher collision risk compared with females, while vehicle owne

259 ypically walked in areas with low pedestrian collision risk when walking for recreation, walking at a

260 of young children walked in areas with lower collision risk.

261 ration and distance were not associated with collision risk.

262 In our computational analysis, ribosome collisions selectively stimulate abortive termination wi

263 We propose that ribosome collisions serve as a robust timer for translational qua

264 Accordingly, specific populations such as collision sport athletes and certain military personnel

265 At high temperatures, electron-electron collisions suppress focusing.

266 The coexpansion brought the collision temperature down to 1 kelvin, restricting scat

267 are increasing potential for iceberg-seabed collisions, termed ice scour.

268 the small moons formed in the aftermath of a collision that produced the Pluto-Charon binary.

269 rgely confined area hence leads to increased collisions that are compatible with the formation of gen

270 aged on the UME surface and the number of NP collisions that led to their adsorption, a spherical NP

271 e, liquid state systems, including: (i) near-collision-time-scale hydrodynamic organization of single

272 on of hydrazine exactly at the time of Pd-NP collision to the CFUME surface, was used to detect each

273 ng times increased from <200 mus for head-on collisions to approximately 1200 mus for highly off-cent

274 amplitudes and faster propagation with more collisions to each other.

275 pes of RWs from standard breathers and their collisions to more general nonlinear modes characterized

276 sed to detect single Pd nanoparticle (Pd-NP) collisions to the surface of a carbon fiber ultramicroel

277 and stable background was used to record the collision transients.

278 At collision velocities >7 m/s, droplet separation and frag

279 These results suggest a limited range of collision velocities over which complete and rapid mixin

280 pphire and aluminum, across a broad range of collision velocities, from 50 to 1,100 m/s.

281 imes ranging from approximately 900 mus at a collision velocity of 0.1 m/s to <200 mus at approximate

282 enhancing local concentration and promoting collision via two-dimensional diffusion.

283 Indian subcontinent after Eocene continental collision was not a uniform process, but was subject to

284 For head-on collisions, we achieve submillisecond mixing times rangi

285 ycles of Okazaki fragment initiation using a collision with a completed Okazaki fragment or primer-pr

286 generally not thought to react chemically on collision with a third molecule in the gas-phase systems

287 r, our measurements support a model in which collision with a trailing ribosome causes abortive termi

288 sity, thereby improving its odds of a chance collision with prey and ultimately reducing BV's search

289 The collision with primer-primase complexes triggering the e

290 nergy to the lattice through nuclear-nuclear collision with the crystal lattice remains largely unadd

291 r domain of E-cadherin, and was designed for collision with the healing edge of an epithelial monolay

292 by monitoring their catalytically amplified collisions with a Hg-coated microelectrode used as the t

293 of the diatomic molecule undergo consecutive collisions with a metal surface atom without bond ruptur

294 As GNRs are slowed by intermittent collisions with ECM fibers, DT is sensitive to ECM poros

295 g action of Cut7 is selectively inhibited by collisions with neighbors under crowded conditions, wher

296 quency change is due to ion energy loss from collisions with the background gas.

297 investigated through precise single particle collisions with two distinctive substrates, sapphire and

298 Collisions with vessels are believed to represent the ma

299 ormation and structures along the India-Asia collision zone are primarily controlled by the strength

300 thquake in Tohoku-Oki, Japan, or along large collision zones, such as the 1999 moment magnitude 7.7 e