ライフサイエンスコーパス: avalanche

1 c mechanism as the result of "coevolutionary avalanches".

2 nts of a large number of particles known as 'avalanches'.

3 e (aging) and involve intermittent dynamics (avalanching).

4 ine are different from those involved in the avalanche.

5 iant, cascades of activity known as neuronal avalanches.

6 cal branching process that produces neuronal avalanches.

7 on leads to a different subsequent series of avalanches.

8 across many spatial scales, termed neuronal avalanches.

9 rticles and does not involve any large-scale avalanches.

10 d variability of synchrony, and (3) neuronal avalanches.

11 natural to focus on the attributes of these avalanches.

12 t which ongoing activity emerges as neuronal avalanches.

13 us monkeys carries the signature of neuronal avalanches.

14 clusters in space and time, called neuronal avalanches.

15 described by the same equations that govern avalanches.

16 ing critical generational models of neuronal avalanches.

17 tworks is described by equations that govern avalanches.

18 c patterns of activation not seen in smaller avalanches.

19 -invariant spatiotemporal clusters, neuronal avalanches.

20 g state in the presence of cortical neuronal avalanches.

21 mporal cascades of activity, termed neuronal avalanches.

22 cooling and large-scale, inward propagating avalanches.

23 reciable levels of intrinsic noise can cause avalanching, a complex mode of operation that dominates

24 agnetic fluctuations that manifest as domain avalanches and chaotic magnetization jumps exemplify suc

25 human subjects at rest organizes as neuronal avalanches and is well described by a critical branching

26 Neuronal avalanches and long-range temporal correlations (LRTCs)

27 correlated with those of concurrent neuronal avalanches and LRTCs in anatomically identified brain sy

28 d in a complex manner with cortical neuronal avalanches and LRTCs in MEG but not SEEG.

29 The exponents of power-law regimen neuronal avalanches and LRTCs were strongly correlated across sub

30 Our results identify avalanches and oscillations as dual principles in the te

31 ere, we show that critical-state dynamics of avalanches and oscillations jointly emerge in a neuronal

32 experiments and model suggest that neuronal avalanches and peak information capacity arise because o

33 governing the cascading activity of neuronal avalanches and the distribution of phase-lock intervals

34 and quiescence in the framework of neuronal avalanches and will help to enlighten the mechanisms und

35 quiet times depend on the size of preceding avalanches and, at the same time, influence the size of

36 d here can be used to study the emergence of avalanching (and other complex phenomena) in many biolog

37 of soft spots, the fractal dimension of the avalanches, and their duration.

38 ) is characterized by intermittent bursts of avalanches, and this trend results in disastrous failure

39 By investigating the quasi-static avalanche angle, compaction, and dilatancy effects in di

40 and extinction, very large-scale extinction avalanches appear to be absent from the dynamics, and we

41 Neuronal avalanches are a type of spontaneous activity observed i

42 These avalanches are associated with the more heterogeneous di

43 Snow slab avalanches are believed to begin by the gravity-driven s

44 reover we evidence that sizes of consecutive avalanches are correlated.

45 This demonstrates that neuronal avalanches are linked to the global physiological state

46 ts that criticality and, therefore, neuronal avalanches are optimal for input processing, but until n

47 al performance or whether neuronal LRTCs and avalanches are related.

48 Neuronal avalanches are spatiotemporal patterns of neuronal activ

49 ) is near critical and organizes as neuronal avalanches at both resting-state and stimulus-evoked act

50 egularity and assembles into scale-invariant avalanches at the group level.

51 llium, MMAN; Nucleus Interface, NIf; nucleus Avalanche, Av; the Robust nucleus of the Arcopallium, RA

52 Vps45, and we further identify the syntaxin Avalanche (Avl) as a target for Vps45 activity.

53 that has been used to describe steady-state avalanche behaviour in different materials.

54 hat cortical networks that generate neuronal avalanches benefit from a maximized dynamic range, i.e.,

55 Sight Foundation, Brian King Fellowship, and Avalanche Biotechnologies, Inc.

56 rs (APD) using charge amplification close to avalanche breakdown can achieve high gain and thus detec

57 various electric field strengths up to near avalanche breakdown in high magnetic fields of about 1.2

58 However, initiating the impact ionization of avalanche breakdown requires a high applied electric fie

59 field phenomena of inter-valley transfer and avalanching breakdown have long been exploited in device

60 At high drain currents (>10 muA/mum) avalanching breakdown is also observed, and is attribute

61 ir pocket may improve chances of survival in avalanche burial.

62 yxia is the most common cause of death after avalanche burial.

63 whether the device improves survival during avalanche burial.

64 rties are co-responsible for survival during avalanche burial.

65 ich we observe unconventional quasi-periodic avalanche bursts and higher critical exponents as the st

66 hat crystallization is associated with these avalanches but that the connection is not straightforwar

67 of crystal in the system increases during an avalanche, but most of the particles that become crystal

68 ates the nonlocal transport by truncation of avalanches by local sheared toroidal flows which develop

69 nd experimental demonstration of engineering avalanche characteristics in InGaAs/AlInAs SLs and would

70 co-existence of a scale-free behaviour (the avalanches close to criticality) and scale-dependent dyn

71 The avalanches collected during interictal epileptiform acti

72 This theory suggests that whenever avalanches compete with slow relaxation--in settings ran

73 The nanopillar optical antenna avalanche detector (NOAAD) architecture is utilized for

74 In this work, we use a single-photon avalanche detector array camera with pico-second timing

75 tary metal oxide semiconductor single photon avalanche detector imaging array, miniaturised optical i

76 Silicon single-photon avalanche detectors are becoming increasingly significan

77 nge.The performance of silicon single-photon avalanche detectors is currently limited by the trade-of

78 multimode light to an array of single-photon avalanche detectors, each of which has its own time-to-d

79 a trade-off in current silicon single-photon avalanche detectors, especially in the near infrared reg

80 to improve the performance of single-photon avalanche detectors, image sensor arrays, and silicon ph

81 0.5 MP resolution, time-gated Single Photon Avalanche Diode (SPAD) camera, with acquisition rates up

82 ermanium-on-silicon (Ge-on-Si) single-photon avalanche diode (SPAD) detectors for short-wave infrared

83 ve detection system based on a Single Photon Avalanche Diode (SPAD) with high sensitivity and low noi

84 a 780-nm pulsed diode laser, a single-photon avalanche diode (SPAD), and a high-numerical-aperture mi

85 maging when used with emerging single-photon avalanche diode array detectors with resolution only lim

86 ght-trapping, thin-junction Si single-photon avalanche diode that breaks this trade-off, by diffracti

87 ve area (diameter 500 microns) single-photon avalanche diode that was actively quenched to provide a

88 ton-counting detectors such as single-photon avalanche diode, photomultiplier tube, or arrays of such

89 er diode and a custom designed Single-Photon Avalanche Diodes (SPADs) camera.

90 color channels monitored with single-photon avalanche diodes (SPADs) that could transduce events at

91 the luminescence to a pair of single-photon avalanche diodes (SPADs).

92 ce a technique that co-designs single-photon avalanche diodes, ultra-fast pulsed lasers, and a new in

93 limited recovery speed of the single-photon avalanche diodes.

94 Meanwhile, the avalanche distributions display two distinct power-law r

95 istance, which allows for the scaling of the avalanche distributions vis-a-vis the archetypal disloca

96 cooperative rearrangements of displacements (avalanches) diverges.

97 text] 2.5 decades of slip sizes) to a large avalanche domain (spanning [Formula: see text] 4 decades

98 c processes of saltation and grainfall (sand avalanching down the dune slipface) operate on both worl

99 own voltage when field emission and Townsend avalanche drive breakdown.

100 ggest optimization principles identified for avalanches during ongoing activity to apply to cortical

101 However, insight into the avalanche dynamics and LRTCs in the human brain has been

102 In experiment and theory, avalanche dynamics are identified by two measures: (1) a

103 Both MEG and SEEG revealed avalanche dynamics that were characterized parameter-dep

104 a previously-validated test of criticality: avalanche dynamics to assess the differences in brain dy

105 Avalanching dynamics are studied in many disciplines, wi

106 For example, avalanches, earthquakes, and forest fires all propagate

107 zero field is influenced by a bulk magnetic avalanche effect coupled with tunneling of the magnetiza

108 nputs and power-law statistics of forgetting avalanches, emerge naturally from this mechanism, and we

109 In vitro spike avalanches emerged naturally yet required balanced excit

110 The effects of system size on the avalanche events are examined, and average values of Del

111 using Paschen's law (PL), driven by Townsend avalanche, fails for gap distance d [Formula: see text]

112 nhuman primates that the temporal profile of avalanches follows a symmetrical, inverted parabola span

113 storage, and transfer, but the relevance of avalanches for fully functional cerebral systems has bee

114 that cortical resting activity organizes as avalanches from firing of local PN groups to global popu

115 tage of only 1.5 V is required to achieve an avalanche gain of over 10 dB with operational speeds exc

116 ological model of bacterial infection, where avalanching has not been characterized before, and a pre

117 Recently, neuronal avalanches have been observed to display oscillations, a

118 critical theory on the temporal unfolding of avalanches have yet to be confirmed in vivo.

119 The disastrous shear avalanches have, then, been delayed by forming a stable

120 them by adapting the definition of "neuronal avalanches" (i.e., spurts of population spiking).

121 The oscillations organized as neuronal avalanches, i.e., they were synchronized across cortical

122 otection against hazards such as landslides, avalanches, ice breaks, and rock or soil failures.

123 lem not yet resolved to inhibit the electron avalanche in RF equipment that limit their maximum worki

124 is the coincidence of a large coevolutionary avalanche in the ecosystem with a severe environmental d

125 Here we report Fourier space studies of avalanches in a system exhibiting competing magnetic str

126 ing functions for the dynamics of individual avalanches in both systems, and show that both the slip

127 ing and comparing the full time evolution of avalanches in bulk metallic glasses and granular materia

128 eement with recent mean-field theory of slip avalanches in elasto-plastic materials, revealing the ex

129 e for the existence and extent of the domain avalanches in ferroelectric materials, forcing us to ret

130 riticality, as evidenced by the emergence of avalanches in fitness that propagate across many generat

131 l features, such as the size distribution of avalanches in gene activity changes unleashed by transie

132 -flow mechanisms in BMGs and controlling the avalanches in relating solids.

133 bust power-law scaling in neuronal LRTCs and avalanches in resting-state data and during the performa

134 dependent spontaneous recurrence of specific avalanches in superficial cortical layers might facilita

135 r cortical dynamics such as ongoing neuronal avalanches in the alert monkey and evoked visual respons

136 evels, e.g., in the distribution of neuronal avalanches in vitro and in vivo, but also in the decay o

137 Cortical avalanches in vitro were accompanied by low-correlated r

138 tion, and are subject to stochastic chemical avalanches, in the absence of nucleotides or any monomer

139 , diversity, and temporal precision of these avalanches indicate that they fulfill many of the requir

140 This parabola constrains how avalanches initiate locally, extend spatially and shrink

141 andom, although correlations are found among avalanche initiation events.

142 as supported by the spatial spreading of the avalanches involved.

143 s the plasma density in the seed channel via avalanche ionization.

144 d by a combination of Zener and Zener-seeded avalanche ionization.

145 Third, the occurrence of the avalanches is a largely stochastic process.

146 hing under snow, e.g. while buried by a snow avalanche, is possible in the presence of an air pocket,

147 This instrument, called the Pulsed Electron Avalanche Knife (PEAK), can quickly and precisely cut in

148 Gravity-driven avalanches, known as turbidity currents, are the primary

149 dams formed by landquake events such as rock avalanches, landslides and debris flows can lead to seri

150 This study models the probabilities of snow avalanches, landslides, wildfires, land subsidence, and

151 Here, we show that although neuronal avalanches lasted only a few milliseconds, their spatiot

152 tion of the device is accompanied with large avalanche like noise that is ascribed to the redistribut

153 s we observed pronounced supercooling and an avalanche-like abrupt transition from the ferromagnetic

154 ting that IFT injection dynamics result from avalanche-like behavior.

155 The tunably rugged NK-model is used to study avalanche-like events that occur when environmental chan

156 ide evidence that IFT injections result from avalanche-like releases of accumulated IFT material at t

157 lex behaviour in sudden airway narrowing and avalanche-like reopening.

158 Our findings suggest that "neuronal avalanches" may be a generic property of cortical networ

159 ices undergo reversal through a dendritic 2D avalanche mechanism.

160 Overall, the neuronal avalanche metrics provide a quantitative novel descripti

161 To examine the sensitivity of neuronal avalanche metrics to altered EIB in humans, we focused o

162 ed by analytic and computational dislocation avalanche modelling that we have extended to incorporate

163 ized by a statistical hierarchy of discrete "avalanche" motions described by a power law distribution

164 feedback processes become important, with an avalanche multiplication factor of 4,500.

165 Here, we report avalanche multiplication of the photocurrent in nanoscal

166 to a restricted area of the CM known as the avalanche nucleus (Av).

167 fluctuations of the number of excited atoms (avalanches) obeying a characteristic power-law distribut

168 A new statistical analysis of large neuronal avalanches observed in mouse and rat brain tissues revea

169 he functional linking of cortical sites into avalanches occurs on all spatial scales with a fractal o

170 With the avalanche of biological sequences generated in the post-

171 eported in recent years have revealed a near avalanche of breakthroughs in the melanoma field-breakth

172 Proteomics techniques generate an avalanche of data and promise to satisfy biologists' lon

173 ecent experimental advances are producing an avalanche of data on both neural connectivity and neural

174 200 kb (human cytomegalovirus) leading to an avalanche of data that demanded computational analysis a

175 With the avalanche of DNA sequences generated in the post-genomic

176 as experimental approaches catch up with an avalanche of freely available informatics data.

177 and functions of these enzymes, catalyzed an avalanche of further studies.

178 With the avalanche of genome sequences emerging in the post-genom

179 With the avalanche of genome sequences generated in the post-geno

180 With the avalanche of genome sequences generated in the postgenom

181 With the avalanche of genome sequences generated in the postgenom

182 Faced with the avalanche of genomic sequences and data on messenger RNA

183 The avalanche of genomic sequences generated in the post-gen

184 echniques, discussed here, are generating an avalanche of high-resolution genome-wide data through wh

185 past decade, these advances have yielded an avalanche of metagenomic data.

186 There was an avalanche of new information about hepatitis C virus inf

187 However, the recent avalanche of newly described costimulatory molecules may

188 An avalanche of next generation sequencing (NGS) studies ha

189 With the avalanche of protein sequences emerging in the post-geno

190 ologists is to harness computing and turn an avalanche of quantitative data into meaningful discovery

191 forced to reconsider this definition by the avalanche of reports that molecules and cells associated

192 arly two decades ago helped set in motion an avalanche of research exploring how genomic information

193 In the past decade, an avalanche of research has shown that many real networks,

194 f gastroduodenal disease, which triggered an avalanche of research intended to prove or disprove thei

195 methods for individuals sifting through this avalanche of research to identify the preprints that are

196 Parasite genome projects are generating an avalanche of sequence data.

197 The isolation of graphene has triggered an avalanche of studies into the spin-dependent physical pr

198 interface, we find that slip is nucleated by avalanches of asperity detachments of extension larger t

199 wer-law in the distribution of the lakes and avalanches of discharges.

200 anche shapes, i.e., the temporal profiles of avalanches of fixed duration.

201 r infrared laser pulses produce high density avalanches of low energy electrons via laser filamentati

202 ss Sigmac, the extension and duration of the avalanches of plasticity observed at threshold, and the

203 An analytic model explains these slips as avalanches of slipping weak spots and predicts the obser

204 A simple mean field model for avalanches of slipping weak spots explains the agreement

205 en noise signals and scaling of the critical avalanches of the domain wall motion.

206 ndent substrates may secondarily produce an "avalanche" of aggregation, the observations raise the po

207 An avalanche or cascade occurs when one event causes one or

208 anize themselves into a critical state, with avalanches or "punctuations" of all sizes.

209 By engineering a microwave avalanche oscillator into the laser cavity, which provid

210 evealing the emergence of the self-organized avalanche oscillator: a novel critical state exhibiting

211 We find that a large scale avalanche over the entire network can be triggered in th

212 oscillations coexist with and modulate these avalanche parabolas thereby providing a temporal segment

213 The spatial distribution of avalanching particles appears random, although correlati

214 d to exhibit a higher neural gain and larger avalanches, particularly during interictal epileptiform

215 8% of the mutual information shared by these avalanche patterns were retained.

216 ic statistical fluctuations play in creating avalanches--patterns of complex bursting activity with s

217 roduced 4736 +/- 2769 (mean +/- SD) neuronal avalanches per hour that clustered into 30 +/- 14 statis

218 Here we report the observation of ballistic avalanche phenomena in sub-mean free path (MFP) scaled v

219 at the breakdown originates from a ballistic avalanche phenomenon, where the sub-MFP BP channel suppo

220 tivity, possibly originating from a neuronal avalanching phenomenon.

221 ystems, one system based on a single-photon, avalanche photo-diode array and the other system on a ti

222 Although germanium avalanche photodetectors (APD) using charge amplificatio

223 We use these heterojunctions to fabricate avalanche photodetectors (APDs) with a sensitive mid-inf

224 at is well suited to indium gallium arsenide avalanche photodiode (APD) detectors operated in Geiger

225 ght scattering (DLS) instrument that uses an avalanche photodiode (APD) for recording the scattered i

226 We instead employed a solid-state avalanche photodiode (APD)-based detector for real-time,

227 gnetic field-insensitive, position-sensitive avalanche photodiode (PSAPD) detectors coupled, via shor

228 Single-photon avalanche photodiode (SPAD) array cameras offer single-p

229 A fast avalanche photodiode and a GHz-bandwidth digital oscillo

230 A custom-built avalanche photodiode array is used for detection, permit

231 um oxyorthosilicate crystal arrays and 3 x 3 avalanche photodiode arrays.

232 n be monitored simultaneously using separate avalanche photodiode detectors operating in single photo

233 We use a type of silicon avalanche photodiode in which the lateral electric field

234 d built a MR-compatible PET scanner based on avalanche photodiode technology that allows simultaneous

235 The beta-camera uses a position-sensitive avalanche photodiode to detect charged particle-emitting

236 e 780 nm photons are measured with a silicon avalanche photodiode, and the 3950 nm photons are measur

237 , each monitored by a single-photon counting avalanche photodiode.

238 e fiber bundle was detected by a solid-state avalanche photodiode.

239 Avalanche photodiodes (APDs) are essential components in

240 3)Ga(0.47)As/Al(0.48)In(0.52)As superlattice avalanche photodiodes (InGaAs/AlInAs SL APDs) on InP sub

241 l measurements demonstrate that the nanowire avalanche photodiodes (nanoAPDs) have ultrahigh sensitiv

242 icate (LSO) arrays with 2 position-sensitive avalanche photodiodes (PSAPDs), was developed.

243 While expensive avalanche photodiodes and superconducting bolometers are

244 ing the replacement of photomultipliers with avalanche photodiodes and the need for MRI-based attenua

245 diode lasers (680/780-nm excitation) and two avalanche photodiodes as the basic building blocks.

246 conductor-based flow cytometer that utilizes avalanche photodiodes, wavelength-division multiplexing,

247 s of the lung during inspiration in terms of avalanches propagating through a bifurcating network of

248 onses can in turn have marked effects on the avalanche properties.

249 st that the repetitive formation of neuronal avalanches provides an intrinsic template for the select

250 l spin ice lattices, which occurs through 1D avalanches, quasicrystal lattices undergo reversal throu

251 ) or as components of the endocytic pathway (avalanche, rab5, ESCRT components).

252 se, at moderate dopamine concentrations, the avalanche rate and recurrence of specific avalanches was

253 Computational models based on avalanching recapitulate observed IFT dynamics, and we f

254 mes, as well as between sizes of consecutive avalanches recorded in cortex slice cultures.

255 We propose that avalanches reflect the transient formation of cell assem

256 ly separating the absorption region from the avalanche region via the NOA resulting in single carrier

257 separate conditions have to be met for slab avalanche release.

258 nce between nested oscillations and neuronal avalanches required activation of the dopamine D(1) rece

259 The emergence of avalanches reveals how huddling can introduce correlatio

260 the most accurate model for predicting snow avalanche risk.

261 s - mainly debris and mud flows, landslides, avalanches, rock falls, and (flash) floods - that affect

262 he presence of relativistic runaway electron avalanches (RREA), the same process underlying terrestri

263 to derive an equation governing the average avalanche shape for cascade dynamics on networks.

264 ality demonstrates that nonsymmetric average avalanche shapes (as observed in some experiments) occur

265 n the two-dimensional limit, and the average avalanche shapes are asymmetric.

266 point of the dynamics, the rescaled average avalanche shapes for different durations collapse onto a

267 disciplines, with a recent focus on average avalanche shapes, i.e., the temporal profiles of avalanc

268 cascade of dynamic pressure instabilities -- avalanche 'shocks' -- manifests as negative elastic resi

269 icantly high intrasubject similarity between avalanche size and duration distributions at both cognit

270 This was expressed by the distance between avalanche size and duration distributions of different p

271 riticality and from the power law scaling of avalanche size distribution.

272 Here, we investigate the relation between avalanche sizes and quiet times, as well as between size

273 rheology and non-diffusive bubble motion and avalanches, stems directly from the fractal dimension an

274 ions to organize as scale-invariant neuronal avalanches, suggesting cortical dynamics to be critical.

275 The scale-invariant nature of avalanches suggests that the brain is in a critical stat

276 The analysis of neuronal avalanches supports the hypothesis that the human cortex

277 In particular, we show that an avalanche tends to be larger or smaller than the followi

278 The 2013 Mount Haast rock avalanche that failed from the slopes of Aoraki/Mount Co

279 These nLFPs form neuronal avalanches that are scale-invariant in space and time an

280 e cortex, they arise in the form of neuronal avalanches that capture ongoing and evoked neuronal acti

281 nal activity comprises cascade-like neuronal avalanches that exhibit power-law size and lifetime dist

282 networks undergo rare convulsive movements, "avalanches," that release strain in the network.

283 tterns are organized in the form of neuronal avalanches, thereby maximizing spatial correlations in t

284 The devices show a low avalanche threshold (<1 V), low noise figure and distinc

285 signals arising from multiple photon-induced avalanches to be precisely discriminated.

286 Electron avalanche transfection is a powerful new technology for

287 In chorioallantoic membrane, electron avalanche transfection was approximately 10,000-fold mor

288 d for nonviral DNA transfer, called electron avalanche transfection, was used that involves microseco

289 inal DNA injection and transscleral electron avalanche transfection.

290 tic flows consisting of several catastrophic avalanches under the applied loading.

291 xia, hypercapnia and hypothermia in a buried avalanche victim.

292 he avalanche rate and recurrence of specific avalanches was maximal with recurrence frequencies after

293 d model of computational neuroscience, where avalanching was erroneously attributed to specific neura

294 the scaling exponents of neuronal LRTCs and avalanches were strongly correlated during both rest and

295 lysis revealed that the correlations between avalanches were temporally precise to within +/-4 msec.

296 eling studies suggested that these "neuronal avalanches" were optimal for information transmission, i

297 t-neighbor cages, are interrupted by abrupt "avalanches," where a subset of particles undergo large r

298 atically restricted the size and duration of avalanches, while ketamine allowed for more awake-like d

299 This is characterized by activity "avalanches" whose size distributions obey a power law wi

300 ences of synchronized bursts, named neuronal avalanches, whose size and duration are power law distri