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 -invariant spatiotemporal clusters, neuronal avalanches.

6 on leads to a different subsequent series of avalanches.

7 across many spatial scales, termed neuronal avalanches.

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

9 natural to focus on the attributes of these avalanches.

10 t which ongoing activity emerges as neuronal avalanches.

11 us monkeys carries the signature of neuronal avalanches.

12 clusters in space and time, called neuronal avalanches.

13 described by the same equations that govern avalanches.

14 tworks is described by equations that govern avalanches.

15 g state in the presence of cortical neuronal avalanches.

16 mporal cascades of activity, termed neuronal avalanches.

17 cooling and large-scale, inward propagating avalanches.

18 iant, cascades of activity known as neuronal avalanches.

19 cal branching process that produces neuronal avalanches.

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

36 Neuronal avalanches are a type of spontaneous activity observed i

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

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

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

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

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

42 Neuronal avalanches are spatiotemporal patterns of neuronal activ

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

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

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

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

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

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

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

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

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

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

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

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

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

56 whether the device improves survival during avalanche burial.

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

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

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

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

61 The avalanches collected during interictal epileptiform acti

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

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

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

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

66 Silicon single-photon avalanche detectors are becoming increasingly significan

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

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

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

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

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

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

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

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

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

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

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

78 cooperative rearrangements of displacements (avalanches) diverges.

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

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

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

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

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

84 Avalanching dynamics are studied in many disciplines, wi

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

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

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

88 In vitro spike avalanches emerged naturally yet required balanced excit

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

141 200 kb (human cytomegalovirus) leading to an avalanche of data that demanded computational analysis a

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

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

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

145 With the avalanche of genome sequences generated in the postgenom

146 With the avalanche of genome sequences generated in the postgenom

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

175 8% of the mutual information shared by these avalanche patterns were retained.

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

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

178 tivity, possibly originating from a neuronal avalanching phenomenon.

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

180 Although germanium avalanche photodetectors (APD) using charge amplificatio

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

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

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

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

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

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

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

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

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

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

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

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

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

194 Avalanche photodiodes (APDs) are essential components in

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

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

197 While expensive avalanche photodiodes and superconducting bolometers are

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

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

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

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

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

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

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

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

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

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

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

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

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

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

212 The emergence of avalanches reveals how huddling can introduce correlatio

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

232 Electron avalanche transfection is a powerful new technology for

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

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

235 inal DNA injection and transscleral electron avalanche transfection.

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

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

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

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

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

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

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

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

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