ライフサイエンスコーパス: bubble

1 DNA (ssDNA) in the genome as 'transcription bubbles'.

2 e DNA strand within the paused transcription bubble.

3 een the anterior inferior retina and the gas bubble.

4 ate then forms on the surface of the trapped bubble.

5 scripts, but not ssDNA, at the transcription bubble.

6 nd finally stabilized by an intracameral gas bubble.

7 e perforation and the occurrence of a type 2 bubble.

8 les an evacuated and limb-brightened bipolar bubble.

9 ithin a stalled or backtracked transcription bubble.

10 ually halts due to poor conduction along the bubble.

11 g energy and GC content in the transcription bubble.

12 promoter DNA to stabilize the transcription bubble.

13 pture leaves a collection of small drops and bubbles.

14 on enabled by enzymatic generation of oxygen bubbles.

15 poured into a small vessel to induce surface bubbles.

16 is less prone to blockage by any formed gas bubbles.

17 close to unity, corresponding to 2 mm Mezcal bubbles.

18 dies mostly limited to isolated droplets and bubbles.

19 eas larger bubbles were actually clusters of bubbles.

20 nect the Galactic Centre region to the Fermi bubbles.

21 ransverse elongation of pinned ferrimagnetic bubbles.

22 ies of aquatic sediment due to the ascending bubbles.

23 and PRC2 can recognize R-loops and open DNA bubbles.

24 hickening and 20% localized extraluminal air bubbles.

25 ness, fatty infiltration or extraluminal air bubbles.

26 central few parsecs to the base of the Fermi bubbles(4).

27 in 113 of 155 eyes (72.9%), with 100 type 1 bubbles (88.4%), 11 type 2 (9.8%), and 2 mixed-type (1.8

28 As demonstrated by the nitrogen bubble adhesive force, superhydrophilic measurements, an

29 further affecting the dynamic oxygen (O(2) ) bubbles adsorption on Pt.

30 trate the compounds in foam produced via the bubble aeration of landfill leachate.

31 During the second re-bubbling, an upside-down orientation was observed and so

32 the relationship between an intraocular gas bubble and contact with the retina has been evaluated in

33 nds the DNA duplex to form the transcription bubble and loads the DNA into the RNAP active site.

34 The relationship between the gas bubble and residual vitreous fluid showed a rapid shift

35 Relationship between the gas bubble and residual vitreous fluid.

36 tioning gives better contact between the gas bubble and the inferior and anterior retina than prone p

37 The processes of formation of the bubble and the nanoparticle aggregation are intertwined.

38 Implantation resulted in the formation of He bubbles and an increase in the average size of the Fe gr

39 ed change in the local electric field around bubbles and creases, in agreement with theoretical calcu

40 ding can produce millimeter-sized cavitation bubbles and flow accelerations up to ~ 450 times the acc

41 of rough sea-surfaces, near-sea-surface air bubbles and internal waves.

42 g and diminish the likelihood of information bubbles and polarization.

43 of various thickness of zones denuded in gas bubbles and precipitates, and their relation to the atom

44 mbedded CaCO(3) nanoparticles generate CO(2) bubbles and subsequently disconnect the nanoconjugate, t

45 contrasting interaction between growing gas bubbles and the crystal framework in crystal-rich magma.

46 between decompression rate, retention of gas bubbles, and integrity of the crystal framework leads to

47 tin condensation, cellular swelling with big bubbles, and leakage of cell content, has been proven to

48 ties and volumes of liquid oil droplets, gas bubbles, and two-phase droplet-bubble pairs.

49 ed within grains, while significantly larger bubbles are formed along high-angle grain boundaries (GB

50 Denuded zones (DZ) nearly free from bubbles are found along both high- and low-angle grain b

51 Only type-I and type-II magnetic bubbles are found and images purported to show biskyrmio

52 Viscous bubbles are prevalent in both natural and industrial set

53 promoted, whereas under rapid decompression, bubbles are retained and the crystal framework collapses

54 Bubbles are ubiquitous in the natural environment, where

55 shing, masks, social distancing, and "social bubbles" are used to limit community transmission, but i

56 Replication foci, or 'bubbles,' are identified by the presence of the incorpor

57 entrapped air evolves into single or double bubbles, as determined by competition among inertia, cap

58 Predicting a bubble ascent scenario in muddy sediment will further al

59 ffective overburden loads induce only stable bubble ascent, which stops at the gas horizon frequently

60 bubble to the lower index material inside a bubble at appropriate angles of incidence, which can lea

61 here in nature, from foams to submillimetric bubbles at a free surface, and their rupture leaves a co

62 PMA) were produced from seawater by bursting bubbles at two biologically productive and two oligotrop

63 the effect of air injection depth in the big-bubble (BB) technique, which is used for corneal tissue

64 theoretical modeling and characterization of bubble behavior, we propose a bubble-free microfluidic P

65 This ultimately leads to the bubble being released to the water column.

66 ties are consistent with the presence of gas bubbles beneath the water table under valley and ridge.

67 were used: video (DVD; n = 27), playing with bubbles (Bubbles; n = 67), and music accompanied by inst

68 Bubble burst occurred in 1/16 cases of type I BB and 3/1

69 For higher or lower alcohol content, the bubbles burst rapidly.

70 water was drastically different from that of bubble-bursting aerosols from the tank experiments-sugge

71 using a marine aerosol generation tank-five bubble-bursting experiments (with contrasting incubation

72 , Acta Mater. 144, 561-578 (2018)] for small bubbles, but the current model uses no adjustable parame

73 ) top layer that minimizes the generation of bubbles by inhibiting mass transport along a vertical di

74 he T7 promoter contained in the enlarged DNA bubble can be melted and transcribed by the bound RNAPs

75 ribed by the bound RNAPs as the enlarged DNA bubble can help the separation of the two DNA strands, d

76 filaments within and in the vicinity of the bubble cavities.

77 o create a UV light beam from aspherical air bubble collapse near a gallium-based liquid-metal microp

78 Subsequently, the bubble collapses and releases metastable He[Formula: see

79 However, because a spherical bubble collapsing in the bulk of water creates isotropic

80 Certain NP-in-bubble configurations can lead to the optical pulling of

81 Non-invasive bubble continuous positive airway pressure (bCPAP) is co

82 rast scores were assessed by agitated saline bubble counts, and separately by appearance of 25-um mic

83 rface gravity waves and near-sea-surface air bubbles decorrelate acoustic signals over seconds or les

84 inates and the single layer Fe film, but the bubble density and grain size were found to be smaller i

85 s of individual layers in the nanolaminates, bubble density and grain size were further decreased.

86 nt a theoretically-motivated model of helium bubble density as a function of volume for high-pressure

87 o the nuclease Bax1 and their complex with a bubble DNA having one arm unwound in the crystal.

88 main walls, closure domains, polar vortices, bubble domains, and polar skyrmions) and their emergent

89 Combined with constraints on bubble-driven ebullitive fluxes, we place total oceanic

90 Our findings have important implications for bubble/drop generation in microfluidic devices, with app

91 verall shape, since the outer shell of these bubble droplets consist of a low-viscosity monomer that

92 justing the gas pressure used to produce the bubble droplets.

93 Using an in-situ camera, bubble dynamics at the source were measured every 6 h ov

94 e-resolved photography to measure cavitation bubble dynamics generated by the delivery of focused 500

95 ed data to a theoretical model of cavitation bubble dynamics in a Neo-Hookean viscoelastic medium sub

96 e and the direct spatial mapping of isolated bubble echos, for which both find excellent agreement wi

97 t from the angle between the current and the bubble elongation directions.

98 Nanostructured cellulose fabric with an air-bubble-enhanced anti-oil fouling property is introduced

99 a we call the no-open-edge condition and the bubble equivalence.

100 vation of enzyme-induced vacuole-formation ("bubbling") events, which can only occur through enzyme i

101 gative impacts such as Joule heating and gas bubble evolution from common nanosecond pulse treatment

102 complex likely reflects the state of repair bubble extension by the XPB and nuclease machine.

103 reventing DNA incision by Bax1 during repair bubble extension.

104 cutive cases of keratoconus treated with big-bubble F-DALK from August 1, 2015, to September 1, 2018

105 ervations have revealed the so-called 'Fermi bubble' features(4), implying that our Galactic Centre h

106 integrity of perforated fluid films, such as bubble films and biological membranes, as well as fundam

107 perforation (OR = 6.09, P = .03), and type 2 bubble formation (OR = 14.17, P < .001).

108 h a single pore to study the dynamics of gas bubble formation and evolution.

109 lectrochemical reactions resulted in surface bubble formation and near-surface pH modulation that dec

110 the difference and predicts that peeling and bubble formation do not occur in overstretching double-s

111 ges of keratoconus were predictors of type 2 bubble formation during BB-DALK that was associated with

112 ME performed in narrow channels/tubing where bubble formation is critical.

113 We found that the laser pulses induce bubble formation on the surface of a nanoparticle and a

114 s were significantly higher in eyes in which bubble formation succeeded (respectively, P = .006 and P

115 ntraoperative central DM perforation, type 2 bubble formation, and presence of scar in keratoconic an

116 e oil droplets within 14.5 min, prior to gas bubble formation, during the experiments of Pesch et al.

117 /nanofluidic device was employed for a micro bubble formation, plasma negation and penetration of the

118 rane perforation, the rate of successful big-bubble formation, suture-related complications, and graf

119 found beneficial by eliminating detrimental bubble formation.

120 5 bar pressure to avoid complications due to bubble formation.

121 We investigate the stability of gas bubbles formed at saturated (bubble-point) conditions du

122 Type 1 bubbles formed in eyes with significantly lower age, K-m

123 r droplet encapsulated by a larger air shell bubble, forming an antibubble.

124 interband transition, a void nanometer-sized bubble forms around the localized excitation (He[Formula

125 h powered Peltier-based thermal cycler under bubble-free conditions.

126 t allow efficient H(2) supply on demand in a bubble-free form.

127 cterization of bubble behavior, we propose a bubble-free microfluidic PCR device via controlled fluid

128 However, the underlying physics of how bubbles freeze has not been studied.

129 trast, videographers have shown that as soap bubbles freeze, a plethora of growing ice crystals can s

130 Here, we characterize the physics of soap bubbles freezing on an icy substrate and reveal two dist

131 ractions (0.27 < nu < 0.4) of near-spherical bubbles from a fracturing regime supporting reduced void

132 mode, occurring for isothermally supercooled bubbles, generates a strong Marangoni flow that entrains

133 f the major drawbacks of microfluidic PCR is bubble generation and reagent evaporation, which can cau

134 he molecular level cavitation mechanisms and bubble growth kinetics in soft gelatin hydrogel and wate

135 calculations reveal that the polar-skyrmion bubbles have a skyrmion number of +1, and resonant soft-

136 for the lowest irradiation temperature, gas bubbles have the shape of thin hexagonal prisms with ave

137 ive negative co-movements around the Dot.com bubble in 2001 as well as the Global Financial Crisis (G

138 Surprisingly, however, the pinch-off of a bubble in a large tank of viscous liquid is known to be

139 A control model containing a 5 nm bubble in pure water is also created.

140 tiation state and the complete transcription bubble in the elongation state.

141 Total internal reflection from air bubble in water is one of the few sources of elliptical

142 e is associated with the onset of cavitation bubbles in a cell culture chamber and (2) the dynamics o

143 ng the lithium-water reaction kinetics using bubbles in a channel.

144 we discover room-temperature polar-skyrmion bubbles in a lead titanate layer confined by strontium t

145 llition); spring release of CH(4) trapped in bubbles in and under the ice during fall freeze (bubble

146 We also show that surface gravity waves and bubbles in high sea states can cause increasingly signif

147 function of volume for high-pressure helium bubbles in plasma-facing tungsten.

148 e chamber and (2) the dynamics of cavitation bubbles in the chamber induces localized compressive/ten

149 roduced by a blast can generate micron-sized bubbles in the tissue.

150 Stationary and dynamic scenes of air bubbles in water in both indoor and outdoor settings are

151 Here, we explore how gas bubbles in water subjected to a thermal gradient, a like

152 ht from acoustically-induced collapse of air bubbles in water, is an efficient means of generating UV

153 .3 Tg from spring release of CH(4) stored in bubbles in winter lake ice.

154 op 22 teams isolated together (known as the "bubble") in Orlando, Florida to play eight games each as

155 etracting forces, and trapped multiscale air bubbles increasing the buoyancy and backpressure for an

156 Since bubbles induce a phase shift of opposite sign to that of

157 mFRET) and cleavage assays, we show that DNA bubbles induce off-target binding and cleavage at these

158 0.04-0.5 mg L(-1) while still being prone to bubble-induced fluctuations and suffering from considera

159 When compared to bolus injections, a bubble infusion offers a more controlled and consistent

160 Herein, we show that bubble infusions were able to achieve consistent BBB ope

161 acheal trunks (DTTs) by the expulsion of gas bubbles into the body.

162 pts duplex DNA at internal unpaired regions (bubbles) into strongly bent structures, and suggest how

163 The pinch-off of a bubble is an example of the formation of a singularity,

164 In liquid, cavitation bubble is created when surrounding pressure drops below

165 d inside its internal body cavity, where the bubble is resonated using acoustic waves.

166 A high number density of small bubbles is observed within grains, while significantly l

167 problems for which the stability of surface bubbles is of importance, such as bio-foams, froth float

168 To test if the attachment on fluid bubbles is strong enough to efficiently float magnetite

169 The honeycombed network of bubbles is supported by glassy threads and forms a struc

170 suggest how XPG complexes may bind both NER bubble junctions and replication forks.

171 These bubbles, known as pearls by the Mezcal artisans, remain

172 flux, and the individual characterization of bubbles larger than 1.50-1.72 mm in diameter.

173 s higher than 10 mg CO(2) m(-2) h(-1) and of bubbles larger than 5.3-8.4 mm in diameter.

174 The long bubble lifetime is the result of surfactant-induced surf

175 The dimensionless bubble lifetime was found to reach its maximum value whe

176 f surfactants are all relevant to extend the bubble lifetime.

177 search to take place within a migrating DNA bubble-like structure that is bound by replication prote

178 August 1, 2015, to September 1, 2018 and big-bubble M-DALK from September 1, 2012, to September 30, 2

179 ations were managed conservatively in type 1 bubbles; macroperforations occurring in both types of bu

180 Bubbles may nucleate below the water table because water

181 A coupled macroscopic single-bubble mechanical/reaction-transport numerical model was

182 The bubble-mediated link between the benthic and pelagic env

183 A simple budget approach showed that this bubble-mediated transport has the potential to maintain

184 These findings demonstrate that the bubble-mediated transport of microorganisms influences t

185 It is shown that the bubble migration scenario is managed predominantly by in

186 expected to pose a problem to efficient DNA bubble migration.

187 nanobubble concentration within 10(9)-10(11) bubbles/ml.

188 : video (DVD; n = 27), playing with bubbles (Bubbles; n = 67), and music accompanied by instruments (

189 actant analyte to affect the electrochemical bubble nucleation and then transduces the change in nucl

190 recent studies revealed heterogeneous fluid bubble nucleation on oxide minerals such as magnetite du

191 We present the first bubble-nucleation-based electrochemical method for the s

192 eled a gel like structure with a preexisting bubble of 5 nm radius.

193 served the Galactic Centre lobe, an apparent bubble of emission seen only at positive Galactic latitu

194 In this process, many bubbles of carbon dioxide are instantly formed in the sa

195 t YaaA binds to dsDNA, duplex DNA containing bubbles of unpaired nucleotides, and Holliday junction c

196 Wettability alteration and bubble-oil pinch-off were identified as contributing mec

197 reasoning for the abundant formation of gas bubbles on intermetallic precipitates, observation of va

198 Recent studies of individual gas bubbles on nanoelectrodes have resulted in unprecedented

199 estigate the mechanisms of nucleation of gas bubbles on nanoelectrodes, and characterize their statio

200 ldom give rise to emergent phenomena such as bubbles or crashes.

201 The net fluidic flow due to the bubble oscillation orients the microrobot's axisymmetric

202 The results demonstrate that magnetite-bubble pairs do ascend in silicate melt, accumulating in

203 droplets, gas bubbles, and two-phase droplet-bubble pairs.

204 self-similar regime restores universality to bubble pinch-off by erasing the system's memory of the i

205 Here, we consider bubble pinch-off in a turbulent flow representative of n

206 sues to be free of imaging artefacts such as bubbles, pixel saturation, organ specularity and debris,

207 We present a new model of bubble (plume) dynamics, advection-dispersion of dissolv

208 thickening and several focal intramural gas bubbles (pneumatosis intestinalis) surrounding the polyp

209 tability of gas bubbles formed at saturated (bubble-point) conditions during two-component ([Formula:

210 Increased connectivity of the bubble population appeared highly significant in limitin

211 e distribution and connectivity of spherical bubble populations, with narrow sedimentary pore throats

212 lex (IC), the template in the expanded 7-mer bubble positions the RNA and NTP analog UTPalphaS, while

213 MP), through investigation of gas exsolution bubbles preserved by melt inclusions.

214 as release or by dissipating excess internal bubble pressure, thereby diminishing further growth.

215 n scenario is managed predominantly by inner bubble pressure, which defines a bubble solute exchange

216 ation and sequestration of CO(2) into vapour bubbles, producing spurious barometric estimates.

217 WS(2)/Pt and MoS(2)/Pt bubble propelled micromotors are used as "on-the-fly" se

218 ng from tailor-made motile bacteria and tiny bubble-propelled microengines to hybrid spermbots, can b

219 same rate of production of gas, but distinct bubble properties, suggests that these dissipative syste

220 stopped-flow operations as well as efficient bubble propulsion (1% H(2)O(2), 1,5% NaCh, speed 140 mum

221 d PtNPs inner catalytic layer (for catalytic bubble propulsion).

222 ersy about where XPA is bound within the NER bubble, provide structural insights into the molecular b

223 w electron beam dose rate generates hydrogen bubbles, providing a reservoir of sacrificial reductant.

224 o an explosive-like rapid production of H(2) bubbles, providing the necessary force to breach dermal

225 The bubbles rapidly extract and liberate volatile compounds

226 Overall re-bubbling rates were comparable in both groups.

227 s and at 1, 2, and 3 years' follow-up and re-bubbling rates.

228 in a scenario where no teams travel (restart bubble) reduces the typical effects of travel and home-c

229 les in and under the ice during fall freeze (bubble release), and diffusion of CH(4) from sediments t

230 del scenarios suggest that 5 mm diameter gas bubbles released at a <470 m water depth can transport m

231 is emitted from lakes by several processes: bubbles released from bottom sediments that reach the at

232 m the sediment into the water column via gas bubbles released from the seabed was documented.

233 macroperforations occurring in both types of bubbles required conversion to MK.

234 d a lack of postoperative OCT data after gas bubble resolution.

235 he depth of the gas horizon increases, while bubble rise velocity decreases with an increase in the o

236 ept up the surrounding material to create a 'bubble' roughly four parsecs in diameter with a 2,600-so

237 pse and wrinkling arise independently of the bubble's orientation.

238 Saline contrast bubble score was associated with microsphere shunt (rho

239 group investigated with transcranial Doppler bubble screen.

240 few repeated contacts akin to forming social bubbles; seeking similarity across contacts; and strengt

241 e complex flow field induced by the deformed bubble shape.

242 In principle, a cavitation bubble should continue to grow as long as tensile pressu

243 ystem was distinctly more robust against gas bubbles, showed a higher signal gain, and allowed us to

244 singly, the dependence of the phase shift on bubble size indicates that only those with 0.15-0.20 mum

245 The average bubble size reached a value as small as 6.5 mum at a she

246 To refine the bubble size, foams were further sheared in a Couette's c

247 oral variability of seep dynamics, including bubble size, rise velocity, composition, and upwelling a

248 eating polymer foams with locally programmed bubble size, volume fraction, and connectivity is report

249 acking, whereas high GC in the transcription bubble slows elongation.

250 ly by inner bubble pressure, which defines a bubble solute exchange with ambient porewaters.

251 rsistent substructure characterized by inter-bubble spacings similar to those observable when the gas

252 phases such as the dipolar maze and the nano-bubble state have been appraised as essentially distinct

253 report radio imaging that reveals a bipolar bubble structure, with an overall span of 1 degree by 3

254 Bubble structures between each microneedle and the patch

255 in determining size and structure of the gas bubble superlattice as a function of irradiation conditi

256 ngs similar to those observable when the gas bubble superlattice has formed with very large ordering

257 To understand the formation of the void/gas bubble superlattices in crystals under irradiation, we e

258 on the formation and structure of helium gas bubble superlattices within a tungsten host matrix to un

259 presence of crystalline particles at the air bubble surface and in bulk.

260 s (PMA) at the sea surface via modulation of bubble surface tension.

261 A "Bubbles" technique was used to identify which areas of t

262 The dynamic oxygen-bubble template (DOBT) programmably controlled by a squa

263 is likely applicable to significantly larger bubbles than the ones examined here, and its assumptions

264 racellular vesicles (sEV), membrane-enclosed bubbles that carry signaling molecules, from senescent s

265 Otherwise, all gas bubbles that form undergo, possibly oscillatory, growth

266 the nontemplate strand of the transcription bubble to drive promoter melting.

267 e higher refractive index material outside a bubble to the lower index material inside a bubble at ap

268 ly, a sub laser spot was focused next to the bubble to yield a temperature gradient in the direction

269 We estimate the age of the bubbles to be a few million years, with a total energy o

270 ultrasound (CEUS) uses shell-stabilized gas bubbles to provide acoustic backscatter in vasculature.

271 used to explore the ascent of a mature CH(4) bubble toward the seafloor in muddy aquatic sediment.

272 The sensor combines a traditional funnel bubble trap with an Arduino logger, a pressure sensor, t

273 t-shaped microrobot contains a spherical air bubble trapped inside its internal body cavity, where th

274 diagnostic power for discrimination between bubble types, followed by AS-OCT stage, pachymetry, K-me

275 ntrol of flow direction around a water vapor bubble using the thermoplasmonic effect of a gold nanois

276 show biskyrmions can be explained as type-II bubbles viewed at an angle to their axes.

277 A controlled glass bubble volume concentration from 0 to 70% leads to a sel

278 The recent bust of the Blockchain bubble was detrimental to many projects intended to retu

279 mination of the size and symmetry of the gas bubbles was performed using a combination of small angle

280 rains in the form of "fingers" and "granular bubbles." We demonstrate that this RT-like instability a

281 dius were individual bubbles, whereas larger bubbles were actually clusters of bubbles.

282 No He bubbles were observed in the SiOC layers of the nanolami

283 asound (US) guidance allowed by BH-generated bubbles were previously demonstrated ex vivo and in vivo

284 rnal reflection occurs at the interface of a bubble, where light travels from the higher refractive i

285 se with 0.15-0.20 mum radius were individual bubbles, whereas larger bubbles were actually clusters o

286 tional instabilities: the rise of a granular bubble which leaves a trail of particles behind it and t

287 smon resonance peak can generate a nanoscale bubble, which can encapsulate the NP (i.e., supercavitat

288 he intrinsic degradation is masked by oxygen bubbles, which are inherently being formed during the re

289 uctural modification is the formation of gas bubbles, which is revealed at all studied irradiation te

290 quently, rapid flow was generated around the bubble, whose flow direction was dependent on the power

291 In the stable spiral case gas bubbles will achieve a steady-state finite size only if

292 nd other barriers to transmission, or social bubbles will be most effective.

293 NF immersed in degassed water, a water vapor bubble with a diameter of ~10 mum is generated.

294 Numerical simulations predict that the oily bubbles with diameters larger than 8 mm reach the surfac

295 w sedimentary pore throats promoting coarser bubbles with diminished connectivity.

296 the sudden, unstable expansion of a void or bubble within a liquid or solid subjected to a negative

297 viable optical coating by integrating glass bubbles within a polymer film.

298 ion of sodium 1-(13) C-acetate, parahydrogen bubbling within a microtesla magnetic field (i.e. under

299 Direct bubble writing relies on rapid generation and patterning

300 manufacturing method, referred to as direct bubble writing, for creating polymer foams with locally