ライフサイエンスコーパス: condensate

1 on (the hallmark of superfluid Bose-Einstein condensates).

2 e. the formations with and without film-like condensate.

3 um coherent state similar to a Bose-Einstein condensate.

4 bridges across the population of supercooled condensate.

5 herent exciton-photon transformations in the condensate.

6 s a collective polaron formed by a polariton condensate.

7 of such monopoles in a spin-1 Bose-Einstein condensate.

8 tic field produced by a spinor Bose-Einstein condensate.

9 particle velocities made after releasing the condensate.

10 in any superfluid, atomic-gas Bose-Einstein condensate.

11 s, at the termini of vortex lines within the condensate.

12 nsional and nonequilibrium characters of the condensate.

13 distances, as expected for a two-dimensional condensate.

14 ution in momentum space, characteristic of a condensate.

15 ed DNA via formation of a bright spot or DNA condensate.

16 sympathetic cooling of the single ion by the condensate.

17 appearance of vortices in our Bose-Einstein condensate.

18 th density wave and a short-coherence-length condensate.

19 enhancement by self-shedding and sweeping of condensate.

20 ion of the valence electrons into an exciton condensate.

21 ts stem from the quantum fluctuations of the condensate.

22 ter-wave soliton trains from a Bose-Einstein condensate.

23 pair-breaking speed limit of superconducting condensate.

24 ntum fluids, hydrodynamics and Bose-Einstein condensates.

25 mixture of the monomer melem and its higher condensates.

26 nating from the two distinct superconducting condensates.

27 re bosonic and may give rise to new types of condensates.

28 her measures of quantum turbulence in atomic condensates.

29 erging field of quantum turbulence in atomic condensates.

30 s, polymer mixtures and binary Bose-Einstein condensates.

31 such as superfluid helium and Bose-Einstein condensates.

32 LCs), Langmuir monolayers, and Bose-Einstein condensates.

33 (LPA)-generating enzyme in embryonic dermal condensates.

34 be ideal systems to study out-of-equilibrium condensates.

35 ting new states of matter with Bose-Einstein condensates.

36 as well as in the screening of tobacco smoke condensates.

37 development and have small or absent dermal condensates.

38 perfluids, liquid crystals and Bose-Einstein condensates.

39 aves, spin density waves and superconducting condensates.

40 rns of collagen alignment around and between condensates.

41 e lattice of 45 coherently coupled polariton condensates.

42 ed tissue forms from patterns of mesenchymal condensates.

43 b the flow and dynamics of exciton-polariton condensates.

44 ids, fibre optics, plasmas and Bose-Einstein condensates.

45 chaos, polymers and turbulent Bose-Einstein condensates.

46 ma MCP-1 on day 3 and reduced exhaled breath condensate acidification.

47 Shaking the lattice drives condensates across an effectively ferromagnetic quantum

48 charge fractionalization in a Bose-Einstein condensate, all of which are not possible with conventio

49 This type of macroscopic polariton ring condensate allows for the possibility of direct control

50 The digit pre-chondrogenic condensates also become wider, thicker and shorter.

51 14053 demonstrate that isotopically light Zn condensates also occur on some mare basalts after their

52 rly screening methods such as exhaled breath condensate analysis and low dose computed tomography (CT

53 f a freely expanding turbulent Bose-Einstein condensate and a propagating optical speckle pattern.

54 crossover between a molecular Bose-Einstein condensate and a superfluid with BCS (Bardeen-Cooper-Sch

55 Biomarkers in exhaled breath condensate and airway resistance (pre- and post- broncho

56 s, and commercial products, along with smoke condensate and ash from these samples.

57 l quantum billiard for the exciton-polariton condensate and demonstrate a diabolical point in the spe

58 th various doses of nicotine and e-cigarette condensate and determined myofibroblast differentiation,

59 We create a large exciton-polariton condensate and employ a Michelson interferometer setup t

60 terize the amplitude excitations in a spin-1 condensate and measure the energy gap for different phas

61 the quantum coherence of the superconducting condensate and render the wire slightly resistive (i.e.,

62 Condensate and stormwater contained numerous carcinogeni

63 bulk defeats the adhesive force between the condensate and the solid surface triggers the self-shedd

64 fresh approaches to the creation of quantum condensates and crystals.

65 Neutral atomic Bose condensates and degenerate Fermi gases have been used to

66 s coordinated signal exchange between dermal condensates and placode stem cells.

67 Although toroidal DNA condensates and vesicles with different numbers of handl

68 in the loss of the DP precursor, the dermal condensate, and a stage 2 hair follicle arrest phenotype

69 e is too weak to deplete the superconducting condensate, and for cuts inside the Fermi arc region.

70 t of bitumen, it is diluted with natural gas condensate, and the resulting mixture, "dilbit", differs

71 ratchet by the apical and junctional myosin condensates, and an external one by the supracellular ac

72 At 0.5 K, the pair condensate appears to adjust to the 3D CDW by a sharp tr

73 Biomarker measurements in exhaled breath condensate are the least well-validated techniques.

74 ine lung surfactant and human exhaled breath condensate are used as first-order surrogates for infect

75 crystals and therefore both superconducting condensates are expected to be pushed deep into the type

76 The TH/siRNA condensates are formulated into a core-membrane structur

77 roaching the Mott density, exciton-polariton condensates are generally thought to revert to a standar

78 parated and provide evidence that the higher condensates are isolated oligomers of melem.

79 Polariton condensates are macroscopic quantum states formed by hal

80 s sufficient concentration of IP-(S)-proline condensate, as this chiral reactive intermediate becomes

81 o anionic nucleic acids, forming more stable condensates, as demonstrated by the binding affinity ass

82 ecrosis Factor-alpha level in exhaled breath condensate at week 12.

83 to account for contributions from gases and condensates at initial leak source conditions.

84 rate the realization of an organic polariton condensate, at room temperature, in a microcavity contai

85 ffer (BCS) and strong-coupling Bose-Einstein condensate (BEC) limits gives a unified framework of qua

86 d states in a harmonic trapped Bose-Einstein condensate (BEC), which resembles the long-sought Dicke

87 elongated [Formula: see text] Bose-Einstein condensates (BECs) and showed that a dilute background o

88 Bose-Einstein condensates (BECs) composed of polarons would be an adva

89 y bound, large Cooper pairs to Bose-Einstein condensates (BECs) of tightly bound molecules.

90 Spin-orbit-coupled Bose-Einstein condensates (BECs) provide a powerful tool to investigat

91 superconductivity with that of Bose-Einstein condensates (BECs).

92 lution is insufficient to directly observe a condensate before the growth of a bulk crystal.

93 ing SC/CDW composite order above to a SC/CDW condensate below.

94 to directly control the spin of a polariton condensate, bias-tuning the emission polarization.

95 precisely control the structure of the petal condensates both by carefully modifying the excitation g

96 y the metabolomic approach to exhaled breath condensate (breathomics) to discriminate different asthm

97 s the transition on a given quench time, the condensate builds up with a delay that can be deduced us

98 is two-fold: (1) that the external force on condensate bulk defeats the adhesive force between the c

99 e to the timely suppression over the growing condensate bulk on the condensing surface through the se

100 fluid, which are time-independent, while the condensate bulk thermal resistance depends on the conden

101 condensation and holds afterwards while the condensate bulk thermal resistance gradually takes over

102 tition mechanism suggests that only when the condensate bulk thermal resistance is reduced after it t

103 nsic competition between the interfacial and condensate bulk thermal resistances in timeline and the

104 strengths) in a neutral atomic Bose-Einstein condensate by dressing two atomic spin states with a pai

105 vortices in trapped dilute-gas Bose-Einstein condensates by repeatedly imaging the vortex cores.

106 The condensate can be observed at room temperature.

107 m cells is essential for induction of dermal condensates, cell clusters of precursors for the hair fo

108 ryonic hair follicle (HF) placode and dermal condensate cells, precursors of adult HF stem cells and

109 he Hh pathway, was impaired in mutant dermal condensate cells, suggesting that Gorab may be required

110 Condensate completely dissolved Daphnia magna within 24

111 a gapless spin liquid) to the Bose-Einstein condensate (corresponding to a magnetically ordered phas

112 n mice, paternal exposure to cigarette smoke condensate (CSC) causes molecular defects in germ cells

113 normal media with or without cigarette smoke condensate (CSC) for up to 9 months under potentially re

114 Cigarette smoke condensate (CSC) is comprised of thousands of chemicals.

115 Cigarette smoke condensate (CSC) is the particulate matter of cigarette

116 f esophageal cancer cells to cigarette smoke condensate (CSC) led to upregulation of the xenobiotic p

117 e investigated the effect of cigarette smoke condensate (CSC) on the characteristics of monocyte-deri

118 We examined the effect of CS condensate (CSC) or extract (CSE) on signal transduction

119 studies, we have shown that cigarette smoke condensate (CSC), a surrogate for cigarette smoke, is ca

120 nchial epithelium exposed to cigarette smoke condensate (CSC), and alteration of mir-218 levels in th

121 normal media with or without cigarette smoke condensate (CSC).

122 n the presence or absence of cigarette smoke condensate (CSC).

123 ons is about five per cent of the background condensate density and their form factor exhibits primar

124 identified from spin-resolved images of the condensate density profile that exhibit a characteristic

125 Experimental observations show that the condensate droplet jumping is induced by coalescence of

126 ttering resonance causes the increase of the condensate droplet radius without affecting the condensa

127 Coalescence-induced jumping of condensate droplets from a superhydrophobic surface with

128 significant changes in the behaviour of the condensate due to the curvature of the dispersion relati

129 Collection of exhaled breath condensate (EBC) and quantification of biomarkers in bre

130 xide measurement, spirometry, exhaled breath condensate (EBC) collection.

131 sought to investigate whether exhaled breath condensate (EBC) lipoxin and leukotriene measurements ca

132 Exhaled breath condensate (EBC) metabolite profiles also correlated wit

133 ccessible body fluids such as exhaled breath condensate (EBC), saliva, urine, and blood has not been

134 ally accepted H2O2 content in exhaled breath condensate (EBC), with the sensitivity of 8 A M(-1) cm(-

135 resulting in virions that contain "eccentric condensates," electron-dense aggregates located outside

136 The temporal patterns of the condensate emission result from the intrinsic disorder a

137 densate, generating ultrashort pulses of the condensate emission.

138 most all currently proposed hyperon or boson condensate equations of state (M(middle dot in circle),

139 te to the establishment of many biomolecular condensates, eukaryotic cell structures that concentrate

140 milar molecular responses to cigarette smoke condensate ex vivo and in vivo.

141 re condensate vortex and defect disorder and condensate excitations.

142 Biomarkers in exhaled breath condensate, exhaled volatile organic compounds (VOCs), g

143 nce of dissipation the relative phase of two condensates exhibits non-equilibrium PT from the quantum

144 e solid surface in dropwise mode or thin the condensate film on the solid surface in filmwise mode, w

145 me high-emitting operations occur by design (condensate flashing and liquid unloadings), they occur m

146 uring the quasimomentum of the Bose-Einstein condensate for different velocities and strengths of the

147 e 15 when osteochondrogenic mesenchyme forms condensates for each plastron bone at the lateral edges

148 ding inability to specifically target dermal condensates for gene ablation.

149 way for the application of coupled polariton condensates for the realisation of a quantum annealing a

150 , the ability of ALLINIs to induce eccentric condensate formation required both IN and viral RNA.

151 ntails a relaxation oscillation in polariton condensate formation, resulting in ultrafast emission pu

152 NA is necessary for ALLINI-induced eccentric condensate formation.

153 the excess heat, and allowing Bose-Einstein condensate formation.

154 In contrast, the condensate formed in the uniform GaN nanowire-dielectric

155 densate droplet radius without affecting the condensate fraction inside it.

156 er decays to zero exponentially although the condensate fraction remains finite.

157 -lipoxin-A4 was identified in exhaled breath condensate from LAM subjects and was increased by aspiri

158 fying whether metabolomics of exhaled breath condensate from obese asthmatic (OA) patients, lean asth

159 fying whether metabolomics of exhaled breath condensate from obese asthmatic (OA) patients, lean asth

160 usand), and high U/Pb supports the origin of condensates from a volatile-poor internal source formed

161 efractory minerals predicted to be the first condensates from the solar nebula.

162 rily emptied by stimulated scattering to the condensate, generating ultrashort pulses of the condensa

163 Because they are spinor condensates, half-quanta are allowed in where there is a

164 t determines the final expanse of the frozen condensate halo, which, in turn, controls frost formatio

165 e show that (4)He atoms in the Bose-Einstein condensate have environment significantly different from

166 Eccentric condensates have a high NC content, as demonstrated by "

167 the polariton lasing generated by dynamical condensates have received considerable attention in rece

168 vious experiments on colliding Bose-Einstein condensates have revealed matter-wave interference, halo

169 mions is prepared along with a Bose-Einstein condensate in a shallow three-dimensional optical lattic

170 We prepare a Bose-Einstein condensate in an optical box, drive it out of equilibriu

171 ormation of a near-equilibrium Bose-Einstein condensate in the GaN region of the nanowire at room tem

172 itions, cavity polaritons form a macroscopic condensate in the ground state.

173 measures the temperature of a Bose-Einstein Condensate in the sub-nK regime.

174 We test this symmetry based on Bose condensates in a shaken optical lattice.

175 f a Tonks-Girardeau gas and of Bose-Einstein condensates in different dimensions, where the method ex

176 makes it possible for the system to have two condensates in momentum space.

177 we report the spontaneous formation of such condensates in programmable potential landscapes generat

178 the localized states of atomic Bose-Einstein condensates in this strip; via excitation dynamics, we f

179 ed hedgehog (Hh) signaling pathway in dermal condensates in vivo.

180 nbiogenic origin, such as comet impact plume condensates in what may be very rapidly deposited CIE cl

181 and contrast this to the case of a repulsive condensate, in both cases finding excellent agreement wi

182 A549 cell exposure to cigarette smoke condensate increased these enhancer marks significantly

183 nstein magnon condensate: the density of the condensate increases immediately after the external magn

184 uilibrium dynamics of a spin-1 Bose-Einstein condensate initialized as a minimum uncertainty spin-nem

185 Sox2(+) dermal condensates initiate normally; however by E16.5 guard ha

186 without affecting DNA dissociation from DNA condensates inside the cytoplasm should be a perfect car

187 will return to the macroscopically occupied condensate instead of entering any other state.

188 coupling achieved by loading a Bose-Einstein condensate into periodically driven optical lattices.

189 the activator of the yeast AMP kinase Snf1, condensates into granules to tune Snf1 activity.

190 techniques to determine the temperature of a condensate involve an indirect estimation through mean p

191 produced by numerical simulations, where the condensate is coupled to the excitonic reservoir describ

192 The fascinating nonlinear behaviour of this condensate is largely dictated by the strength of polari

193 The temperature of the condensate is mapped onto the quantum phase of an atomic

194 en adjacent nucleation sites for supercooled condensate is properly controlled with chemical micropat

195 many-body systems like trapped Bose-Einstein condensates is enriched by the emergence of quantum corr

196 ggesting that active Wnt signaling in dermal condensates is important for hair follicle formation to

197 Controlling the size and shape of DNA condensates is important in vivo and for the improvement

198 In the study of non-equilibrium polariton condensates it is usually assumed that the dispersion re

199 By imprinting polariton condensate lattices of bespoke geometries we show that w

200 erformed, and indicated that cigarette smoke condensate leads to genome instability in human bronchia

201 tomic loss due to the finite lifetime of the condensate leads to larger spin oscillation amplitudes,

202 me much slower with respect to the polariton condensate lifetime.

203 After crossing the critical point, the condensates manifest delayed growth of spin fluctuations

204 The jumping-condensate mechanism is shown to spontaneously clean sup

205 tomic impurities immersed in a Bose-Einstein condensate mixture (BEC).

206 nockout in embryonic day 14.5 (E14.5) dermal condensates, morphogenesis proceeds regularly with norma

207 he supersaturation, we observed a variety of condensate morphologies consistent with those reported i

208 pling also implies new structures of exciton condensates, new functionalities of excitonic circuits a

209 rmed from a ring of superfluid Bose-Einstein condensate obstructed by a rotating weak link (a region

210 ht solitary matter-wave from a Bose-Einstein condensate of (85)Rb, which is observed to propagate ove

211 t the superfluid in underdoped cuprates is a condensate of coherently-mixed particle-particle and par

212 The quantum condensate of Cooper pairs forming a superconductor was

213 ss of [Formula: see text] state containing a condensate of d-wave Cooper pairs, concealed by their en

214 ochastic exciton-photon transitions within a condensate of exciton polaritons.

215 of a single trapped ion into a Bose-Einstein condensate of neutral atoms.

216 ly consistent with the presence of a central condensate of nuclear pore proteins in the NPC channel.

217 es, and indicates the formation of many-body condensate of optical phonons around resonant defects.

218 t circulation in a macroscopic Bose-Einstein condensate of polaritons in a ring geometry.

219 d-wave superconducting microscope tip to the condensate of the superconductor Bi2Sr2CaCu2O8+x.

220 ers of lipid peroxidation, in exhaled breath condensate of three healthy subjects (N = 3).

221 f impurity atoms immersed in a Bose-Einstein condensate of ultra cold atoms.

222 nent Rabi oscillations in driven-dissipative condensates of exciton-polaritons in semiconductor micro

223 e also been developed based on Bose-Einstein condensates of exciton-polaritons in semiconductor micro

224 generating different three-dimensional (3D) condensates of human mesenchymal stromal cells (MSCs).

225 otein) expression and Cre activity in dermal condensates of nascent first-wave hair follicles at E14.

226 opic efficiency, conclusions consistent with condensates of silicates, perovskite, and silica of subm

227 Stress granules (SGs) are cytoplasmic condensates of stalled messenger ribonucleoprotein compl

228 s (SG) are membrane-less organelles that are condensates of stalled translation initiation complexes

229 utagenicity was particularly observed in the condensates of the gas phase.

230 Metabolomic profiling of exhaled breath condensate offers opportunities for the development of n

231 herently imprinted into an exciton-polariton condensate on a planar semiconductor microcavity.

232 perhydrophobic surface, sweeping the growing condensate on the condensing surface downstream.

233 How such droplets condensate or melt and how the orientational symmetry is

234 most likely inhibit the formation of larger condensates or nontubular structures.

235 surface of the Moon likely have a partially condensate origin from its interior.

236 NP packaging; instead, vRNPs form "eccentric condensates" outside the core.

237 Condensate pH was 6.2 and its chemical oxygen demand (CO

238 ess (exhaled nitric oxide and exhaled breath condensate pH, malondialdehyde, and nitrite), and system

239 cytokines and intraoperative exhaled breath condensate pH; alveolar type 1 epithelial injury was ass

240 inflammatory agents, such as cigarette smoke condensate, phorbol 12-myristate 13-acetate, okadaic aci

241 One compressor station and one natural gas condensate processing facility were found to have signif

242 production, and hydrocarbon liquids (oil or condensate) production.

243 2) the release of the surface free energy of condensate promotes the self-shedding.

244 mechanisms by which Wnt signaling in dermal condensates regulates hair follicle formation, we analyz

245 nucleation densities while maintaining easy condensate removal and low contact angles.

246 We conclude that eccentric condensates represent nonpackaged vRNPs and that either

247 antized vortices in atomic gas Bose-Einstein condensates, research is beginning to focus on the roles

248 PLC-HRMS/MS experiments using exhaled breath condensate, respectively.

249 atoms, revealed by measuring a Bose-Einstein condensate's transport properties perpendicular to a syn

250 zoles were also determined in exhaled breath condensate samples by means of ultra high-performance li

251 ance spectroscopy was used to analyse breath condensate samples from 82 subjects with asthma and 35 h

252 Condensate samples were analyzed using a metabolomic app

253 el structure, ranging from a central polymer condensate (selective phase) to brushlike polymer arrang

254 e in dropwise or filmwise mode, the grown-up condensate self-sheds and falls off the superhydrophobic

255 Exciton-polariton condensates-sharing the same basic device structure as a

256 energy to high wavenumber components in the condensate spatial profile.

257 ar magnetic resonance spectroscopy of breath condensate successfully differentiates asthmatics from h

258 mic features similar to atomic Bose-Einstein condensates, such as long-range coherence, superfluidity

259 bove 0.01 g/s and included short-term (i.e., condensate tank flashing) and maintenance-related emissi

260 BaP) is a major component of cigarette smoke condensate that has received significant attention due t

261 We characterize the dynamics of condensate that the continuous self-shedding and sweepin

262 RNA metabolism and comprise a large class of condensates that are enriched in RNA-binding proteins an

263 (PT) depending on the PEL for two polariton condensates that might be described as transition from t

264 rmis, enlarged epidermal placodes and dermal condensates that result in prematurely differentiated en

265 Our source of light is a polariton condensate, that allows high-resolution filtering of a s

266 miscibility of the spin components of such a condensate, the presence of stripes has not been detecte

267 ransitional dynamics of Bose-Einstein magnon condensate: the density of the condensate increases imme

268 Additionally, in exciton-polariton condensates there is a variety of dynamical scenarios an

269 thermal resistance gradually takes over with condensate thickness growing.

270 nsate bulk thermal resistance depends on the condensate thickness, which is time-dependent.

271 nnel is realized by coupling a Bose-Einstein condensate to an optical cavity with ultranarrow bandwid

272 tories determined the DNA-DNA force in a DNA condensate to be pairwise, the DNA condensation to be dr

273 ling spectroscopy reveal the superconducting condensate to emerge first in surface puddles, with the

274 of low-energy quasi-particles needed for the condensate to form can be produced via external pumping.

275 ternal degrees of freedom of a Bose-Einstein condensate to the light field of a high-finesse optical

276 allenges, particularly the ability of liquid condensates to both facilitate and respond to biological

277 n normal media with or without tobacco smoke condensate (TSC) under clinically relevant exposure cond

278 aterally associate in vitro into polymorphic condensates typically imaged on surfaces.

279 ogical breakthroughs including Bose-Einstein condensates, ultrafast spectroscopy, superresolution opt

280 We demonstrate condensate visualization capabilities directly by using

281 ng dissipation patterns whose precedents are condensate vortex and defect disorder and condensate exc

282 urg-Landau equation, which indicates why the condensate wants to rotate.

283 mortality (100%) occurred in 48 h, even when condensate was diluted by a factor of 10,000 and styrene

284 ater contamination potential and that of its condensate waste was characterized.

285 e complex water samples including feedwater, condensate water, and boiler water, all collected from l

286 date how the CDW transition impacts the pair condensate, we have used torque magnetization to 45 T an

287 lial cell lines treated with cigarette smoke condensate were also performed, and indicated that cigar

288 stigate the dynamics of an exciton-polariton condensate which emerges in semiconductor microcavity su

289 pontaneous formation of a linearly polarized condensate, which exhibits a superlinear power dependenc

290 elled jumping motion of the resulting liquid condensate, which partially covers or fully encloses the

291 s superfluid helium and atomic Bose-Einstein condensates, which are characterized by quantized vortic

292 methyl ketones with >95% yields into trimer condensates, which can then be hydrodeoxygenated in near

293 ble quantum well systems can support exciton condensates, which consist of electrons in one well tigh

294 onal systems, including atomic Bose-Einstein condensates with attractive interactions.

295 As bosons, polaritons can form condensates with coherent laser-like emission.

296 tically dressed neutral atomic Bose-Einstein condensates with equal, and opposite, momenta and observ

297 naway stimulated collisions in Bose-Einstein condensates with periodically modulated interaction stre

298 tion ability and could form very compact DNA condensates with small particle size (approximately 100

299 Bose-Einstein condensates with spin-orbit coupling are predicted to po

300 efforts have focused on easy removal of the condensate, yet the other desired properties of low cont