ライフサイエンスコーパス: phase transition

1 l energy of monoclinic phase and induces the phase transition.

2 a system possessing such a feedback-induced phase transition.

3 FE order through a well-defined first-order phase transition.

4 ream molecular targets of this developmental phase transition.

5 pecific monoclonal antibody (MAb) 4D1 during phase transition.

6 g to an exotic ferromagnetic to paramagnetic phase transition.

7 le unwinding, that is, a cholesteric-nematic phase transition.

8 ge ([Formula: see text]) at the point of the phase transition.

9 the existence of a purely thermal structural phase transition.

10 ccumulates gradually and accounts for the Mn phase transition.

11 antiferromagnetic (AF) to ferromagnetic (FM) phase transition.

12 ty and the structural heterogeneity close to phase transition.

13 tomic multiplet symmetry across the magnetic phase transition.

14 scopic shape change through a liquid crystal phase transition.

15 called super-saturated system in first order phase transition.

16 mblies by leveraging the host's thermotropic phase transition.

17 driving forces underlying this nonmonotonous phase transition.

18 melting the PCM to trigger a solid-to-liquid phase transition.

19 n and inducing cell cycle arrest at the G1/S phase transition.

20 how ring-shaped complexes could survive the phase transition.

21 nization of lipids, eventually to a membrane phase transition.

22 a strongly correlated material undergoing a phase transition.

23 ling behavior for the QAH to axion insulator phase transition.

24 eter and a thermometer and is "reset" by the phase transition.

25 rge ordering mechanism drives the structural phase transition.

26 onnuclear kinases might be influencing FUS's phase transitions.

27 ctivity, spectral anomalies, and unexplained phase transitions.

28 eal probe for mapping a materials structural phase transitions.

29 aining a deeper understanding of the quantum phase transitions.

30 sorder-to-order transition and modulation of phase transitions.

31 t these conditions, and does not undergo any phase transitions.

32 ditivity for organogenesis and developmental phase transitions.

33 gnatures at the same fields confirming these phase transitions.

34 tanding of the physics of wetting and drying phase transitions.

35 here obligate heterotypic interactions drive phase transitions.

36 behavior often displaying easily accessible phase transitions.

37 the framework of metal-insulator topotactic phase transitions.

38 bducting plate, nonlinear rheology and major phase transitions.

39 network activity was maximal at respiratory phase transitions.

40 ion mismatch(14), and heat-induced substrate phase transition(15), the controllable and device-compat

41 terrupted by competing phases or first-order phase transitions(6-8).

42 rsal behaviours akin to standard equilibrium phase transitions(8,23,24).

43 Here, with phase transitions actuated by in situ silicon PIN diode

44 Phase transitions also vary with particle shape: rod-sha

45 A rare temperature-induced phase transition alters the conformation of the photoact

46 by two quantum criticalities: a superradiant phase transition and a spectral collapse, that is, the c

47 Here, unusual phase transition and band renormalization effects in 2D

48 ea, are critically important for respiratory phase transition and duration control.

49 alyses demonstrate that SPL7 and SPL8 induce phase transition and flowering in grasses by directly up

50 and EMSA were used to identify regulators of phase transition and flowering.

51 pairing fluctuations condense at a separate phase transition and form a nematic state with broken Z(

52 ne lipids, introduce a similar primary lipid-phase transition and liquid-ordered properties.

53 ed and reduced forms, which have contrasting phase transition and LSPR characteristics.

54 of both qubit and photon dissipation on the phase transition and on the instability induced by the s

55 , which is associated with layered-to-spinel phase transition and oxygen redox reaction.

56 shaped particles show a partially reversible phase transition and the onset of the structural phase t

57 epresented TFs involved mainly in cell-cycle phase transitions and 15 under-represented TFs primarily

58 ns of low sequence complexity that can drive phase transitions and are commonly found in many protein

59 Striking examples are broken symmetry, phase transitions and collective excitations(2).

60 The sequence of phase transitions and Dirac revivals is observed at temp

61 , can be used to accurately detect different phase transitions and gain information about dynamics of

62 observe the disappearance of the structural phase transitions and indications of a glassy dipolar ph

63 sregulated LLPS can also facilitate aberrant phase transitions and lead to protein aggregation and di

64 Development of methods to measure the phase transitions and physical properties of submicron a

65 ptions of PTMs might be involved in aberrant phase transitions and the formation of amyloid-like prot

66 spin-momentum locking, a Meissner-to-vortex phase transition, and signatures of topological chiral o

67 coding for proteins involved in development, phase transition, and transport.

68 ous peak in specific heat at low T, magnetic phase transitions, and no mixed valency), YbB(6) (mixed

69 ntropy at low temperatures, pressure-induced phase transitions, and related features in Raman spectra

70 al framework to classify topological quantum phase transitions, and reveals their ubiquitous relation

71 ent means for triggering the solid-to-liquid phase transition are discussed.

72 Phase transitions are driven by collective fluctuations

73 e has accrued indicating that aberrations in phase transitions are early events in the pathogenesis o

74 While equilibrium phase transitions are easily described by order paramete

75 The phase transitions are induced by severe tetrahedral dist

76 Solid-solid phase transitions are processes ripe for the discovery o

77 We find a phase transition as a function of F or q, resulting in a

78 y diffraction, and phase-field modeling, the phase transition as a function of layer thickness (numbe

79 flash freeze submicron particles to measure phase transitions as a function of relative humidity (RH

80 inite flocks not only fails to peak near the phase transition, as demonstrated for the canonical 2D I

81 the membrane structure and dynamics close to phase transition, as well as its stability with respect

82 teractions, long-range ordering, and related phase transitions, as well as the atomic thickness yet h

83 diffusionless athermal cubic-to-rhombohedral phase transition at around 700 K.

84 t across the alpha-Zr to omega-Zr structural phase transition at room-temperature, with nucleation an

85 ncreases, amorphous ITO thin films undergo a phase transition at ~ 200 degrees C and develop polycrys

86 tle, and buoyancy forces associated with the phase transitions at 410 km and 660 km.

87 PC:cholesterol lipid bilayers to investigate phase transitions at temperatures from 310 to 270 K.

88 densed matter physics and chemistry, such as phase transition, atomic diffusion, grain boundary dynam

89 The potassium salt presented a solid-solid phase transition before decomposition.

90 ighlighted the origin, structure, nature and phase transition behavior of the smart polymers found su

91 been widely conducted, their shape-dependent phase transition behavior still remains unclear.

92 disorder, although the former affected their phase-transition behavior.

93 The phase transition between self-assembled molecular networ

94 ics of neural systems to be tuned toward the phase transition between stability and instability as is

95 d that the reversible redox-based topotactic phase transition between the insulating brownmillerite p

96 fect, whereby rhombohedral graphite exhibits phase transitions between a gapless semimetallic phase a

97 dback has been suggested as a tool to induce phase transitions beyond the dissipative ones and tune t

98 w-dimensional ice formation and liquid-solid phase transitions, but with structural and dynamical sig

99 bration time scales, we demonstrate that gel phase transitions can be identified in aerosol particles

100 The location of phase transitions can shift between the micrometer and n

101 group Fm3m), which shows reversible thermal phase transitions, can be readily obtained by ball mill

102 markedly altered crystallographic phase and phase transition characteristics as compared to single-d

103 text] exhibits a tetragonal-to-orthorhombic phase transition consistent with ferroquadrupole order o

104 only observed below 54 K, where a structural phase transition creates inequivalent Cu-O bonds, we dis

105 Upon reversible alpha-to-gamma phase transition, crystals of (phenylazophenyl)palladium

106 ess organelles, including rescue of aberrant phase transitions, demixing of condensates, and time evo

107 Metal to insulator phase transition due to electron localization in disorde

108 : i) absence of a genuine zero-field quantum phase transition due to the presence of B(loc); ii) conn

109 pological Hall effect at the boundary of the phase transition due to the proton concentration gradien

110 nfirmations that reveal an interesting sharp phase transition during the drying state and in the drie

111 Phase transitions during epidermal stratification crowde

112 peaked specifically at the three respiratory phase transitions, E2-I, I-PI and PI-E2.

113 solution, fluid density changes, and gas-oil phase transitions (ebullition, condensation) may all con

114 similar or identical state via at least two phase transitions elicited by variation of a single para

115 ree nature of this unique insulator-to-metal phase transition enabled us to engineer the temperature

116 a significant suppression of the structural phase transitions, enhanced disorder and stabilization o

117 the dilution concentration for the observed phase transition equivalent to 62% (v/v).

118 NMR can therefore readily observe phase transitions, evaluate phase purity and composition

119 spectroscopy enables the characterization of phase transitions even in the absence of static magnetic

120 In particular, we identified a phase transition event, namely the folding of antigenic

121 ttery were probed, revealing a heterogeneous phase transition evolution at solid-solid interfaces.

122 al excitation energy, we show that transient phase transitions exhibit timing jitter in the condensat

123 The reversible 3delta <-> 3gamma phase transition exhibits thermal hysteresis of 20 K.

124 ents by allowing for characterization of the phase transitions for individual particles in a populati

125 ndensates can undergo a further irreversible phase transition, forming solid nanoscale aggregates ass

126 rocity, the binary fluid mixture undergoes a phase transition from a homogeneous mixed state to a dem

127 hase to the alpha-phase drives a topological phase transition from a nontrivial WTI to a normal insul

128 electric-field plane, and is attributed to a phase transition from a normal metal to a spin-polarized

129 observe the few-body precursor of a quantum phase transition from a normal to a superfluid phase.

130 A magnetic-field-driven quantum phase transition from a QAH insulator to an axion insula

131 , our experiment suggests a possible quantum phase transition from an antiferromagnetic to a weak fer

132 trolling, understanding, and elucidating the phase transition from gel to crystal are highly importan

133 Upon further addition of PW, a phase transition from globules to micrometric sheets is

134 ve 415 K the material undergoes a structural phase transition from monoclinic (C2/c) to orthorhombic

135 e spontaneous symmetry breaking results in a phase transition from motionless temperature profiles, d

136 the external coupling strengths, at which a phase transition from synchronization to incoherence occ

137 The topological phase transition from the metallic state to the dielectr

138 symmetry breaking, identifying a first-order phase transition from the normal to the superradiant pha

139 Consequently, the main factor causing the phase transition from the tetragonal to cubic phase near

140 reochemical activity compete, giving rise to phase transitions from a nonchiral cubic structure to an

141 OFs and allows a strategy to achieve quantum phase transitions from antiferromagnet to spin liquid an

142 Furthermore, we reveal topological phase transitions from higher- to lower-order multipole

143 The phase transitions from one plateau to the next plateau o

144 rimental observation of the full sequence of phase transitions from perovskite to post-perovskite to

145 pressures up to 42.1 GPa through a series of phase transitions from the cubic P2(1)3, through orthorh

146 tome analysis revealed up-regulation of G1/S phase transition genes (myelocytomatosis oncogene cellul

147 The occurrence and mechanism of the AFE phase transition have been also confirmed by heat capaci

148 associated with classical, thermally driven phase transitions have been extensively studied in syste

149 Reentrant phase transitions have been modeled in vitro using prote

150 Over the past decade, phase transitions have emerged as a fundamental mechanis

151 or even pure elemental systems, can undergo phase transitions hosting nontrivial topological phase t

152 e transitions hosting nontrivial topological phase transitions hosting nontrivial topological propert

153 dynamically impossible during a second-order phase transition in a bulk single crystal.

154 Here, the novel phase transition in anisotropic Nb((1-) (x) ()) Ti(x) S(

155 gap at the Fermi level, leading to an exotic phase transition in CrN.

156 explore the properties of the nonequilibrium phase transition in dynamics that occurs in trajectory s

157 to control the ground states and associated phase transition in epitaxial films.

158 t of the pressure-driven [Formula: see text] phase transition in iron and the complex pressure-temper

159 ration (LLPS); however, observations of this phase transition in living cells are limited.

160 lts not only attest to the efficacy of using phase transition in manipulating the microstructures of

161 ature required for the lamellar-to-hexagonal phase transition in PE bilayers, suggesting that it impo

162 After this phase transition in silica, subducted oceanic crust will

163 at this arises as a consequence of a natural phase transition in the dynamic self-organization among

164 onstration of such an effect in a trajectory phase transition in the dynamics of a structural glass f

165 ttern as the single-photon-triggered quantum phase transition in the Rabi model.

166 its increased partitioning and the smoothed phase transition in the ternary mixture compared to the

167 Importantly, Ir doping facilitates a phase transition in the WO(3) bulk lattice, which furthe

168 Phase transition in thermoelectric (TE) material is a do

169 discontinuously across a topological quantum phase transition in two-dimensional time-reversal invari

170 ork opens up possibilities for studying such phase transitions in 2D materials.

171 is used as a model system for understanding phase transitions in ABX(3) systems (e.g., MgSiO(3)) at

172 and K and heavier become transition metals); phase transitions in Ca, Sr, and Ba correlating well wit

173 shown to alter FUS's liquid-phase and solid-phase transitions in cell models and in vitro.

174 paradigm underlying physiologically relevant phase transitions in cells is the reversible head-to-tai

175 ubiquitous soft modes that trigger important phase transitions in diverse classes of materials while

176 the potential of manipulating order-disorder phase transitions in metal-organic materials for thermal

177 e and shed light on rational manipulation of phase transitions in nanomaterials.

178 Nonequilibrium phase transitions in open dissipative systems can be des

179 mological structure creation and topological phase transitions in quantum matter(10-12), and may tran

180 cts antibiotic-induced collapses to gelation phase transitions in soft materials, providing a framewo

181 d possible connections with disorder-induced phase transitions in statistical physics.

182 ametric statistical models and the theory of phase transitions in statistical physics.

183 In particular, the role of phase transitions in the assembly of large, complex ribo

184 RUS) revealed two distinct symmetry-breaking phase transitions in the mononuclear Mn(3+) compound [Mn

185 We study the quantum phase transitions in the nickel pnctides, CeNi(2-delta)(

186 ects are cooling effects of pressure-induced phase transitions) in a class of disordered solids calle

187 temperature conditions, XAS is sensitive to phase transitions, including melting, and allows gatheri

188 n a multistage process where each successive phase transition incurs the smallest loss of free energy

189 d the United States, showing a discontinuous phase transition, indicating that a small local disturba

190 This phase-transition-induced volume expansion strategy could

191 one interactions driving the liquid-to-solid phase transition into heterogeneous solid-like aggregate

192 More recently, protein condensation phase transitions, into three-dimensional droplets or in

193 Phase transition is a fundamental physical phenomenon th

194 This phase transition is also visualized by in situ TEM, acqu

195 peratures when the first-order ferroelectric phase transition is driven supercritically (as verified

196 depth change, where a remarkable statistical phase transition is generated by varying the inverse tem

197 g of how protons and electrons behave in the phase transition is lacking, mainly due to the difficult

198 The experimentally observed A15-disorder phase transition is not captured using mean-field approx

199 A phase transition is often accompanied by the appearance

200 ulations show that the energy barrier of the phase transition is responsible for the observed thickne

201 A phase transition is termed reentrant if it involves the

202 It is shown that the nature of phase transitions is linked to the lattice V(3+)/V(5+) c

203 al responses that signal topological quantum phase transitions is of both theoretical and experimenta

204 ed Na(+) /vacancy arrangement and P2->O2/OP4 phase transitions, leading them to exhibit multiple volt

205 unique phase diagram where the second-order phase transition line terminates at a tricritical point

206 having nondangling bonds on the surface, 2D phase-transition materials have vast potential for use i

207 Phase-transition materials provide exciting opportunitie

208 proposed that ferroelectric-like structural phase transitions may occur in metals, despite the expec

209 DFT calculations trace the phase-transition mechanism via the existence/absence of

210 Fine-tuning strain and vacancies in 2H-phase transition-metal dichalcogenides, although extreme

211 solar cells(1) but suffer from an undesired phase transition near room temperature(2).

212 rgoes a reversible and isotropic first-order phase transition near-room temperature, corresponding to

213 Analogous to RNA-induced liquid-liquid phase transitions observed for other proteins implicated

214 In order to assess the phase transitions occurring in the products, a state dia

215 on diffraction patterns demonstrate that the phase transition occurs across the whole sample at ~147

216 and revealed that the lamellar gel-to-fluid phase transition occurs below 0 degrees C, reflecting th

217 It has been predicted that a first-order phase transition occurs during white-dwarf cooling, lead

218 This phase transition occurs isothermally and is governed by

219 te transformations on cooling; below 300 K a phase transition occurs to form 3gamma (monoclinic P2(1)

220 pulation may have a range of RH over which a phase transition occurs.

221 Co nanoparticles have a lower order-disorder phase transition (ODPT) temperature relative to the bulk

222 articles is associated with the simultaneous phase transition of amorphous carbon to a highly defecti

223 Here we report that condensation and phase transition of heat-shock factor 1 (HSF1), a transc

224 evidence of defects at multiple levels, from phase transition of individual proteins to the dynamic b

225 The first order chain-melting phase transition of lipid membranes is observed to be ac

226 This study highlights the contribution of phase transition of peptide antigens on vaccine formulat

227 zine-bearing paper channels as the result of phase transition of the hydrogels, realizing multiplexed

228 labile, cross-beta polymers that facilitate phase transition of the protein into liquid-like or gel-

229 tamaterial is heated, the insulator-to-metal phase transition of vanadium dioxide effectively renders

230 Examples of phase transitions of CdS nanoparticles are very limited,

231 Furthermore, we show that aberrant phase transitions of cytoplasmic TDP-43 are neurotoxic a

232 estigation into the crystalline to amorphous phase transitions of prepared 1,3,6-substituted pentaful

233 s and homogeneous nucleation in liquid-solid phase transitions of Pt.

234 diation shed light for the first time to the phase transitions of the higher layer 2D R-P perovskites

235 an approach for in-situ characterization of phase transitions of ultrathin nickel silicides using 3D

236 This flow-induced phase-transition of the stored native silk molecules is

237 lows us to probe the dependence of dynamical phase transitions on system size, initial state and othe

238 to the two-dimensional F-model, with exotic phase transitions on topologically-constrained configura

239 analyses for DEs characterized by two forms (phase transition or magnitude tuning), under different c

240 evidence of large systematic effects on the phase transition owing to dynamical fluctuations of the

241 It plays a key role in the study of phase transitions, pattern formation, protein folding, a

242 e can readily describe mechanical stress and phase transition phenomena.

243 relationship in clock-controlled growth and phase transition phenotypes.

244 lses via ultrafast photo-induced first-order phase transitions (PIPTs).

245 e transition and the onset of the structural phase transition pressure decreases with decreasing surf

246 ersible phase transition with relatively low phase transition pressure.

247 All quantum phase transitions (QPT) reported previously were induced

248 Quantum phase transitions (QPTs) involve transformations between

249 at are key to understanding how pathological phase transitions relate to pleiotropic defects in cellu

250 ules and possesses only one pressure-induced phase transition related to PbBr(6) octahedra and BA til

251 2) Br(7) (n = 2) layers undergo two distinct phase transitions related to PbBr(6) octahedra, butylamm

252 ELF3 between active and inactive states via phase transition represents a previously unknown thermos

253 lly as a function of the parameters, and the phase transition separating regions in the phase space w

254 An unusual inverse phase transition sequence from a BCC phase to a sigma ph

255 Structural phase transitions serve as the basis for many functional

256 it is found that the electric-field-induced phase transition spreads over a large area in (001) orie

257 The photoinduced phase transition, starting with a compact crystalline so

258 rimental and theoretical study of structural phase transitions, structural phases and dipolar dynamic

259 edge of the biophysics underlying biological phase transitions suggests that this process offers a un

260 Hence, investigating the phase-transition superstructures that self-assemble thro

261 the (13)C and (207)Pb nuclei varied near the phase transition temperature (T(C) = 236 K), indicating

262 domains in a fluid-like bilayer close to the phase transition temperature (T(m)).

263 Raw TMC exhibited a first-order phase transition temperature at 58.15 +/- 0.38 degrees C

264 Phase transition temperature measurements were correlate

265 ipoTherm sized around 100 nm and exhibited a phase transition temperature of 43 degrees C.

266 size at temperatures below the lipid's main phase transition temperature T(m) and, based on these re

267 low its structural antiferrodistortive (AFD) phase transition temperature.

268 red thermally by taking the crystal over the phase transition temperature.

269 by revealing the soft-mode mechanism of the phase transition that impacts thermal transport and ther

270 osing driving forces and, in particular, the phase transitions that emerge in the periodic geometry o

271 Based on the Landau theory of phase transition, the resulting free energy barrier is f

272 ne near T(C), indicating the occurrence of a phase transition to a cubic phase with higher symmetry t

273 ication of a magnetic field drives a quantum phase transition to an easy-plane antiferromagnet, which

274 multilayer films undergo a pressure-induced phase transition to antiferroelectric phase at 1.7 GPa a

275 stingly, protamine undergoes a DNA-dependent phase transition to gel-like condensates and SRPK1-media

276 e phonon-instability conditions that promote phase transition to graphite.

277 the antigen-bound autoantibodies to undergo phase transition to insoluble aggregates at lower temper

278 lation properties allow systems exhibiting a phase transition to self-tune to their critical point.

279 sulfide nanoparticles undergo a spontaneous phase transition to tetragonal chalcocite in situ, prior

280 nhibition during cocaine's initial rewarding phase transitioning to excitation during cocaine's delay

281 hese discoveries extend the understanding of phase transitions to the nanoscale and shed light on rat

282 ead towards a better understanding of matter phase transitions under extreme irradiation conditions.

283 esults revealing a nonequilibrium continuous phase transition unify the structural arrest and yieldin

284 lts show that 2D Janus layers do not undergo phase transition up to 15 GPa, and in this pressure regi

285 are polymeric drug solutions that undergo a phase transition upon injection into an aqueous environm

286 ing pseudo-prime numbers and random SAT with phase transitions), using a D-Wave 2000Q quantum process

287 /mmc) to low temperature orthorhombic (Pnma) phase transition via differential scanning calorimetry (

288 specific heat, and pressure induced magnetic phase transitions), we present a unifying dynamic bondin

289 espite the non-equilibrium character of this phase transition, we construct an effective free-energy

290 ording to DFT calculations, Li/TM mixing and phase transition were aided by the low diffusion barrier

291 No structural phase transitions were observed from 1.8 K to 523 K.

292 Ir(2)In(8)Te, respectively) low-temperature phase transitions, where the chalcogenide anions in the

293 versible, photoinduced orthorhombic-to-cubic phase transition which is discernible at fluences greate

294 ey are populated through a sequence of sharp phase transitions, which appear as strong asymmetric jum

295 metry-preserving, purely thermal, reversible phase transitions, which are fundamental in physics and

296 which display first-order magnetostructural phase transitions whose large latent heats are tradition

297 ile spherical particles undergo irreversible phase transition with relatively low phase transition pr

298 magnetic T(C) and sharpness of the magnetic phase transitions with increasing oxygen growth pressure

299 y allows the spatiotemporal evolution of the phase transition within a single nanoparticle to be moni

300 The interplay between these two phase transitions yields exquisite composition fluctuati