ライフサイエンスコーパス: phase transition

1 sibly drives a ferromagnetic-to-paramagnetic phase transition.

2 sponsible for the missing of the percolation phase transition.

3 nic Arabidopsis during the juvenile-to-adult phase transition.

4 nt for the selectivity enhancements near the phase transition.

5 hat encode proteins critical for the G1-to-S phase transition.

6 5 and 50 mol% led to suppression of the main phase transition.

7 , the glass transition results in an avoided phase transition.

8 eved at high temperatures or pressures via a phase transition.

9 ize reduction effect on the MnAs crystalline phase transition.

10 s in a narrow range, characteristic of lipid phase transition.

11 rotein, suggesting inhibition of the G1-to-S phase transition.

12 e collapse of 10.2% was estimated during the phase transition.

13 alysis datasets, we verified the percolation phase transition.

14 eformations in another phase upon crossing a phase transition.

15 an antiferromagnet (AFM) to ferromagnet (FM) phase transition.

16 ts as the gold standard method for measuring phase transition.

17 on observation of hallmarks of a reversible phase transition.

18 um phase transition and, in turn, a magnetic phase transition.

19 h pressure and dramatically dropped near the phase transition.

20 n to the local transition temperature of the phase transition.

21 l root QCs coincided with this developmental phase transition.

22 ose to (1/4), as predicted for a tricritical phase transition.

23 temperature is tuned across the topological phase transition.

24 phase around 160 K, again via a first-order phase transition.

25 , and it does not accelerate G1/S cell cycle phase transition.

26 ivision and coincides with the developmental phase transition.

27 tic dynamics of a system across a continuous phase transition.

28 possible tetragonal to collapsed tetragonal phase transition.

29 s an example of a (zero temperature) quantum phase transition.

30 ed the propensity of TIA1 protein to undergo phase transition.

31 ution, decreasing the driving force for this phase transition.

32 rimentally realize a mixed-order equilibrium phase transition.

33 f inducing the semiconductor-metal 2H-1T TMD phase transition.

34 he first-order thermodynamics nature of this phase transition.

35 cubic-like symmetry through an isostructural phase transition.

36 sorption is the major driving force for this phase transition.

37 ive to the selectivity observed far from the phase transition.

38 ically described in terms of the first-order phase transition.

39 the octahedra become tilted, leading to two phase transitions.

40 the unconventional properties of mixed-order phase transitions.

41 asmonics and catalysis, light harvesting, or phase transitions.

42 self-organized synchronization and dynamical phase transitions.

43 cell differentiation and allow developmental phase transitions.

44 tions in large systems and their relation to phase transitions.

45 cal defects which occur at symmetry-breaking phase transitions.

46 poised to undergo a small number of demixing phase transitions.

47 universal when the systems cross continuous phase transitions.

48 he soil modify plant growth, development and phase transitions.

49 om the critical scaling laws of second-order phase transitions.

50 ately linked to symmetry-lowering structural phase transitions.

51 n, anomalies occur which may lead to quantum phase transitions.

52 l variable is reminiscent of non-equilibrium phase transitions.

53 ls that include discontinuous and continuous phase transitions.

54 We observe a dynamical phase transition after a sudden change of the Hamiltonia

55 We show that the phase transition also changes the observed SWCNT corona

56 dimension of space, the nature of a quantum phase transition also depends on the dynamics.

57 d/gas phases) have different symmetries, the phase transitions among them can be explained by Landau'

58 mponent lipid bilayer membranes display rich phase transition and associated compositional lipid doma

59 Our theory further predicts a phase transition and discontinuous charge regulation of

60 mediated by proximity to the order-disorder phase transition and the size and hydrophobic mismatch o

61 diamond-cubic (dc) to diamond-hexagonal (dh) phase transition and then proceeds by dislocation nuclea

62 demonstrate the universality of this quantum phase transition and to present convincing experimental

63 effect, which induces a topological quantum phase transition and, in turn, a magnetic phase transiti

64 a states and interaction-induced topological phase transitions and also identify trivial-superconduct

65 t respond to mild stimuli through collective phase transitions and amplify signals could open up new

66 K2 and thereby contributes to increased G1-S phase transitions and cell proliferation.

67 materials with the intrinsic diffuseness of phase transitions and correlation characteristics.

68 ear dynamic behavior of materials undergoing phase transitions and domain switching at the structural

69 required to characterize driven-dissipative phase transitions and enable the investigation of topolo

70 logy, and may enable explorations of quantum phase transitions and macroscopic quantum tunnelling in

71 ratory for the in-depth study of topological phase transitions and related phenomena that range from

72 ns are required to promote all developmental phase transitions and to control cell proliferation duri

73 hod can be adopted to fabricate other porous phase-transition and thermoelectric chalcogenide materia

74 rance exists at which the system undergoes a phase transition, and above which the network almost com

75 pin liquids, Berezinskii-Kosterlitz-Thouless phase transition, and classical magnetism, among the man

76 may be related across the nematic-smectic A phase transition, and presents new possibilities for con

77 ar correspondence between the emergence of a phase transition, and the emergence of attractor-like st

78 Polymers with a thermally triggered phase transition are important in the design of material

79 The structural changes associated with the phase transition are similar to the fluctuation modes of

80 re refinements indicate that the consecutive phase transitions are correlated to the changes in the B

81 Solid-solid phase transitions are the most ubiquitous in nature, and

82 Phase transitions are ubiquitous in nonliving matter, an

83 Phase transitions are ubiquitous in structurally complex

84 The potential model reproduces the VIII-X phase transition as observed in experiment.

85 ction, ordered moments vanish at the quantum phase transition as pressure increases the electron kine

86 , organic aerosol was thought to undergo two phase transitions as the relative humidity around the pa

87 blishes the understanding of non-equilibrium phase transitions as topological transitions in configur

88 The structural phase transition, as well as the spin-density-wave order

89 The compound experiences a ferroelectric phase transition ascribed to the 6s(2) lone-pair effects

90 he switch from a first-order to second-order phase transition associated with social contagion dynami

91 n open to a closed state is identical to the phase transition associated with the reversal of magneti

92 identification of a class of non-equilibrium phase transitions associated with the loss of combined p

93 e solid electrolyte AgI, near its superionic phase transition at 420 K.

94 erent perfect absorption and demonstrate the phase transition at the exceptional point.

95 iffraction of Sb2S3 up to 53 GPa reveals two phase transitions at 5 GPa and 15 GPa.

96 s controlled by the self-assembly and unique phase transition behavior of elastin-like polypeptides i

97 We explore the diverse structural and phase transition behavior of these materials through sin

98 conditions, significantly affecting its CDW phase-transition behavior.

99 phase coexistence mediated by a first-order phase transition between an emergent, low-temperature vo

100 ent switching driven by a voltage-controlled phase transition between CDW states in films of 1T-TaS2

101 ighest-performing known nanomaterials, and a phase transition between stable 1D metal and an antiferr

102 QH phase transitions, including a continuous phase transition between the even-denominator FQH state

103 onstration of an electrostatic-doping-driven phase transition between the hexagonal and monoclinic ph

104 oes a semimetal-to-semiconductor topological phase transition between the inverted and normal alignme

105 Using real-time optical spectroscopy, the phase transition between the two structurally distinct p

106 l peak is the consequence of a polyamorphous phase transition between two supercooled liquids, involv

107 vestigate quantum anomaly effects in quantum phase transitions between competing orders and striking

108 iscrete steps across 32 electric field-tuned phase transitions between states of different valley, sp

109 We discover Casimir force phase transitions between these staggered 2D materials i

110 em can thus elucidate not only physiological phase transitions but also their link to pathological ag

111 coverable from tetragonal-rhombohedral (T-R) phase transition by compressive stress.

112 Here, we bridge the gap between the two-phase transitions by density-functional theory calculati

113 equilibrium properties of observables near a phase transition can be classified according to few crit

114 This RNA-mediated reentrant phase transition can drive the formation of dynamic drop

115 zing point depression also impacts the lipid phase transition, causing a ssNMR-observed reduction in

116 nhibited cell proliferation, cell cycle G1/S phase transition, cell migration and invasion, indicatin

117 predicted at the critical temperature of the phase transition, consistent with a thermodynamic descri

118 Mixed-order phase transitions display a discontinuity in the order p

119 inement is a vivid illustration of a quantum phase transition dramatically affecting the superconduct

120 Phase transitions driven by intrinsically disordered pro

121 tion in the metallic phase, and measures the phase-transition dynamics in the insulating phase.

122 Considering the widely studied phase-transition dynamics in VO2, the proposed hybrid me

123 d analyze a generic, ionic strength-mediated phase transition exhibited by over 25 distinct oligonucl

124 py (NIRS) method to monitor the onset of fat phase transition (freezing/melting) in human abdominal a

125 The Berezinskii-Kosterlitz-Thouless phase transition from a disordered to a quasi-ordered st

126 psis thaliana, the xylem undergoes a drastic phase transition from a parenchyma-producing phase to a

127 hat it undergoes a first order meta-magnetic phase transition from an antiferromagnet to a ferromagne

128 ulations also revealed that GaSb undergoes a phase transition from F-43m to Imma at 7.0 GPa and expla

129 y 7.0 GPa, which corresponds to a structural phase transition from F-43m to Imma.

130 re range includes the well-known solid-solid phase transition from Ga-I to Ga-II at low temperature.

131 underlies the formation of crystals and the phase transition from liquid to solid.

132 ectly examine defects in the in situ thermal phase transition from nematic to smectic A in hybrid-ali

133 cate that this T c enhancement arises from a phase transition from pristine Bi2212 to a mixture of su

134 ysis on changing the pH between 5 and 8, via phase transition from super hydrophilic to hydrophobic.

135 hat increasing order in cell motion causes a phase transition from symmetric to asymmetric body elong

136 f a liquid-crystalline material to exhibit a phase transition from the heliconical twist-bend phase i

137 unexpected temperature-induced morphological phase transition from the nanodot to nanoribbon regime.

138 ctric field could cause the KTN to undergo a phase transition from the paraelectric phase to the ferr

139 rimental observations of consecutive quantum phase transitions from a Rashba type topological trivial

140 A novel phase transition, from multilayered 2H-MoTe2 to a parall

141 strain, Pentagon Carbon exhibits topological phase transitions, generating a series of novel quasipar

142 ortex motion can be disruptive; it can cause phase transitions, glitches in pulsars, and losses in su

143 derstanding the microscopic mechanism of the phase transitions, highlighting the importance of cooper

144 s shown to reproduce a second-order critical phase transition, i.e., a smooth switch to huddling when

145 ic transition is decoupled to the electronic phase transition, i.e., the AFM-to-FM transition occurs

146 ediated by electric-field induced structural phase transition in a ferroelectric BaTiO3 nanoparticle.

147 membrane bilayer following the gel-to-fluid phase transition in a pure phospholipid vesicle was obse

148 Monitoring phase transition in adipose tissue and formation of lipi

149 ements, which provides a versatile probe for phase transition in an electric manner in minute devices

150 nce of neural maps, which we link to a known phase transition in an Ising-like model from statistical

151 re we show that the first-order metamagnetic phase transition in FeRh films becomes strongly asymmetr

152 ates and investigate the dynamics across the phase transition in large arrays of atoms.

153 scopy, we are able to trigger a gel-to-fluid phase transition in lipid vesicles and monitor in real t

154 we show that the semiconductor-to-semimetal phase transition in monolayer MoTe2 can be driven by a g

155 Near room temperature second-order magnetic phase transition in soft magnetic material, gadolinium,

156 The topotactic phase transition in SrCoO x (x = 2.5-3.0) makes it possi

157 authors provide evidence for such a quantum phase transition in the attractive Coulomb potential of

158 size analysis method to identify the type of phase transition in the giant connected components (GCC)

159 In IrMn/FeCo bilayers, a structural phase transition in the IrMn layer develops at room temp

160 e has focused on the empirical findings of a phase transition in the parameter space of maximum entro

161 ests that pressure causes a liquid-to-liquid phase transition in this metallic alloy supercooled melt

162 The insulator-to-metal phase transition in vanadium dioxide (VO2) is a canonica

163 edge is used to track the insulator-to-metal phase transition in VO2 This technique allows observatio

164 proposed that organic aerosol can undergo a phase transition in which liquid-liquid phase separation

165 a new methodology to control liquid crystal phase transitions in anisotropic colloidal suspensions.

166 Information about EMT may also inform other phase transitions in cancer, such as those between prost

167 orm that uses light to activate IDR-mediated phase transitions in living cells.

168 en thermal changes can be giant near ferroic phase transitions in materials that display magnetic or

169 ize, show features of criticality known from phase transitions in physical systems.

170 f metallic quantum ferromagnets.The study of phase transitions in quantum ferromagnets has shown that

171 ntains genome stability and halts cell cycle phase transitions in response to DNA lesions that block

172 Here, we present direct measurements of phase transitions in single bilayers of 1,2-dimyristoyl-

173 Structural phase transitions in TMDs have so far been induced by th

174 long-wavelength fluctuations that influence phase transitions in two dimensions.

175 is a potential pathway to induce structural-phase transitions in two-dimensional materials.

176 To further investigate phase-transition in adipose tissue in microscopic level,

177 Landau-level indices reveal a cascade of FQH phase transitions, including a continuous phase transiti

178 hat exhibits no bulk classical thermodynamic phase transition, independent of the computational circu

179 splay an unusual, strongly hysteretic volume-phase transition indicating useful thermal memory proper

180 rance of the spanning cluster is marked by a phase transition, indicating that the system behaves in

181 no one reported the observation of structure phase transition induced by pressure.

182 Fluid phase transitions inside single, isolated carbon nanotub

183 Within this model, we observe phase transitions into spatially ordered states that bre

184 t-principles calculations indicate that this phase transition is driven by the relative phase stabili

185 The compositions where the phase transition is observed agree well with the theoret

186 omalous valence crossover without structural phase transition is observed in archetypal cubic YbCu5 b

187 This characteristic phase transition is of significant biological and biophy

188 The phase transition is only observable by fluorescence quen

189 Accordingly, percolation phase transition is proposed as a new test bed, which de

190 paradigmatic example of a continuous quantum phase transition is the transverse field Ising ferromagn

191 becomes metastable close to a thermodynamic phase transition it can exhibit unique catalytic behavio

192 e gel-to-liquid crystalline (Lbeta - Lalpha) phase transition, leading to a large Lbeta/Lalpha phase

193 The NAO/AO phase transition leads to a rapidly strengthened Siberia

194 er, a lack of tools to control intracellular phase transitions limits our ability to understand their

195 Phase-transition materials are able to provide real-time

196 ombination of Fourier transform infrared and phase transition measurements as well as molecular compu

197 and NdNiO3 , which undergo a metal-insulator phase transition (MIT), the origin of which is still und

198 arameter, we show that it drives the thermal phase transition near 200 kelvin in Cd2Re2O7 and induces

199 rovskite is maintained through the different phase transitions observed as a function of temperature.

200 fied and additional insight on the nature of phase transitions obtained.

201 rent space group of C2(5), indicating that a phase transition occurred during further compression.

202 e identify the parity-time symmetry-breaking phase transition occurring in spin-transfer torque-drive

203 The phase transition occurs as monovalent salts are used to

204 We find that the insulator-to-metal phase transition occurs on a timescale of 26 +/- 6 fs an

205 Moreover, this structural phase transition occurs simultaneously across the whole

206 ase separation, the mechanisms by which this phase transition occurs, and the resultant morphologies

207 suggest that a sequence of symmetry-breaking phase transitions occurs as temperature is lowered: firs

208 ow that depletion of EZH2 suppresses G1 to S phase transition of GC B cells in a Cdkn1a-dependent man

209 with the reported orthorhombic-to-tetragonal phase transition of La2NiO4+delta.

210 superconducting dome, unveiling the quantum phase transition of local character.

211 mperatures above and below the gel to Lalpha phase transition of milk-SM (Tm approximately 34 degrees

212 iquid expanded (LE) to liquid condensed (LC) phase transition of milk-SM monolayers was observed at s

213 mechanistically designing a liquid-to-solid phase transition of oxidized catholyte (or reduced anoly

214 the lamellar-to-inverted hexagonal (L - HII) phase transition of POPE.

215 the first time, experimentally revealed the phase transition of ThC from B1 to P4/nmm at pressure of

216 ther enhances the pressure and can lead to a phase transition of the trapped material.

217 Here, by exploiting the hysteretic phase transition of vanadium dioxide, an all-solid, rewr

218 rmation of metastable phases in photoinduced phase transition of VO2 are elucidated through ultrafast

219 nal lattice when subjected to two structural phase transitions of BaTiO3 (001) single crystal substra

220 ions of vibrational spectroscopy in studying phase transitions of ionic liquids.

221 Phase transitions of linear multivalent proteins control

222 information in disordered linkers influences phase transitions of multivalent proteins.

223 s of the atoms, one can experimentally study phase transitions of open quantum systems.

224 The opposite influence on the two-phase transitions of POPE brings a three-phase coexisten

225 amined the crystal structures and structural phase transitions of the deuterated, partially deuterate

226 on tyrosine residues that are necessary for phase transitions of the EWSR1 prion-like domain.

227 The complex phase transitions of vanadium dioxide (VO2) have drawn c

228 tudies that address the implications of this phase transition on climate-related properties of aeroso

229 ation, we studied the dependence of magnetic phase transition on exchange interaction strength.

230 s electrostatic-doping control of structural phase transition opens up new possibilities for developi

231 The LCST phase transition originates from the interaction between

232 s signed unipartite network, which reveals a phase transition phenomenon.

233 The applications of photoinduced phase transitions, photoalignment, photomodulation of ch

234 ition, both the second-order and first-order phase transition points can be decreased by increasing t

235 The mass spectrometry experiment confirmed phase transition polymerization, with mainly trimer and

236 This rapid phase transition produces numerous vacancies and defects

237 on takes place through a genuine first-order phase transition, provided that the interconnected pores

238 ersal features of the first and second order phase transition (PT) depending on the PEL for two polar

239 al theoretical approaches to non-equilibrium phase transitions remain scarce.

240 with a small number of dependency links, the phase transition remains second-order.

241 The droplet-generating phase transition responded to modification of even a sin

242 We find that the phase transition shows a hysteretic loop in Raman spectr

243 Phase transitions significantly differ between 2D and 3D

244 Universality is key to the theory of phase transitions, stating that the equilibrium properti

245 vity over a broad temperature range, diffuse phase transitions, strong frequency dependence in dielec

246 crease the fraction of dependency links, the phase transition switches from second-order to first-ord

247 ature first-order field-induced metamagnetic phase transitions (T N = 58 K) and high spontaneous pola

248 one transitions away from the ferroelectric phase transition (TC).

249 Phenolic compounds also increased phase transition temperature (Tc) of nanoliposomes (2.01

250 in films which results in an increase in the phase transition temperature as thickness is reduced.

251 l dichalcogenide semimetal 1T-TiSe2 Near the phase-transition temperature (190 kelvin), the energy of

252 33 of 185 picocoulombs per newton and a high phase-transition temperature of 406 kelvin (K) (16 K abo

253 properties and lipid vesicles with different phase transition temperatures.

254 e pronounced effects on observables, such as phase-transition temperatures.

255 materials, particularly in the case of high phase-transition temperatures.

256 Light is used to initiate the final gel-sol phase transition that disrupts the hydrogel network, all

257 ct may be viewed as a unique type of quantum phase transition that is driven by the size of the syste

258 imal model systems that exhibits solid-solid phase transitions that are driven by changes in the shap

259 In optics, the abrupt nature of the phase transitions that are encountered around exceptiona

260 neer quantum spin liquids and access elusive phase transitions that are not readily accessible in equ

261 , the growing simplicial complex can undergo phase transitions that are reflected by relevant changes

262 However, such mappings display thermodynamic phase transitions that may prevent reaching solution eve

263 Here we observe and study a non-equilibrium phase transition, the condensation of supermode-density-

264 is, we have found that close to the Cu2O-CuO phase transition there is a boost in activity for a kine

265 The delay in phase transition (theta --> alpha), and alteration of po

266 er the claims of the record pressure nor the phase transition to a metallic state are supported by da

267 itinerant electrons tuned through a quantum phase transition to an Ising nematic phase.

268 red in a single shot, enabling the dynamical phase transition to be probed directly and revealing com

269 ins reveal that they undergo an irreversible phase transition to cylindrical domains under the electr

270 sp(2) carbon framework induces ferromagnetic phase transition to develop spin-spin coherence and alig

271 probability distributions, interpreting this phase transition to indicate a critical tuning of the ne

272 Cu(+) ion intercalation leads to a permanent phase transition to intrinsic low-chalcocite Cu2S nanocr

273 us to use the physical theory of first-order phase transitions to understand the onset of rapid cycli

274 ycomb lattice is expected to exhibit several phase transitions to unique magnetic states as a functio

275 Cr-doped Bi2(SexTe1-x)3, a magnetic quantum phase transition tuned by the actual chemical compositio

276 Both materials exhibit a rocksalt-to-MnP phase transition under compression with ca. 22 % unit-ce

277 riginates from rhombohedral-tetragonal (R-T) phase transition under electric-filed, and is recoverabl

278 d provide a useful model system for studying phase transitions under confinement.

279 Our investigation of the structural phase transitions under the influence of an external ele

280 e attributed to the elimination of the P2-O2 phase transition upon cycling to 4.5 V.

281 als that the material undergoes a reversible phase transition upon K extraction and insertion.

282 In this critical review, the phase transitions upon encapsulation of more than 130 am

283 he size-dependent orthorhombic-to-tetragonal phase transition using a combined temperature-dependent

284 Tailoring structural phase transitions using alloying is a novel idea with im

285 that occurs indirectly in atomic solid-solid phase transitions via changes in temperature, pressure,

286 However, a low-temperature phase transition was experimentally detected to a struct

287 ttice displacements near the charge ordering phase transition, we directly visualize the local compet

288 Using the Abeyaratne-Knowles formulation of phase transitions, we developed a new theoretical method

289 t that the polymorphs can be on the verge of phase transitions when heated as low as ~400 degrees C.

290 ory: The mechanical yield is a thermodynamic phase transition, where yield occurs as a spinodal pheno

291 Phase transitions, where observable properties of a many

292 ound states and uncover a remarkable quantum phase transition whereby the entanglement scaling change

293 n the possibility that this is a first-order phase transition which provides evidence that the real n

294 Despite the first-order phase transition with a large lattice mismatch between t

295 ycrystalline samples have identified a 105-K phase transition with a pronounced electronic and magnet

296 he imidazolium ion and M=Fe, Co, undergo two phase transitions with temperature; at low temperatures

297 the other hand, macroscopic observations of phase transitions, with millisecond or longer time resol

298 ries of isochoric, diffusionless solid-solid phase transitions within a single shape family and find

299 , incorporating realistic rheology and major phase transitions, yielding a model slab that is nearly

300 More importantly, the phase transition yields a three orders of magnitude incr