ライフサイエンスコーパス: phase diagram

1 the metastable or the spinodal region of the phase diagram.

2 immiscible according to the Co-Mo bimetallic phase diagram.

3 ability conditions of both species through a phase diagram.

4 ferent regions of magnetic field-temperature phase diagram.

5 binding energies at every point in the alloy phase diagram.

6 t belong to the ambient-pressure PbS-PbBr(2) phase diagram.

7 ems to thin films additionally affects their phase diagram.

8 y liquid (LDL) in the metastable part of the phase diagram.

9 la: see text]-[Formula: see text]) transport phase diagram.

10 and burstiness and we analytically study its phase diagram.

11 neighbors a magnetically ordered one in the phase diagram.

12 mmensurate charge-density-wave states in the phase diagram.

13 LaCrGe3 exhibits both these features in its phase diagram.

14 r, allowing them to directly reconstruct the phase diagram.

15 hat are absent in the native block copolymer phase diagram.

16 in the universe, has a surprisingly complex phase diagram.

17 ent antiferromagnetic (LMAFM) regions of the phase diagram.

18 ns govern the larger part of the geometrical phase diagram.

19 he entire overdoped side of the La2-xSrxCuO4 phase diagram.

20 and fields H, we construct a detailed vortex phase diagram.

21 nt and throughout the metastable fluid-fluid phase diagram.

22 tures that map onto known regions of water's phase diagram.

23 ithin a narrow range of concentration in the phase diagram.

24 phase introduced to the state-of-the-art T-P phase diagram.

25 tion as a function of F or q, resulting in a phase diagram.

26 COFs into the antiferromagnetic side of the phase diagram.

27 the capillary number (Ca)-viscosity ratio(M) phase diagram.

28 n and analysis of changes in parameter A and phase-diagram.

29 utilizing pseudodoping to control electronic phase diagrams.

30 A structural stability is encoded within the phase diagrams.

31 s have enabled the exploration of their rich phase diagrams.

32 e at incremental fluences, as well as linear phase diagrams.

33 g the accessibility of target regions in the phase diagrams.

34 protein interactions for the construction of phase diagrams.

35 by computing or measuring sequence-specific phase diagrams.

36 enable the calculation of sequence-specific phase diagrams.

37 f domains, in excellent agreement with known phase diagrams.

38 are typically not accessible on equilibrium phase diagrams.

39 ttributes associated with eutectic points in phase diagrams.

40 n approaches by also being able to interpret phase diagrams.

41 over an extended regime in their respective phase diagrams.

42 rance cannot be anticipated from traditional phase diagrams.

43 ucting phase forms a dome-shaped area in the phase diagram(1).

44 of the lowest-energy regions of the computed phase diagram affords two materials with previously unre

45 Construction of a partial phase diagram allowed us to determine the criteria for t

46 The phase diagrams also revealed a semi-compact intermediate

47 Phase diagram analysis shows the existence of only two p

48 n of a quasi de Almeida-Thouless line in the phase diagram and a logarithmic time dependence of the m

49 When combined with the protein phase diagram and a tailored patchy particle model, we s

50 sitions and concentration regimes within the phase diagram and are formed through the phase separatio

51 Helium has a unique phase diagram and below 25 bar it does not form a solid

52 is, it can mimic the model and simulate its phase diagram and dynamics(4,5)), has a vital role in so

53 We fingerprint the transient phase diagram and find a stable photo-induced chiral spi

54 aracterized portion of the phosphorus-sulfur phase diagram and has therefore been subjected to a rang

55 quid and non-compressed fluid domains on the phase diagram and is supported by calculations within th

56 ces reveal details about the superconducting phase diagram and its relationship to the nearby insulat

57 xists only in a narrow region of the Ti-Al-C phase diagram and readily reacts with Al.

58 We study the phase diagram and the pseudogap phenomena throughout the

59 Both the phase diagram and the relative superfluid fraction of th

60 fferences relate both to the topology of the phase diagram and to the nature of the transitions, with

61 The respective phase diagrams and "tie-surfaces" were determined, follo

62 erest due to the discovery of rich proximate phase diagrams and unusual quantum coherence phenomena.

63 aviors, such as threshold energy, linewidth, phase diagram, and angular dispersion are verified.

64 iform everywhere on the pressure-temperature phase diagram, and to change only in a monotonic way eve

65 ink collective behavior, captured in protein phase diagrams, and molecular-level details, determined

66 By mining data from hundreds of experimental phase diagrams, and thousands of thermodynamic data sets

67 monstrate that, by solubility design using a phase diagram approach, the filling fraction limit (FFL)

68 y-coupled layer is magnetically active, rich phase diagrams are expected in FeSCs, but this has not b

69 A general procedure for constructing the phase diagram as a function of system composition f and

70 We construct a phase diagram as a function of twist angle and displacem

71 of a magnetic field reveals a wing-structure phase diagram as seen in itinerant ferromagnets such as

72 important for a proper interpretation of the phase diagram as well as practical modeling of high-temp

73 First, we study phase diagrams as a function of macromolecule concentrat

74 We find that these phase diagrams as a function of pH strongly depend on wh

75 that greigite is a stable phase in the Fe-S phase diagram at ambient temperature.

76 Here, we construct a comprehensive phase diagram based on detailed magnetization measuremen

77 capture these behaviors with a jamming-like phase diagram based on local cell density and EGF.

78 te rung coupling dramatically simplifies the phase diagram below half-saturation magnetization by sta

79 high-precision torsion pendulum, and map the phase diagram between 0.1 and 5.6 bar.

80 n asymmetric and symmetric structures in the phase diagram by 30 gigapascals.

81 f catalytic activities at every point in the phase diagram can be created, enabling the identificatio

82 While the equilibrium phase diagram can be fit to an analytical theory, a more

83 We show that the triangular phase diagram can be generalized to other topological se

84 However, a much richer electronic phase diagram can emerge and, in the specific case of Cr

85 A phase diagram capturing the structural changes as functi

86 ian case, this model presents an interesting phase diagram characterized by two quantum criticalities

87 ur in materials like ice having an anomalous phase diagram characterized with dTm/dP < 0, where Tm is

88 ield-Hall conductivity (E(F)-E(z)-sigma(xy)) phase diagrams clearly exhibit oscillatory behaviors and

89 ment of our experimental results both with a phase diagram computed on the basis of the volume access

90 ic point of the macromolecules and study how phase diagrams depend on pH.

91 t-ordered states, we calculated and analyzed phase diagrams dependence on the film-substrate mismatch

92 We characterize the phase diagram determining the minimal volume of transact

93 of scaffolds, with a sharp switch across the phase diagram diagonal.

94 tween these two factors gives rise to a rich phase diagram displaying high diversity in aggregated st

95 dependence and hysteretic dynamics over the phase diagram due to the impacts of complex slow inactiv

96 Construction of a suitable phase diagram enables each of these three morphologies t

97 and subsequent construction of an empirical phase diagram (EPD).

98 gs along the drop wall, as demonstrated by a phase diagram established here, with different power-law

99 both low- and high-concentration regions of phase diagrams establishes an important role for electro

100 We show how the topology of the phase diagram evolves from the known case of (4)He, as t

101 The corresponding phase diagrams exhibit increased compositional resolutio

102 We determined the surface phase diagram, explored the possible reaction pathways i

103 determination of an equilibrium (solubility) phase diagram for a real amyloid-forming peptide, Abeta(

104 quantitative calculation of a thermodynamic phase diagram for a specific peptide requires extremely

105 We demonstrate a phase diagram for air evolution regarding hydrodynamics.

106 The proposed mechanism gives rise to a phase diagram for cellular memory that may be generally

107 particle-network model, we first establish a phase diagram for compression-driven, stretching-dominat

108 A dynamic phase diagram for non-linear flow was created to describ

109 an equilibrium concentration and temperature phase diagram for the amyloidogenic peptide fragment Abe

110 An experimental phase diagram for the formation of Ag nanocubes as a fun

111 ; we can thus present a structural stability phase diagram for the LnAuZ (Z = Ge, As, Sn, Sb, Pb, Bi)

112 We have established a rich phase diagram for these topological superconducting stat

113 ry-aided computations through calculation of phase diagrams for a set of archetypal intrinsically dis

114 We calculate the phase diagrams for both 2D and 3D systems and compare th

115 s emerges from the ellipsoidal structures of phase diagrams for multicomponent systems and it has dir

116 ctions) that enables the calculation of full phase diagrams for multicomponent systems comprising of

117 urn, this permits us to compute ground-state phase diagrams for multicomponent systems.

118 our experimental observations and establish phase diagrams for QAH insulators with high, tunable Che

119 construct magnetic field, temperature (H, T)-phase diagrams for the 200 nm-thick Er sample that serve

120 model is then combined with the data-driven phase diagram generation tool to expand the limited numb

121 The hydrogen phase diagram has several unusual features which are wel

122 gime from the corners towards the centers of phase diagrams has led to worldwide attention by materia

123 The obtained phase diagram highlights unique features of FeSe among i

124 This relies on two crucial features of the phase diagram: (i) the marginal stability of the free-en

125 We deduce a phase diagram identifying key regimes for the dynamics (

126 ions of [Formula: see text] and construct a 'phase diagram' identifying different phylodynamic regime

127 ons are enforced by the anomalies in a whole phase diagram in sharp contrast to the case of the Landa

128 Using numerical simulations, we present a phase diagram in strain-friction space that shows chaoti

129 red to the case of salt-free conditions, the phase diagram in the presence of high-saline buffer (bot

130 effects are crucial in understanding of the phase diagram in these materials.

131 etric determination of the field-temperature phase diagram in underdoped YBa2Cu3Oy single crystals.

132 Formula: see text] to construct the magnetic phase diagram in untwinned crystals with hole density p

133 surprising results by invoking the notion of phase diagrams in higher dimensional parameter space.

134 Each phase diagram included hydrate and anhydrate deliquescen

135 It exhibits a rich phase diagram including a supersolid phase where a latti

136 d to access different parts of electron-hole phase diagram, including BEC-BCS crossover, enabling tan

137 We observe a complex phase diagram, including phases with chain and square ar

138 The phase diagrams indicate that a crucial role is played by

139 Accordingly, we introduce several phase-diagram inspired parameters and employ machine lea

140 nature of a quantum critical point in their phase diagram is a central enigma of the high-temperatur

141 a that characterizes hard-sphere models, the phase diagram is a function of an additional parameter t

142 A morphological phase diagram is accomplished to systematically evaluate

143 Using this methodology, a borophene phase diagram is assembled, including a transition from

144 Moreover, the universal QAHE phase diagram is confirmed through the angle-dependent m

145 n original magnetic field-versus-temperature phase diagram is constructed to indicate the region of s

146 A quantitative phase diagram is constructed to rationally select parame

147 The theoretical chirality phase diagram is found to be in excellent agreement with

148 zone centre (Gamma point), whose topological phase diagram is mapped out in the parameter space of or

149 Furthermore, a fruitful phase diagram is obtained by controlling the direction o

150 Knowledge of such a phase diagram is of potential importance to applications

151 A three-dimensional phase diagram is proposed to illustrate the collaborativ

152 A more direct method based on the phase diagram is proposed to observe and determine tripl

153 A partial phase diagram is proposed.

154 om this fact the transport and thermodynamic phase diagram is reproduced in detail.

155 anation for the missing ice phase in the T-P phase diagram is that ice chi is a rare polarized ferroe

156 well below room temperature and the magnetic phase diagram is unknown.

157 d through intrinsic fluorescence parameters, phase diagram method, and quenching experiments using ac

158 chroism and tryptophan fluorescence, and the phase-diagram method.

159 pct.) via CALPHAD (CALculation of PHAse Diagram) modeling and experimental validation.

160 We reveal a strongly non-mean-field-like phase diagram, much richer than the common local-moment

161 rplay between the two orders and the complex phase diagram near the pseudogap critical point.

162 In the resulting phase diagram, next to configurations predicted earlier

163 The superconducting phase diagram of (6)Li is compared with that of (7)Li th

164 to construct a detailed temperature-pressure phase diagram of a material on the border of a ferroelec

165 High-pressure melting anchors the phase diagram of a material, revealing the effect of pre

166 ntalization exploits general features of the phase diagram of a multicomponent biomolecular mixture.

167 ent a comprehensive theoretical study of the phase diagram of a system of many Bose particles interac

168 We experimentally determined the full phase diagram of an IgG antibody.

169 ps to the valley or spin quantum numbers.The phase diagram of bilayer graphene at high magnetic field

170 The solid-phase diagram of binary systems consisting of particles

171 We resolved the crystal structure and phase diagram of borophene on Ag(111), but found that th

172 tal orbital degeneracy, leading to a complex phase diagram of broken symmetry states.

173 We derived a phase diagram of CO2 in ZIF-7, which exhibits surprising

174 lated flat electronic bands that host a rich phase diagram of correlated insulating, superconducting,

175 Here we present a theoretical study of the phase diagram of dense hydrogen that uses machine learni

176 A specific pressure-temperature (P-T) phase diagram of Eu(Fe0.925Co0.075)2As2 is established.

177 phases under strain is investigated, and the phase diagram of FGT in the strain-temperature plane is

178 in iron and the complex pressure-temperature phase diagram of gadolinium.

179 Unfolding events were registered in the phase diagram of glutenins up to 80 degrees C, followed

180 Here we report the high-magnetic field phase diagram of graphite to exhibit just such a crossov

181 on fundamentally changes the superconducting phase diagram of H3S.

182 icate a non-Fermi liquid phase in the global phase diagram of heavy fermion metals.

183 The phase diagram of high-pressure hydrogen is of great inte

184 ta may require a significant revision of the phase diagram of hydrogen above 200 GPa.

185 s in the temperature-pressure-magnetic field phase diagram of LaCrGe3.

186 he unusual dependence of the superconducting phase diagram of lithium on its atomic mass opens up the

187 ic method to investigate the low-temperature phase diagram of lithium.

188 example of an additional possibility for the phase diagram of metallic quantum ferromagnets.The study

189 how magnetic fields affect dramatically the phase diagram of mixed Bose-Fermi systems, switching bet

190 port study on the many-body collective-order phase diagram of NbSe2 down to a thickness of one monola

191 ork sizes affect the synchronization and its phase diagram of NONs coupled with nonlinear dynamics.

192 gnetic (LMAFM) phases and established the 3D phase diagram of T-H-x In the HO phase, H/H0 scales with

193 Finally, a phase diagram of tetragonal FeS as functions of pressure

194 In this work we construct the phase diagram of the BZT-xBCT system using a generic six

195 in the bulk of the sample and may affect the phase diagram of the correlated and superconducting stat

196 te Carlo to study the supersolid part of the phase diagram of the extended Bose-Hubbard model on the

197 o experimentally mapping the low-temperature phase diagram of the Fermi-Hubbard model as a function o

198 rimetry were employed to construct a partial phase diagram of the GM1/POPC system.

199 ere remain fundamental open questions on the phase diagram of the Hubbard model, which describes stro

200 We investigate the high-pressure phase diagram of the hydrous mineral brucite, Mg(OH)2, u

201 actual Mott insulator can be realized in the phase diagram of the iron pnictides remains an open ques

202 y fermion metals, we theoretically study the phase diagram of the Kondo lattice model with a nonmagne

203 The phase diagram of the model is similar to the single-fila

204 z for the scale-free networks and obtain the phase diagram of the model.

205 The predicted phase diagram of the N-H system also provides a referenc

206 computed viscosity data, [Formula: see text] phase diagram of the phase transitions of confined water

207 valuate the finite-temperature pseudo-binary phase diagram of the Ti2AlC-Cr2AlC via first-principles-

208 tively monitored, and a pressure-temperature phase diagram of the topotactic transformation is constr

209 Here we obtain the phase diagram of the two-dimensional triangular-lattice

210 , by exploiting the metastable region of the phase diagram of thermally responsive IDPs within microd

211 As a result, the phase diagram of these mixtures is characterized by an e

212 The phase diagram of these ternary mixtures can be studied e

213 We study the phase diagram of this model numerically as a function of

214 obtained here we have constructed a magnetic phase diagram of UN.

215 The phase diagram of water harbors controversial views on un

216 The richness of the phase diagram of water reduces drastically at very high

217 The pressure-temperature phase diagram of ZIF-4 is strikingly complicated when co

218 For this purpose, the pseudoternary phase diagrams of canola oil/lecithin:n-propanol/water m

219 We predicted phase diagrams of CH4, C3H6, and C4H10.

220 Comparisons between the P-T phase diagrams of Eu(Fe0.925Co0.075)2As2 and the parent

221 This is the first report of RH-temperature phase diagrams of glucose and citric acid, information w

222 lly, we apply the DroMiCo to the analysis of phase diagrams of macromolecules, including synthetic po

223 By comparing our results to the partial phase diagrams of other IgGs reported in literature, we

224 Phase diagrams of pollen folding pathways indicate that

225 The rich finite temperature phase diagrams of the effective spin models for fermions

226 RH-temperature phase diagrams of the food ingredients alpha-d-glucose a

227 description of the topological phase space (phase diagram) of the stability of the human telomere fr

228 attracting growing interest since their rich phase diagram often translates into an equally rich out-

229 angle and strain, the dependence of the TBG phase diagram on the alignment(4,6) and thickness of the

230 These findings and HOP phase diagrams open a pathway to a large family of collo

231 ses noticeably, which is consistent with the phase diagram (PD) of cuprates.

232 A phase diagram pressure - milk-SM/cholesterol composition

233 This investigation revealed rich phase diagrams, previously unobserved phase transitions

234 The observed dome-shaped superconductivity phase diagram provides insights into the interplay betwe

235 ual magnetic properties, they possess a rich phase diagram (ranging from an unfrustrated square latti

236 angle' of twist of about 1.1 degrees, with a phase diagram reminiscent of high-transition-temperature

237 The resulting pressure-temperature phase diagram reveals four, previously unknown, high-pre

238 The obtained strain-magnetic field phase diagram reveals that C(4) -symmetry-breaking aniso

239 The resulting phase diagrams show that perturbations to folding by eac

240 Using the Hall angle, we construct a phase diagram showing how the excitations are suppressed

241 the assembly can be recast into a universal phase diagram showing that viruses with high mechanical

242 -line to metallic lithium on the equilibrium phase diagram), so this Coble creep mechanism can effect

243 fy a metastable domain in the global network phase diagram spanned by the model's control parameters

244 observed crawling behavior in the dynamical phase diagram, such as self-trapped localized motion, 2-

245 Moreover, in a large region of the phase diagram, superconductivity sets in from a ferromag

246 reduction reaction, finding 2 regions in the phase diagram that are predicted to result in highly act

247 model for such systems and find a very rich phase diagram that becomes increasingly more complex as

248 thermodynamic phase, and construct a unified phase diagram that can quantitatively predict various ty

249 Binary mixtures of these molecules have a phase diagram that contains dilute liquid, dense liquid,

250 Establishing a phase diagram that delineates the boundaries of phase co

251 We predict a phase diagram that describes how the disruption of cytos

252 By varying f and C, we calculated the phase diagram that shows a sequence of structural transi

253 Our theoretical model culminates in phase diagrams that accurately predict the elastic respo

254 Finally, we generate Pourbaix phase diagrams that serve as a thermodynamic atlas to in

255 nn calculations, which allow us to create a 'phase diagram' that characterizes the electron flow regi

256 es include the astonishing complexity of the phase diagram, the unprecedented prominence of various f

257 quence we find in the plane gamma - p of the phase diagram three distinct phases.

258 , a phenomenological method analysing binary phase diagrams to predict HEA phases is presented.

259 This allowed a phase-diagram to be constructed that can be extended to

260 om our observations a schematic denaturation phase diagram together with energy landscapes for the tw

261 We find a rich variety of phase diagram topologies, including multiple critical po

262 ally explore different regions of the carbon phase diagram traversed during detonation.

263 ambient conditions, has a surprisingly rich phase diagram under pressure, taking up several structur

264 of the energy landscape of the Li-CO2 binary phase diagram using ab initio evolutionary structure sea

265 ulations, which include complete topological phase diagrams using different values of the Hubbard pot

266 Equilibrium temperature-composition phase diagrams using first-principles calculations are g

267 crystal structure prediction, polymorphism, phase diagrams, vibrational spectroscopies, and nuclear

268 dense and a dilute phase; the corresponding phase diagram was computed.

269 ses have been successfully identified, and a phase diagram was constructed for the single bilayer bin

270 The phase diagram was determined using epifluorescence micro

271 nd RuO2-(1 x 1), were found, and the surface phase diagram was determined.

272 Moreover, by means of a phase diagram we can classify societies according to the

273 Guided by our phase diagram, we show that tau can be driven toward LLP

274 composition dependence of field-temperature phase diagrams were constructed, which provide compositi

275 lopment in Caenorhabditis elegans, implies a phase diagram where cell-fate choices are displayed in a

276 even nematic order in TBG in regions of the phase diagram where superconductivity is observed.

277 This yields a unique phase diagram where the second-order phase transition li

278 We look in and around the region of the phase diagram where three phases are expected and use a

279 We take advantage of a theoretically derived phase diagram, where the phenomenon of excitability is r

280 attices observed to date are featured in our phase diagram, whereas several more are predicted for fu

281 alts slightly increased the W/O areas on the phase diagrams, whereas pH variation was not effective o

282 r previously unrecognized classes of surface phase diagram which differ from that established for sim

283 We show that the system can have a similar phase diagram which is discussed in the Haldane's model.

284 an be elegantly obtained from a topological 'phase diagram', which provides a guiding principle for t

285 s possible to establish a carrier scattering phase diagram, which can be used to select reasonable st

286 been proposed in the underdoped part of the phase diagram, which corresponds to a regime of maximum

287 Our stability analysis unveils a very rich phase diagram, which features stable, bistable, and unst

288 model allows the calculation of a stability phase diagram, which shows that, under physiological con

289 llows us to analytically compute topological phase diagrams, which determine quantized observables li

290 ain optimal dosage protocols and establish a phase diagram with an error threshold delineating parame

291 A rich phase diagram with noncollinear twisted phases is obtain

292 We further validate the phase diagram with our experiments on surface instabilit

293 Comparing the phase diagram with theoretical results, the strain-tunab

294 i and LaSb, we construct a temperature-field phase diagram with triangular shape that illustrates how

295 Moreover, this process results in a rich phase diagram with two fundamentally different types of

296 ss structural metals by combining calculated phase diagrams with simple rules based on the phases pre

297 measurement of the full pressure-temperature phase diagram, with 10000 microwells.

298 We explain these results in light of the phase diagram, with dehydration-driven ionic strength in

299 ary simulations predict an extremely complex phase diagram, with new thermodynamically stable compoun

300 We find that TBBG exhibits a rich phase diagram, with tunable correlated insulator states