ライフサイエンスコーパス: phase diagram

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

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

3 and burstiness and we analytically study its phase diagram.

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

5 Ca2C3 and CaC2 have stability fields on the phase diagram.

6 atform for the systematic exploration of its phase diagram.

7 neighbors a magnetically ordered one in the phase diagram.

8 n the Zr-rich rhombohedral region of the PZT phase diagram.

9 allowing us to map out Hc2 across the doping phase diagram.

10 the second critical point in the miscibility phase diagram.

11 oducts that do not appear on the equilibrium phase diagram.

12 nsmission are quantified and summarized in a phase diagram.

13 n of the temperature (T) and hole-doping (p) phase diagram.

14 iples calculations, into a resultant generic phase diagram.

15 ibes all possible scenarios in a non-trivial phase diagram.

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

17 y we studied on the silicon-rich side of the phase diagram.

18 ems to thin films additionally affects their phase diagram.

19 LaCrGe3 exhibits both these features in its phase diagram.

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

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

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

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

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

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

26 ding a general framework to understand their phase diagrams.

27 freedom that lead to complex and interesting phase diagrams.

28 libria and thus can be rationalized by using phase diagrams.

29 particle and many-body physics leads to rich phase diagrams.

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

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

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

33 protein interactions for the construction of phase diagrams.

34 )Sr(2)CaCu(2)O(8+delta) samples spanning the phase diagram 0.06 </= p </= 0.23.

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

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

37 The phase diagrams also revealed a semi-compact intermediate

38 This mechanism leads to a rich phase diagram and allows for rational design of strong t

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

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

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

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

43 r with prior work gives insight into the p-T phase diagram and reveals the fundamental resistance per

44 We further show that both the experimental phase diagram and the observed phase evolution can be ex

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

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

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

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

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

50 s been thoroughly investigated, described in phase diagrams, and theoretically rationalized in terms

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

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

53 Phase diagrams are determined from extremes of thermodyn

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

55 However, equilibrium phase diagrams are of very limited use for the reconstit

56 ne/methanol/water and heptane/methanol/water phase diagrams are very similar at room temperature.

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

58 material system, mapping out the structural phase diagram as a function of temperature and hydrogen

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

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

61 parameters, we identified ternary (kinetic) phase diagrams at specific compositions (i.e., Si, Al, a

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

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

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

65 n coarsening dynamics, but alters the static phase diagram by creating a jump in (thermodynamic) pres

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

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

68 A phase diagram capturing the structural changes as functi

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

70 ical techniques and simulations, we obtain a phase diagram characterizing a first-order transition be

71 lation of electronic and crystal structures, phase diagrams, charge distributions, vibrational freque

72 The phase diagram clearly shows that increasing unsaturated

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

74 common ways, leading to a universal jamming phase diagram conjecture.

75 lar weight (MW) was investigated by means of phase diagram construction, rheometry, fluorescence micr

76 The microemulsion region of a ternary phase diagram containing short chain monoglycerides was

77 or the construction of three lipid-component-phase diagrams containing cholesterol.

78 ition: for a certain region in the (k/n,n/N)-phase diagram, convex optimization typically finds the s

79 t is not only able to reproduce the original phase diagram detailing regions of known crystals, but i

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

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

82 A simple phase diagram encompasses the variety of patterns that c

83 interactions, which generate unconventional phase diagrams encompassing fluid, gel and glassy states

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

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

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

87 In particular, the pseudogap regime of the phase diagram exhibits a variety of mysterious emergent

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

89 A dynamic phase diagram expressed in terms of transcription speed,

90 Over large regions of the phase diagram, fitness increases with increasing fidelit

91 the droplet interaction potential maps out a phase diagram for adhesion as a function of force and sa

92 We derive a phase diagram for amorphous solids and liquid supercoole

93 p (EM) for the nanostructure, analogous to a phase diagram for bulk materials, which fully characteri

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

95 The phase diagram for FFLO superfluids is obtained in the BC

96 ates Ostwald's Rule of Stages and provides a phase diagram for growth of CdSe QDs exhibiting a specif

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

98 We propose a new phase diagram for sediment transport, where 'bed load' i

99 We determine a phase diagram for skyrmion formation and reveal the effi

100 While our results reveal a remarkable phase diagram for the binary superlattice, the mechanism

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

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

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

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

105 We construct phase diagrams for the possible coiling patterns and cha

106 underdoped region of the temperature-doping phase diagram from which superconductivity emerges is re

107 ations in La(2-x)Sr(x)CuO4 across the entire phase diagram, from a strongly correlated insulator (x =

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

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

110 However, mapping out the phase diagram in a confined geometry has been experiment

111 structure to be uncompetitive, and predict a phase diagram in reasonable agreement with experiment.

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

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

114 icrostructural properties and have derived a phase diagram in the parameter space spanned by loading

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

116 chemes emerge as characteristics of the Li-B phase diagram in this ground-state theoretical investiga

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

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

119 Each phase diagram included hydrate and anhydrate deliquescen

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

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

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

123 The phase diagram indicated the existence of at least two di

124 Phase diagrams indicated that the compatibility of the b

125 high rates, whereas its lithium-composition phase diagram indicates that it should react via a kinet

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

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

128 This phase diagram is consistent with quantitative studies of

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

130 A quantitative phase diagram is constructed to rationally select parame

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

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

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

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

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

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

137 A partial phase diagram is proposed.

138 ct of thermal fluctuations on the mean-field phase diagram is that it permits a direct transition bet

139 We find strong evidence that, as the phase diagram is traversed through superconductivity tow

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

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

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

143 ally controlled, rather than governed by the phase diagram, nanocrystals of metastable and hitherto i

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

145 eneralized to the full temperature-dependent phase diagram, not just the crystal structures themselve

146 Thus, equilibrium phase diagrams obtained for protein-free lipid/detergent

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

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

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

150 In general, it is shown that the phase diagram of a soft repulsive potential leads to the

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

152 asis for the construction of a thermodynamic phase diagram of Au nanomolecules in terms of ligands an

153 A phase diagram of average lnalpha versus lnomega identifi

154 The phase diagram of BaPb(1-x)Bi(x)O3 exhibits a superconduc

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

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

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

158 Furthermore, we explore the phase diagram of cell motility by varying myosin II acti

159 The phase diagram of CO(2) includes several non molecular ph

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

161 whose resolution is needed to elucidate the phase diagram of copper oxides.

162 We show that the phase diagram of coupled leaflets allows multiple metast

163 The phase diagram of Cr-H system at high pressures remains l

164 l equation of state, effectively relates the phase diagram of DNA solutions for monovalent salts to t

165 An understanding of the phase diagram of elemental plutonium (Pu) must include b

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

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

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

169 on fundamentally changes the superconducting phase diagram of H3S.

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

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

172 Establishing the phase diagram of hydrogen is a major challenge for exper

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

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

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

176 We propose a new phase diagram of magnetite in which the temperature for

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

178 xplains migration transitions and predicts a phase diagram of migration phenotypes based on three mai

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

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

181 e, pressure and patch-size dependence of the phase diagram of open and close-packed structures.

182 e knot topology and introduce order into the phase diagram of possible structures.

183 However, the universal phase diagram of QAHE and its relation with quantum Hall

184 rochemical significance, many aspects of the phase diagram of solid carbon dioxide remain uncertain o

185 Here, we map the Frenkel line on the phase diagram of supercritical iron using molecular dyna

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

187 thod for the determination of tie lines in a phase diagram of ternary lipid mixtures.

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

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

190 The phase diagram of the carbon-hydrogen system is of great

191 ectron compounds are mapped onto the Doniach phase diagram of the competing RKKY and Kondo interactio

192 We provide a phase diagram of the DOPC/eSM/Chol mixture and predict t

193 road range of compositions, we constructed a phase diagram of the DPPC/DOPC/ergosterol system at 20 v

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

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

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

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

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

199 sed-tetragonal (cT) phases in the structural phase diagram of the iron-based superconductor AFe2As2 (

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

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

202 d materials requires an understanding of the phase diagram of the normal state.

203 Firstly, the phase diagram of the system was established.

204 t captures the quantitative structure of the phase diagram of the tensionless DPPC/DOPC/Cholesterol l

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

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

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

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

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

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

211 As a first approach, the phase diagrams of ATPS composed of different alcohol+ino

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

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

214 The phase diagrams of CI2 and protein G as a function of f a

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

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

217 Isosolid phase diagrams of mixtures of PMF/SHS showed eutectic fo

218 can predict the Gibbs free energies and thus phase diagrams of molecular crystals.

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

220 The folding phase diagrams of SH3 as a function of denaturant concen

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

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

223 Here, we present phase diagrams of vesicles composed of phosphatidylcholi

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

225 Phase diagrams offer a wealth of thermodynamic informati

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

227 hile strong interactions that mediate exotic phase diagrams open new avenues for engineering emergent

228 state-of-the-art experimentally established phase diagrams overwhelmingly dominated by molecular pha

229 continuation from the sphere that provides a phase diagram predicting that, for the same coordination

230 eroids and propose an analytical model and a phase diagram predicting the surface morphology evolutio

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

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

233 Phase diagrams provide 'roadmaps' to the possible states

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

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

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

237 A phase diagram showing regions in the temperature-concent

238 n in vitro genetic oscillator and mapped its phase diagram showing that steady-state conditions were

239 A phase diagram showing the crossovers into the different

240 A phase diagram showing the range of force transmission as

241 Mapping out the phase diagram shows a linear relationship between the di

242 We find that dsRNA has a force-torque phase diagram similar to that of dsDNA, including plecto

243 shold for superconductivity, and possesses a phase diagram similar to that of high-temperature superc

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

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

246 Furthermore, the calculated phase diagrams suggest that knowledge of the dominant as

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

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

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

250 imization is successful over a region of the phase diagram that coincides with the region known for G

251 A phase diagram that demarcates stable and unstable behavi

252 of both patterns, from which we construct a phase diagram that predicts a wrinkle-scar transition in

253 Our data imply a revised phase diagram that reconciles conflicting reports about

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

255 f the simulations are summarized in a global phase diagram that shows fibril, disordered oligomer, or

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

257 We provide phase diagrams that compare various trade-offs, includin

258 Due to the nature of their phase diagram, the modulus of compression of these membr

259 In the Si/C phase diagram, the only stable phases at P = 1 atm are t

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

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

262 Our proposed phase diagram thus has a first-order phase transition ju

263 ther a QCP must be present in the material's phase diagram to induce non-Fermi liquid behavior and tr

264 c light scattering was utilized to construct phase diagrams to identify suitable conditions for the s

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

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

267 in nature, has an exceedingly well-explored phase diagram under pressure, up to and beyond 100 GPa.

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

269 derstanding performance, we examine the Li-S phase diagram using computational techniques and complem

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

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

272 r concentrations, a systematic morphological phase diagram was constructed for the series of PS(n)-AC

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

274 The NIC-RMA binary phase diagram was constructed that contains the congruen

275 A PEG113-PHPMA(x) phase diagram was constructed to enable the reproducible

276 The phase diagram was determined using epifluorescence micro

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

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

279 The phase diagram we predict includes a nonequilibrium tripl

280 In addition to constructing the topological phase diagram, we are able to visualize the microscopic

281 ME formulations from the same pseudo-ternary phase diagram were investigated with respect to their ph

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

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

284 compositions lie in a region of the PbS-SnS phase diagram where no single phase exists, and despite

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

286 f water in a scarcely explored region of the phase diagram, where water is both supercooled and at ne

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

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

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

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

291 sible to study ferromagnetism over a broader phase diagram, which includes the orthorhombic Imma and

292 It is expected that the unified phase diagram will not only advance the understanding of

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

294 In a phase diagram with such a re-entrant melting, kinetic tr

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

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

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

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

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

300 e center and on the lithium-rich side of the phase diagram, Zintl-phase considerations, i.e., bonding