ライフサイエンスコーパス: equilibrium state

1 is distribution is generally not the fitness-equilibrium state.

2 odynamic entropy production in a stable, non-equilibrium state.

3 rgy is released as the system reverts to its equilibrium state.

4 associations occurring at the thermodynamic equilibrium state.

5 ocations that stabilizes the strain-relieved equilibrium state.

6 tween superconductivity and CDW shown in the equilibrium state.

7 ious processing conditions which suggests an equilibrium state.

8 dy-states of SRO that are different from any equilibrium state.

9 power evolves towards a Rayleigh-Jeans (RJ) equilibrium state.

10 ectroscopy and calculated by FactSage at the equilibrium state.

11 nd on the difference between its current and equilibrium state.

12 of a phase-separating system relaxing to its equilibrium state.

13 everal conformations coexisting in a dynamic equilibrium state.

14 le photo-induced chiral spin liquid near the equilibrium state.

15 g the reaction from the initial state to the equilibrium state.

16 model membranes in vitro under thermodynamic equilibrium state.

17 ture at which this orthorhombic phase is the equilibrium state.

18 ures that the system returns to its initial, equilibrium state.

19 eracting the suppression of order in the non-equilibrium state.

20 is, the network will almost surely reach an equilibrium state.

21 enerations without ever approaching a stable equilibrium state.

22 he atmospheric oxygen level to a new, higher equilibrium state.

23 asis of prevalence and duration, assuming an equilibrium state.

24 ting rapid redistribution of densities to an equilibrium state.

25 n of 1.5 mM compared with that under thermal equilibrium state.

26 ers and the scattering profiles of the three equilibrium states.

27 rs and the possibility of stabilizing out-of-equilibrium states.

28 free DNA circuits from equilibrium to out-of-equilibrium states.

29 transport as well as on LeuT conformational equilibrium states.

30 joining two subsystems prepared in different equilibrium states.

31 ting efficient transitions between different equilibrium states.

32 teria based on transformation half-lives and equilibrium states.

33 beta diversity change through transient and equilibrium states.

34 titioning driven by changes in thermodynamic equilibrium states.

35 sired Nash equilibria and preclude undesired equilibrium states.

36 h temperature, and for detecting non-thermal equilibrium states.

37 re transitions between biologically relevant equilibrium states.

38 ses transforms them into highly-excited non- equilibrium states.

39 ms into dissipative, and non-dissipative non-equilibrium states.

40 igh energy nutrition represent preserved non-equilibrium states.

41 and preserve highly ordered, high energy non-equilibrium states.

42 in giving a thorough explanation to particle equilibrium states.

43 may have led to dynamically stable far from equilibrium states.

44 ich phase structure in their low-temperature equilibrium states(1).

45 se competition and fluctuations found in the equilibrium state(14-20).

46 We find that the non-equilibrium state, 2 ps after the excitation, exhibits s

47 olymer surface has two reversibly switchable equilibrium states, a cationic N,N-dimethyl-2-morpholino

48 that the one-site assessment process has two equilibrium states: a disinterested equilibrium (DE) in

49 rowth and interaction parameters could alter equilibrium state accessibility and account for variabil

50 ified key microbial parameters that governed equilibrium state accessibility, such as the importance

51 tates, which are either able to approach the equilibrium state after deviation from metastability or

52 We quench the system to a far-from-equilibrium state and find delayed condensation close to

53 ying molecules and particles away from their equilibrium state and in cases with limited samples.

54 e feasibility of our method, we induce a non-equilibrium state and show that the phase-space distribu

55 Both the equilibrium state and the dynamics of the approach to eq

56 We consider perturbations of the Maxwellian equilibrium states and include the physical cross-sectio

57 ch distributions by using an analysis of the equilibrium states and their stability.

58 operating at high power often have multiple equilibrium states, and this produces complications with

59 Key signatures of the out-of-equilibrium state are current-voltage characteristics th

60 The pathway and rate to reach the equilibrium state are irrelevant, and the resulting asse

61 to study phase transition between different equilibrium states as a function of external magnetic fi

62 ity and time-reversal (PT) symmetries of the equilibrium state, as manifested in the emergence of tra

63 of a number of haemoglobin molecules in the equilibrium states, as well as intermediate forms of the

64 c basis for the macroscopic evolution to the equilibrium state at a well-defined and universal size.

65 lass-forming liquids that allow us to access equilibrium states at sufficiently low temperatures to d

66 that inserted dimers represent the dominant equilibrium state augmented by two metastable states ass

67 ydroxide species and the iron stimulated the equilibrium state between Co(3+) and Co(4+) .

68 he thermodynamics of bioaccumulation and the equilibrium state between the ecosystem compartments.

69 To understand how different equilibrium states between Fyn and the corresponding pho

70 rocessing, may not reach their thermodynamic equilibrium state but, instead, remain trapped in a loca

71 By electrostatic gating, the equilibrium state can be continuously tuned into an exci

72 cape, we genetically engineered a long-lived equilibrium state characterized by an extended life span

73 exceptional volatility before a more stable equilibrium-state community emerged that displayed hallm

74 The transition to this new equilibrium-state community with a broader spectrum of c

75 ol and assess progress towards their dynamic equilibrium state, continuously adapting to environmenta

76 The stability of equilibrium states corresponding to complete tumor eradi

77 e attitude of the actin protofilament at the equilibrium states coupled with the elevations of the li

78 greater the deviation of the plasma from its equilibrium state, coupled with faster propagation veloc

79 the insensitivity to mutation of a network's equilibrium state, depends on the complexity of the netw

80 ort the crystal structure of this exotic non-equilibrium state, determined by femtosecond X-ray diffr

81 This lipid-denatured equilibrium state (DL) is clearly more extensively unfol

82 (4) holds when the population approaches an equilibrium state, e.g. for time values greater than a t

83 lyzed folding mechanism by examining the key equilibrium states, e.g. native and refolded pepsin, bot

84 en its dynamic onset and the theorized final equilibrium state, enabling the direct study of the merg

85 mers which are intrinsically straight in the equilibrium state exhibit the mesoscopic bending anisotr

86 We propose that an equilibrium state exists between Gadd34/PP1c and the opp

87 tide nanosystems in both equilibrium and non-equilibrium states, featuring the formation of supramole

88 ed contact domains are inconsistent with the equilibrium state for an ordinary condensed polymer.

89 an additional elongation of 0.14 nm from the equilibrium state for dissociation.

90 states, with a focus on non-dissipative non-equilibrium states found in one-dimensional supramolecul

91 lution, depending on the correlation between equilibrium state frequencies.

92 n agonist alone is insufficient to shift the equilibrium state from the inactive to the active states

93 ergetic plasmonic hot carriers in nonthermal equilibrium states have pushed the limits of energy conv

94 which may prevent the system relaxing to its equilibrium state, have long been thought to play a key

95 passivity-the inability to extract work from equilibrium states-implies the thermal state's form, too

96 r solar forcings, we find both cold and warm equilibrium states, implying that the climate transition

97 Usually, its equilibrium state in a bulk helimagnet occurs only over

98 tion-desorption steps leading to the dynamic equilibrium state in a mixture of molecules with differe

99 ts reaching an out-of-equilibrium or reverse equilibrium state in aqueous medium.

100 silience of the desired (predator-dominated) equilibrium state in both stochastic and deterministic e

101 tuations around a stable low firing activity equilibrium state in the presence of latent "ghost" mult

102 e incubated with BCA and allowed to reach an equilibrium state in which the majority of the immobiliz

103 Computing equilibrium states in condensed-matter many-body systems

104 als properties is critical for understanding equilibrium states in electronic materials, as well as f

105 tions are important for determining chemical equilibrium states in energetic materials that contain a

106 be an essential feature of the study of non-equilibrium states in general, and non-ideal pathways in

107 at grain boundaries, at defect sites, or as equilibrium states in nominally acarbonaceous crystallin

108 through a process of continual disruption of equilibrium states in recursive reaction networks, drive

109 The model can aid prediction of equilibrium states in the context of further change: wid

110 are thus blocked by the absence of available equilibrium states in the singlet gap.

111 ng interactions enable a variety of pairwise equilibrium states, including the possibility of a local

112 This equilibrium state indicates that a Gly substitution can

113 Each equilibrium state is a direct measure of the bond streng

114 tropic cation localization-and find that the equilibrium state is bent B-DNA stabilized with a self-l

115 An equilibrium state is described, involving a PP-fold mono

116 lacustrine photosynthetic C fixation in this equilibrium state is quantitative and depends on the DSi

117 ining pump activity, and a Gibbs-Donnan-like equilibrium state is reached.

118 Predicting observables in equilibrium states is a central yet notoriously hard que

119 f crystal orientation from the thermodynamic equilibrium states is desired in layered hybrid perovski

120 pression patterns corresponding to different equilibrium states is of great benefit to the diagnosis

121 with the concentration of cardiolipin in the equilibrium state (lipid-dependent parameter).

122 lcano was probably poised in a near-eruptive equilibrium state long before the onset of the 2004-05 e

123 d value, nucleated nanobubbles grow to their equilibrium states, maintaining their nanoscopic size.

124 ave primarily focused on transitions between equilibrium states, many biologically and technologicall

125 Our work suggests that total SOC at an equilibrium state may be an intrinsic property of a give

126 igate how departure from the self-sustaining equilibrium state may be the mechanism responsible for t

127 those derived from experimental work for the equilibrium state metal and silicate reacting under high

128 of a surprisingly rich variety of driven non-equilibrium states (NES), whose formation is caused by a

129 The equilibrium state observed in our optical and NMR studie

130 Metaphase is thought to be a force-equilibrium state of "tug of war," in which poleward for

131 Furthermore, the equilibrium state of a (dA)16*(dT)16 sample in the prese

132 The method allows us to assess the equilibrium state of a large complex system by tracking

133 Quantum mechanics predicts that the equilibrium state of a resistive metal ring will contain

134 The first step is to stabilize a non-equilibrium state of a simple quantum system, such as a

135 al significance of this unique dimer-monomer equilibrium state of B7-1.

136 The equilibrium state of CCR5 is manipulated here toward eit

137 Mean signal attenuation at equilibrium state of contrast media distribution (10 min

138 The thermodynamic equilibrium state of crystalline materials is a single c

139 bonding network is far more tenuous and the equilibrium state of distal pocket is far more open and

140 NA experiments, we examined the unstretched, equilibrium state of DNA by using an anti-Brownian elect

141 The equilibrium state of each system was then determined ove

142 at CD4-induced conformational changes in the equilibrium state of gp120 lead both to movement of V1/V

143 aditionally described in terms of the static equilibrium state of Lotka-Volterra equations in which b

144 rt the observation of a distinct type of non-equilibrium state of matter, Floquet symmetry-protected

145 t allows self-consistent calculations of the equilibrium state of membrane-protein complexes after su

146 gn reliable models capable of predicting the equilibrium state of methane hydrates in saline water so

147 Characterizing and controlling the out-of-equilibrium state of nanostructured Mott insulators hold

148 r channel and therefore fail to describe the equilibrium state of Organic Electrochemical Transistors

149 game theory fundamental for elucidating the equilibrium state of strategic interactions, with applic

150 model results demonstrate that the geometric equilibrium state of the Achilles tendon can coincide wi

151 The equilibrium state of the bI5 intron RNA, prior to assemb

152 of the positions of the particles yields the equilibrium state of the membrane and allows determinati

153 usion model and a shift in the thermodynamic equilibrium state of the solutes toward the gel phase.

154 We also report direct measurement of the equilibrium state of the super-relaxed to disordered rel

155 st equal amounts of the two enantiomers, the equilibrium state of the system produces liquid-phase ch

156 We find that the overall equilibrium state of the system resulting from the mutua

157 ng law' provides a simple description of the equilibrium state of this choice allocation process: ani

158 s important for the maintenance of different equilibrium states of Fyn in situ.

159 ing expectation values of observables in the equilibrium states of local quantum Hamiltonians, both a

160 Creating non-equilibrium states of matter with highly unequal electro

161 s at these three sites resulted in different equilibrium states of NS1 between the tubular and non-tu

162 ." The cultural manifold represents a set of equilibrium states of social and cultural evolution: hyp

163 Analysis shows that kinetics and final equilibrium states of the closed system are highly const

164 This model predicts two equilibrium states of the cofilin-actin, or cofilactin,

165 lytical solutions of the model determine the equilibrium states of the entangled quantum networks and

166 ntermediates that are shown to be metastable equilibrium states of the polymer.

167 e components, suggesting that at least three equilibrium states of the protein exist.

168 ined maximum entropy principle governing the equilibrium states of the statistical theory.

169 rgy and information in leading to punctuated equilibrium states of vocal development.

170 by K-edge absorption spectroscopy, ns-lived equilibrium states of WDM Fe.

171 out by monitoring acid- and alcohol-induced equilibrium states of well-characterized model proteins,

172 hanically trapped in a higher-energy, out-of-equilibrium state on the beads and cannot be removed by

173 f key observables such as rate constants and equilibrium state populations to greater precision than

174 In general, at quasi equilibrium state, pulse protein-polyphenol particles an

175 h biomolecular assemblies exist in an out-of-equilibrium state, requiring continuous consumption of h

176 We show that an out-of-equilibrium state returns to equilibrium so quickly that

177 However, the new state is an out-of-equilibrium state since decarboxylation of the conjugate

178 ions are regularly perturbed away from their equilibrium state, so that acute outbreaks of phage infe

179 mics reflect a collection of local energetic equilibrium states specifically formed during substrate

180 ll effect drives the magnon gas into a quasi-equilibrium state that can be described by the Bose-Eins

181 ation biology is mostly based on the endemic equilibrium state that characterises infections before c

182 -the turbulent plasma transitions into a new equilibrium state that generates the observed soft-state

183 ysics, in which a physical system reaches an equilibrium state that is defined by a few global proper

184 Both processes afford an unfavorable equilibrium state that is subsequently drained toward th

185 ith each minimum corresponding to a possible equilibrium state that may be visited as the system resp

186 emarkable stability, and might correspond to equilibrium states that could hitherto be reached only b

187 orks in living systems, resulting in dynamic equilibrium states that differ for different diseases an

188 as gamma and beta rhythms represent rhythmic equilibrium states that facilitate sustained and efficie

189 ucleotides and nucleotide analogs, to induce equilibrium states that mimic intermediates in the actom

190 ape of yeast replicative aging with multiple equilibrium states that represent different types of ter

191 nd polymorphism may lead to the breakdown of equilibrium states that would otherwise maintain genetic

192 ently learn a classical approximation of non-equilibrium states that yields the gap-ratio distributio

193 ose uniformity in space and time defines the equilibrium state the system is in, this is not the case

194 Under a highly complex structure and non-equilibrium state, the upcoming generation of adaptive s

195 gle (mono-stable) or multiple (multi-stable) equilibrium states, though factors that contribute to st

196 mal annealing to evolve these manifestly non-equilibrium states through the assembly landscape, trave

197 The transition from one equilibrium state to another via rapid snap-through can

198 erstand how these reactions evolve toward an equilibrium state to understand the very long-term behav

199 t these instabilities determine the marginal equilibrium states towards which the magnetodisk plasma

200 t a self-organizing biological system at its equilibrium state tries to minimize its free energy eith

201 um initial conditions that relax to the same equilibrium state, underlies dominant models of how solv

202 Through a systematic study of equilibrium states, using a full three-dimensional micro

203 After the equilibrium state was reached, as determined by agreemen

204 of interesterification to reach the highest equilibrium state were 6% (w/v) of initial substrates, 1

205 ich different transacylations approached the equilibrium state were very similar (enzyme-dependent pa

206 governed when the monolayer is in mechanical equilibrium states when cell motility diminishes.

207 Using Cr(eta-C(6)H(6))(2), an equilibrium state where S and P are present is establish

208 n traditionally focused on the thermodynamic equilibrium state, where one-dimensional assemblies resi

209 age network properties appear to approach an equilibrium state, whereas individual properties are uns

210 ns between nanoceria and PCET reagents reach equilibrium states with good mass balance.

211 appearance of these structures in a thermal equilibrium state (with the same average energy) would b

212 mations are sufficiently rapid to achieve an equilibrium state within 1 week, regardless of the initi

213 To differentiate this state from an equilibrium state without flux, we propose a microscopic