ライフサイエンスコーパス: equilibrium state

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

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

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

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

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

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

7 enerations without ever approaching a stable equilibrium state.

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

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

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

11 ting rapid redistribution of densities to an equilibrium state.

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

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

14 model membranes in vitro under thermodynamic equilibrium state.

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

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

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

18 igh energy nutrition represent preserved non-equilibrium states.

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

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

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

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

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

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

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

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

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

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

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

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

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

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

33 The stability of equilibrium states corresponding to complete tumor eradi

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

56 This equilibrium state indicates that a Gly substitution can

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

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

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

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

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

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

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

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

65 The equilibrium state observed in our optical and NMR studie

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

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

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

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

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

71 The equilibrium state of CCR5 is manipulated here toward eit

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

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

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

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

76 The equilibrium state of each system was then determined ove

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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