戻る
「早戻しボタン」を押すと検索画面に戻ります。 [閉じる]

コーパス検索結果 (１語後でソート)

通し番号をクリックするとPubMedの該当ページを表示します
1 al based on distance-scaled finite ideal-gas reference state).
2 es can be misleading due to ambiguity of the reference state.
3 pproximations, including a definition of the reference state.
4 itely dilute solution in n-hexadecane as the reference state.
5 eractions extracted from these decoys as the reference state.
6 5 cal/mol K (-TDeltaS= +9.7kcal/mol) at a 1M reference state.
7 lly explicit model to represent the unfolded reference state.
8 nol composition, and a helium vapor phase as reference state.
9  of favorable free energy of binding at a 1M reference state.
10 fact that proteins do not unfold to a simple reference state.
11 ultrasonic signal perturbation compared to a reference state.
12 limiting C-C bond-forming step compared to a reference state.
13 interaction landscapes with young cells as a reference state.
14 uivalent and hence able to serve as a common reference state.
15 e stable as anions from their atom and dimer reference states.
16 ic-network model representation near the two reference states.
17 e potential to break ecology's dependence on reference states.
18 the crystallized forms were subtracted using referenced states.
19 1) the measurement equation for genes in the reference state; (2) the measurement equation for genes
20 ,(1)(,)(2)(,)(3) instead commonly relying on reference states.(4)(,)(5) A recently published ecologic
21 ese structural parameters was derived from a reference state, a covalent enzyme-substrate adduct wher
22          Therefore it cannot be assumed that reference state activities are negligible, nor that they
23 s, i.e., the difficulty to design a suitable reference state against which the working enzyme can be
24                                Using the new reference state allows quantitative comparison among var
25 ximately 1.5kcal/mol relative to that of the reference state, an A-form RNA but with cytosine (C7) lo
26 on trophic status being oligotrophic under a reference state and mesotrophic under current conditions
27             The definition of an appropriate reference state and the introduction of a correction ter
28                             The shift in the reference state, and the resulting increase in folding c
29 rtiary contact interactions relative to this reference state are consistent with a hinge-bending moti
30                                              Reference states are useful as models for facilitating c
31           The user is encouraged to choose a reference state based on the appropriateness of the mode
32 ed enthalpy differences between well-defined reference states can be independently and consistently a
33  interaction potentials called Decoys as the Reference State (DARS) and incorporated DARS into the do
34                                Decoys As the Reference State (DARS) is a simple and natural approach
35 ent structures of the apo-CzrA and CzrA*CzrO reference states (DeltaH(c)(t) = 9.4 kcal mol(-1)) in a
36                                      Using a reference state developed from exhaustive sequences, we
37 ns, originates in the assumption of a flawed reference state for energy decomposition analyses.
38                  Our estimates provide a new reference state for future climate studies with rigorous
39                            We also propose a reference state for nonflat surfaces.
40 ing point for protein folding as well as the reference state for protein stability studies and can be
41 e starting state for protein folding and the reference state for protein stability studies.
42 e native disulfide-intact protein provided a reference state for the extent of expansion of intramole
43 thetized state of the leech was taken as the reference state for the model in which the active and pa
44                          They also provide a reference state for the protein in structure-based model
45 , standard state conventions and appropriate reference states for adsorbed species have received less
46            Here, we compare seven choices of reference states for calculations of equilibrium constan
47                                         With reference states for the five mutant classes as a guide,
48            Therefore, the starting point, or reference state, for the transition to the native, funct
49 nergy, in which the total free energy of the reference state (i.e., gas phase) is the CHARMm potentia
50 esolvation mechanism is based on an improper reference state; (ii) a nonpolar active site cannot acco
51 lity of structural elements to move beyond a reference state in two opposite directions, is common in
52 States; we also show the robustness of these Reference States in adjusting to changes in environmenta
53 e information on top of collective dynamical reference states in complex networks.
54 e-substituted GB1 variants typically used as reference states in double mutant-cycle analyses.
55          For cooperative ligand binding, the reference state is a hyperbolic curve for a monomer with
56   The DFIRE distance-scaled finite ideal gas reference state is employed for the distance-dependent c
57 imized atomic potentials (SOAP) in which the reference state is replaced with data-driven 'recovery'
58                                    Using the reference state of exhaustive permutation of residues wi
59 stical energy functions is that the physical reference state of ideal gas used in the DFIRE-based ene
60  the GABAAreceptor, we needed to establish a reference state of the receptor to compare reaction rate
61                        Based on a structural reference state of two protofilaments aligned to create
62     Our goal is to provide the reader a well-referenced state-of-the-art understanding of current kno
63           If a position-independent material reference state such as a full sphere is used in definin
64 ring function to a better description of the reference state-that is, the state of no interactions.
65 n of this statistical potential, such as the reference state, the bin width, cutoff distances between
66                                       In the reference state, the mean intensities are modeled as a s
67             By comparison with a random coil reference state, the nascent structure in the QUA2 regio
68 self has several new features, including its reference state, the random crystal structure, which rem
69     We extend the theory of finite ideal gas reference state to icosahedral local coordinates.
70 ch uses flux and gene expression data from a reference state to predict metabolic responses in a gene
71 est that the group-14 atoms bind in the (3)P reference state to the transition metal in a combination
72               We find that the choice of the reference state used for the in-plane elastic energy is
73 esolve long-standing questions regarding the reference state used in RBC elasticity theory for determ
74         These energy functions differ in the reference states used for energy derivation.
75              The magnitude of departure from reference state varied considerably within the sample; h
76 ) design, state observer design, and desired reference state vector design (whole system performance)
77 tput feedback control and to provide desired reference state vector.
78 which considers relative flux changes from a reference state, we hypothesize a relative metabolic flu
79 aired linear duplex or three-arm junction as reference states, we can establish a thermodynamic cycle
80 and by comparing them to multiple planktonic reference states, we identify patterns of gene expressio
81  set of physiologically sensible baseline or Reference States; we also show the robustness of these R
82 rature was used to generate the straightened reference state, with the required topological relaxatio