ライフサイエンスコーパス: reference state

1 al based on distance-scaled finite ideal-gas reference state).

2 itely dilute solution in n-hexadecane as the reference state.

3 eractions extracted from these decoys as the reference state.

4 5 cal/mol K (-TDeltaS= +9.7kcal/mol) at a 1M reference state.

5 lly explicit model to represent the unfolded reference state.

6 nol composition, and a helium vapor phase as reference state.

7 of favorable free energy of binding at a 1M reference state.

8 fact that proteins do not unfold to a simple reference state.

9 es can be misleading due to ambiguity of the reference state.

10 pproximations, including a definition of the reference state.

11 ic-network model representation near the two reference states.

12 the crystallized forms were subtracted using referenced states.

13 1) the measurement equation for genes in the reference state; (2) the measurement equation for genes

14 ese structural parameters was derived from a reference state, a covalent enzyme-substrate adduct wher

15 Therefore it cannot be assumed that reference state activities are negligible, nor that they

16 s, i.e., the difficulty to design a suitable reference state against which the working enzyme can be

17 Using the new reference state allows quantitative comparison among var

18 ximately 1.5kcal/mol relative to that of the reference state, an A-form RNA but with cytosine (C7) lo

19 The definition of an appropriate reference state and the introduction of a correction ter

20 The shift in the reference state, and the resulting increase in folding c

21 rtiary contact interactions relative to this reference state are consistent with a hinge-bending moti

22 ed enthalpy differences between well-defined reference states can be independently and consistently a

23 interaction potentials called Decoys as the Reference State (DARS) and incorporated DARS into the do

24 Decoys As the Reference State (DARS) is a simple and natural approach

25 ent structures of the apo-CzrA and CzrA*CzrO reference states (DeltaH(c)(t) = 9.4 kcal mol(-1)) in a

26 Using a reference state developed from exhaustive sequences, we

27 Our estimates provide a new reference state for future climate studies with rigorous

28 ing point for protein folding as well as the reference state for protein stability studies and can be

29 e starting state for protein folding and the reference state for protein stability studies.

30 e native disulfide-intact protein provided a reference state for the extent of expansion of intramole

31 thetized state of the leech was taken as the reference state for the model in which the active and pa

32 They also provide a reference state for the protein in structure-based model

33 With reference states for the five mutant classes as a guide,

34 Therefore, the starting point, or reference state, for the transition to the native, funct

35 nergy, in which the total free energy of the reference state (i.e., gas phase) is the CHARMm potentia

36 esolvation mechanism is based on an improper reference state; (ii) a nonpolar active site cannot acco

37 States; we also show the robustness of these Reference States in adjusting to changes in environmenta

38 e information on top of collective dynamical reference states in complex networks.

39 e-substituted GB1 variants typically used as reference states in double mutant-cycle analyses.

40 For cooperative ligand binding, the reference state is a hyperbolic curve for a monomer with

41 The DFIRE distance-scaled finite ideal gas reference state is employed for the distance-dependent c

42 imized atomic potentials (SOAP) in which the reference state is replaced with data-driven 'recovery'

43 Using the reference state of exhaustive permutation of residues wi

44 stical energy functions is that the physical reference state of ideal gas used in the DFIRE-based ene

45 the GABAAreceptor, we needed to establish a reference state of the receptor to compare reaction rate

46 Based on a structural reference state of two protofilaments aligned to create

47 If a position-independent material reference state such as a full sphere is used in definin

48 ring function to a better description of the reference state-that is, the state of no interactions.

49 n of this statistical potential, such as the reference state, the bin width, cutoff distances between

50 In the reference state, the mean intensities are modeled as a s

51 By comparison with a random coil reference state, the nascent structure in the QUA2 regio

52 self has several new features, including its reference state, the random crystal structure, which rem

53 We extend the theory of finite ideal gas reference state to icosahedral local coordinates.

54 ch uses flux and gene expression data from a reference state to predict metabolic responses in a gene

55 est that the group-14 atoms bind in the (3)P reference state to the transition metal in a combination

56 We find that the choice of the reference state used for the in-plane elastic energy is

57 esolve long-standing questions regarding the reference state used in RBC elasticity theory for determ

58 These energy functions differ in the reference states used for energy derivation.

59 which considers relative flux changes from a reference state, we hypothesize a relative metabolic flu

60 aired linear duplex or three-arm junction as reference states, we can establish a thermodynamic cycle

61 and by comparing them to multiple planktonic reference states, we identify patterns of gene expressio

62 set of physiologically sensible baseline or Reference States; we also show the robustness of these R

63 rature was used to generate the straightened reference state, with the required topological relaxatio