ライフサイエンスコーパス: twist angle

1 nked arylene diimide dimer with a 76 degrees twist angle.

2 t potential changes in bend angle as well as twist angle.

3 -systems and sterically regulated inter-aryl twist angles.

4 smaller but constant redshift for all other twist angles.

5 nd the receptor, but showed variation in D23 twist angles.

6 boratory frame as a function of the tilt and twist angles.

7 mise unique properties with their 90 degrees twist angles.

8 ive Poisson's ratios can be tuned by the pre-twisting angles.

9 G2*U16 and U7*G11/C8*G10, while the smallest twist angles (28.24 and 27.27 degrees ) are at G2*U16/G3

10 The largest twist angles (37.70 and 40.57 degrees ) are at steps G1*

11 rmations appear clearly separated by a large twist angle (~40 degrees ) and depend mainly on the comp

12 gles are better hydrated than steps with low twist angles, 6.9 H2O vs 0 H2O; negative roll angles are

13 hromophores reveals large ring-ring dihedral twist angles (80-89 degrees) and a highly charge-separat

14 as the enforcement of consecutive 90 degrees twist angles along the polyimide backbone.

15 The twist angle and base roll combine to significantly affec

16 This causes a decrease in the inter-ring twist angle and, together, these changes are responsible

17 formations and causes distortions in related twist angles and helical rises.

18 erogeneous interactions can we reproduce the twist angles and related properties.

19 tions also indicate that the actin propeller twist-angle and nucleotide cleft-angles are influenced b

20 degrees C</=T</=198 degrees C) and bicrystal twist angle, and insensitive to impurities from the atmo

21 chains, as evidenced by the decrease in the twist-angle, and consequent increase in the cholesteric

22 The presence of the bulge induces very large twist angles (approximately +50 degrees) between the bas

23 e pairs, 2.5 H2O vs 1.3 H2O; steps with high twist angles are better hydrated than steps with low twi

24 The twist angles are reversed (37 degrees and 26 degrees) in

25 significant changes in the opening, roll and twist angles as compared to the normal A:T base pair.

26 multilayer graphene by the introduction of a twist angle between different layers to create van Hove

27 rization and is only weakly dependent on the twist angle between layers.

28 nversion efficiency from 2.6% to 6.4% as the twist angle between the monomeric building blocks in the

29 (11+) was used to gauge the influence of the twist angle between the p-orbital at Si+ and the C-Si bo

30 re of the RNA is characterized by a very low twist angle between the two G.U base-pairs, providing a

31 ve singularities whose energy depends on the twist angle between the two layers.

32 ance is expected to change with the relative twist angle between the two rings, with the planar confo

33 The twist angle between the wobble pairs, 38.1 degrees, is a

34 Yet, ortho branching causes large twist angles between the core and the arms that are detr

35 ls form mobile bulges causing a variation of twist angles between the helix pairs.

36 the aromatic bridges gradually increases the twist angles between the two PDI planes, leading to a va

37 ray scattering, respectively, from which the twist-angle between DNA molecules can be calculated.

38 er than the imaginary part, with the highest twist angle chromophore giving |Re(gamma)/Im(gamma)| app

39 nce for the series decreases with increasing twist angle, consistent with a cosine-squared relation p

40 ent is attributed to the emergence of unique twist-angle-dependent van Hove singularities, which are

41 f two graphene monolayers with an interlayer twist angle, exhibits a strong light-matter interaction

42 junctures, only slightly relaxes the biaryl twist angle from 89.6 degrees to approximately 80 degree

43 om 46 degrees to 22 degrees ), inter-helical twist angle (from 66 degrees to -18 degrees ), and inter

44 HSs in bilayer graphene over a wide range of twist angles (from 5 degrees to 31 degrees ) with wide t

45 ir evolution are systematically studied with twist angle in bilayer and trilayer graphene sheets.

46 NOE NMR measurements of the twist angle in solution confirm that the solid-state twi

47 te the evolution of interlayer coupling with twist angles in as-grown molybdenum disulfide bilayers.

48 The twist angle increases with the increase of deformation a

49 c velocity crosses zero several times as the twist angle is reduced.

50 e TS structure of ribozyme reaction while no twisted angle is found in TS of the reaction in water.

51 he Raman G peak area initially increases for twist angles larger than a critical angle and decreases

52 olanes exist, and they all suffer from small twist angles (<35 degrees ).

53 Enabled by the twist angle measurements of the spontaneous twist, we de

54 erizable conformation is its reduced helical twist angle of 22 degrees.

55 II (G x U/U x G) structure stack with a low twist angle of 25.3 degrees in contrast to that of motif

56 5'-side of the first C6.A27(+) wobble has a twist angle of 27 degrees compared to the 3'-side U7.A28

57 adopts a twisted backbone with an end-to-end twist angle of 28 degrees that was unambiguously confirm

58 t the I.U/U.I mismatch steps, duplex 1 has a twist angle of 33.9 degrees, close to the average for al

59 rystal structure of 17 reveals that it has a twist angle of 45.2 degrees for the carbon-carbon double

60 roll angle of approximately 40 degrees and a twist angle of approximately 20 degrees, between positio

61 roll angle of approximately 40 degrees and a twist angle of approximately 20 degrees, between positio

62 roll angle of approximately 40 degrees and a twist angle of approximately 20 degrees, between positio

63 phenylimidazol-1-yl)purine nucleoside, and a twist angle of approximately 61 degrees was measured bet

64 ees with respect to the surface normal and a twist angle of the CCC plane relative to the tilt plane

65 These results show that maps of the twist angle of the LC constructed from families of optic

66 he stack of images into a spatial map of the twist angle of the LC on the analytic surface.

67 different ring substitutions that alter the twist angle of the molecules.

68 ith the ruffling deformation and the average twist angle of the pyrrole rings.

69 s, but duplexes 2 and 3 are underwound, with twist angles of 24.4 degrees and 26.5 degrees, respectiv

70 anophanes containing a malonyl tether, where twist angles of almost 80 degrees were reached.

71 G7 (roll angles of approximately 42 degrees, twist angles of approximately 16 degrees ), but is much

72 G7 (roll angles of approximately 20 degrees, twist angles of approximately 17 degrees).

73 Furthermore, the twist angles of the LC can be used to quantify the energ

74 etermining effects of nucleotide sequence on twist angle or rise at individual bp steps does not prov

75 lic rotation rate, P =0.05 and P =0.006; net twist angle, P=0.02) movement were significantly reduced

76 re including base stacking energy, propeller twist angle, protein deformability, bendability, and pos

77 esulting from correlated changes in bend and twist angles such that the p53-DNA tetrameric complex is

78 The filaments also exhibit random twist angles that are broadly distributed.

79 escribe DNA deformations (i.e., the bend and twist angles), the translational parameters describing t

80 To explain this behavior with twist angle, the energy separation of the van Hove singu

81 recover a similar equation for the internal twist angle to that of classical vortex tubes.

82 n state geometry requires adjustment for the twist angles to those of the relaxed ground state to pro