ライフサイエンスコーパス: internuclear

1 Abducens internuclear and ascending tract of Deiters (ATD) inputs

2 The abducens internuclear and ascending tract of Deiters (ATD) pathwa

3 and soma-dendritic distribution of abducens internuclear and ATD synaptic endings are correlated wit

4 synaptic membrane profile, both the abducens internuclear and ATD synaptic endings are labeled with g

5 as inferred from comparative analyses of the internuclear and intranuclear coherence between bipolar

6 interproton distance and the (13)C-(1)H-(1)H internuclear angle.

7 e alkylidene CHR fragment relative to the MC internuclear axis.

8 obules in chromatin and did not abrogate the internuclear bridges seen in the FA-G mutant cells.

9 ance of aneuploid cells and the formation of internuclear chromatin bridges, indicating that nuclear

10 GP was no longer apparent, despite increased internuclear coherence.

11 duced dosage of the gene product, failure of internuclear communication, and failure of transvection

12 The internuclear connectivity indicated by the NMR data sugg

13 ng NMR experiment that generates (15)N-(15)N internuclear contacts in protein systems using an optimi

14 The measured H-C internuclear correlation times indicated differences in

15 gs that are necessary for the observation of internuclear correlations in 2-D experiments.

16 electron correlation, the onset of electron-internuclear coupling, and quasi-particle formation.

17 EDOR) pulse sequence was used to measure the internuclear dipolar coupling, and the results demonstra

18 In isotropic solution, internuclear dipolar couplings average to zero as a resu

19 train, the magnitude and orientation of the internuclear dipole vector, within the chemical shift an

20 field, Brownian diffusion no longer averages internuclear dipole-dipole interactions to zero.

21 the MCH plane and is perpendicular to the MC internuclear direction.

22 etermined using 3940 (1970 per VEGF monomer) internuclear distance and 476 (238 per VEGF monomer) dih

23 The structure is based on a total of 887 internuclear distance and dihedral restraints derived fr

24 active site loses its ability to restore the internuclear distance between substrate and Fe(IV)=O tha

25 -resonance (REDOR) NMR was used to probe the internuclear distance between the (19)F and the (31)P-la

26 Finally, the internuclear distance between the amino nitrogens and th

27 proportionally to the difference in a single internuclear distance between the ground and transition

28 The DRAWS technique was used to measure the internuclear distance between two 13C labels at the carb

29 The internuclear distance changes only slightly from the lig

30 A (13)C-(13)C internuclear distance measurement from (13)CO(i) to (13)

31 (17)O HETCOR NMR spectra as well as accurate internuclear distance measurements at natural abundance.

32 Internuclear distance measurements on PLB using rotation

33 fied conformation (the AC conformer) with an internuclear distance of 4.4 A.

34 duced by molecular dynamics simulations with internuclear distance restraints determined by NMR.

35 uality allowed the correct identification of internuclear distance restraints encoded in 3D spectra w

36 gnetic tags, without the use of conventional internuclear distance restraints.

37 Profiles of cumulative energy versus internuclear distance show large fluctuations and provid

38 llows the NN bond polarization energy and NN internuclear distance to be correlated in three states o

39 e the dependence of the wave function on the internuclear distance.

40 ate the average electron position beyond the internuclear distance.

41 We observed similar internuclear distances (4.5 +/- 0.2 A) in both Neu and N

42 turn, is employed in experiments to estimate internuclear distances and molecular torsion angles.

43 mics simulated-annealing scheme in which the internuclear distances and van der Waals repulsive terms

44 The internuclear distances are extracted by using a simple a

45 onal resonance NMR methods, we show that the internuclear distances between [1-(13)C]Leu7 and [3-(13)

46 loit nuclear Overhauser effects to determine internuclear distances between pairs of protons, without

47 The internuclear distances between the HFP 13CO groups and t

48 d explains the difference in the equilibrium internuclear distances for the two spin states.

49 ed to characterize the binding by estimating internuclear distances from (19)F of oritavancin to (13)

50 Internuclear distances from (19)F of the DFPBV to the (1

51 High-precision determinations of internuclear distances from NMR recoupling techniques, r

52 ional-echo double resonance NMR by measuring internuclear distances from the (19)F of FBV to (13)C an

53 l-echo double resonance (REDOR) NMR provided internuclear distances from the 19F of this glycopeptide

54 viations from calculated curves based on the internuclear distances from X-ray crystallography.

55 L-Leu-L-Phe we have determined a total of 16 internuclear distances in the 2.5-6 A range.

56 ble-resonance NMR has been used to determine internuclear distances in the complex of glutamine-bindi

57 cell-wall complexes that are consistent with internuclear distances obtained from (13)C{(19)F} and (1

58 ical shift resolution required for measuring internuclear distances to (13)C in the retinal chain (C8

59 ne bilayers by determining multiple critical internuclear distances using nuclear Overhauser enhancem

60 Internuclear distances were calculated from the initial

61 and ring-current rules, Si bonds at greater internuclear distances, a feature that allows easier des

62 ve a high degree of precision with regard to internuclear distances, geometries, and charges within t

63 o consistent with six other REDOR-determined internuclear distances, most of which agree with values

64 ng linear correlations with boron-phosphorus internuclear distances.

65 (REDOR) to determine intra- and interligand internuclear distances.

66 physiologic signals conveyed by the abducens internuclear (eye velocity and eye position) and ATD (he

67 dividual nRt neurons to the strength of this internuclear inhibition, we obtained whole-cell recordin

68 these latter measurements also resolve weak internuclear interactions that suggest the formation of

69 a direct bilateral projection of hypoglossal internuclear interneurons onto facial motoneurons.

70 Hypoglossal internuclear interneurons projecting to the facial nucle

71 Abducens internuclear neurons are responsible for conjugate gaze

72 were VEGF immunopositive, and that abducens internuclear neurons expressed the VEGF receptor Flk1.

73 Abducens internuclear neurons of host animals showed a complete r

74 stics and synaptology of axotomized abducens internuclear neurons, which mediate gaze conjugacy for h

75 ns receive two main pontine inputs: abducens internuclear neurons, whose axons course through the med

76 divided into broad categories: supranuclear, internuclear, nuclear, and gaze-holding systems.

77 Patients with internuclear ophthalmoplegia (INO) may have preserved ve

78 ), autoimmune retinopathy (n = 1), bilateral internuclear ophthalmoplegia (n = 1), and headache (n =

79 motor deficits in multiple sclerosis include internuclear ophthalmoplegia and nystagmus, resulting in

80 FINDINGS: Studies have supported the use of internuclear ophthalmoplegia, a model to study effects o

81 Internuclear ophthalmoplegia, a new finding, was present

82 ognised syndromes such as optic neuritis and internuclear ophthalmoplegia, respectively.

83 n comparison to those evoked by the abducens internuclear pathway as determined electrophysiologicall

84 genic compensatory mechanism of the abducens internuclear pathway that could lead to the observed fir

85 The abducens internuclear pathway through the medial longitudinal fas

86 orseradish peroxidase labeling, the abducens internuclear projection is predominantly, if not exclusi

87 ser effects (trnOe) experiments to determine internuclear proton distances.

88 sition rate depends strongly on both the N-O internuclear separation and the molecular orientation an

89 During mitosis, the rate of change of internuclear separation in Deltakif12 cells is reduced c

90 ated by one or two covalent bonds, where the internuclear separation is known and the measured dipola

91 d that autoionization cannot occur until the internuclear separation of the fragments is greater than

92 upling across hydrogen bonds: (1) the H...O' internuclear separation r(HO)('), (2) the H...O'=C' angl

93 lso contain binuclear complexes with a 4.4 A internuclear separation.

94 rajectories of chemical reactions (change of internuclear separations with time) on the femtosecond t

95 The majority of abducens internuclear synaptic endings contact distal dendrites,

96 Abducens internuclear synaptic endings furthermore have a higher

97 atory neurotransmitters utilized by abducens internuclear synaptic endings whose burst-tonic physiolo

98 way (~20 degrees ) from the boron-phosphorus internuclear vector, leading to an improved understandin

99 direct information on the orientation of the internuclear vector.

100 n times of tumbling motion of the (13)C-(1)H internuclear vectors in the glucose-treated sample are l

101 each constraint restricts the orientation of internuclear vectors with respect to the laboratory fram