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1 outward from histone octamers along the DNA helix axis.
2 p, the conserved crevice faces away from the helix axis.
3 an anisotropic, directional bend in the DNA helix axis.
4 atic potential gradient perpendicular to the helix axis.
5 about 35 degrees and displaced 3 A from the helix axis.
6 an exposed continuous strip parallel to the helix axis.
7 ely free of any assumptions about an overall helix axis.
8 ibiting the largest, and consequently a bent helix axis.
9 e minor groove with its face parallel to the helix axis.
10 pairs, narrowed minor groove, and a straight helix axis.
11 ix and contains a channel that runs down the helix axis.
12 and a translation of 8.6 angstroms along the helix axis.
13 n angles differing by 180 degrees around the helix axis.
14 om the plane perpendicular to the fiber (DNA helix) axis.
17 e duplexes are translated by 3.4 A along the helix axis and rotated by 10.8 degrees relative to each
18 Tyr 15 and Tyr 39 project along the subunit helix axis, and one phenoxyl engages in hydrogen-bonding
21 Mg(2+) leads to a significant bending of the helix axis at the base of the Specifier Loop domain, but
28 s approach allows simultaneous estimation of helix axis deflection magnitude and direction when a tes
32 s presented that quantifies and projects the helix axis evolution over time, with the choice of unifo
33 ees and the rotational pitch angle about the helix axis for residue Ala29 omegaAla29=-59.8(+/-9.9) de
35 s nearly equatorially from the subunit alpha-helix axis, in contrast to the more axial orientations f
37 d phospholipid bilayer samples show that the helix axis is parallel to the plane of the bilayers.
38 acing between the nucleotide pairs along the helix axis is shorter, suggesting a mixed B/A structure.
39 with DNA lead to substantial bending of the helix axis may facilitate such distortions through solva
41 strategic positions about the putative alpha-helix axis of the extracellular juxtamembrane region.
43 idealized A-form helices (iH1 and iH2) with helix axis oriented along the molecular Z-direction runn
45 he interaction surfaces are smoother and the helix axis separations are closer in the amino-terminal
46 ively charged bacterial phospholipids with a helix axis that is aligned flat on a lipid bilayer surfa
47 helicoid and remaining perpendicular to the helix axis; the structure is called a chiral nematic.
48 r populations assume an orientation with the helix axis tilted by approximately 23 degrees with respe
49 es are flipped out and away from the octamer helix axis to form base-pairing interactions with a seco
50 ckbone carbonyl groups tilting away from the helix axis toward the ions located in the central lumen.
52 ementary strands are displaced away from the helix axis toward the minor groove of the heteroduplex,
56 l base pairs are all displaced away from the helix axis, yielding significant changes in local backbo
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