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1 nds of circumferential rotation around their long axes.
2 ve a 3-fold rotational symmetry around their long axes.
3 dye di-8-ANEPPS, and stimulated along their long axes.
4 urface with a 60 degrees angle between their long axes.
5 ed in situ and after realignment along their long axes.
7 h induces a global realignment of interphase long axes along the direction of extension, this is suff
8 e. rotate about 115 degrees around their own long axes) and the mean relative axial displacement from
9 n coincident to the nanostructure and noodle long axes, and the resulting nanostructures show evidenc
12 differences in conjugation both along their long axes (by the number of fused benzene or thiophene r
15 aldehyde molecules rotate freely about their long axes even at cryogenic temperatures, allowing obser
16 he peptide molecules are oriented with their long axes normal to the bilayer (the "picket fence" orie
17 r, consistently match the orientation of the long axes of aligned and tightly packed polysaccharide f
19 illation over very short distances along the long axes of minicells, supporting the importance of geo
21 chromophore's long axis is aligned with the long axes of the adjacent base pairs, maximizing intermo
26 mpared to propagation at right angles to the long axes of the fibers, propagation along the long axis
29 or Cy5 attached by 3-atom tethers, with the long axes of the fluorophore and the terminal basepair a
31 helial cleavage plane angles relative to the long axes of the major retinal vessels during anaphase w
32 entated along the c axis and parallel to the long axes of the microribbons was observed in vitro.
33 ack in similar triclinic unit cells with the long axes of the molecules nearly perpendicular to the s
34 nsert loop are masked by rhoGDI and that the long axes of the two proteins are in parallel in the het
35 to lipid in an antiparallel manner, with the long axes of their helical repeats running perpendicular
36 rimers are predominantly arranged with their long axes oriented radially, and the width of the high m
37 her of two distinct orientations, with their long axes parallel or perpendicular to the direction of
39 that are thermodynamically stable with their long axes parallel to both the preferred hydrogen-bondin
41 ile, beads predominantly migrated with their long axes parallel to the direction of motion, mimicking
42 fic manner, specifically in cells with their long axes perpendicular to the stretching direction, but
43 cTnI-cTnT(198-298) component lie with their long axes roughly parallel to one another with a relativ
44 gen-bonding substituents along the molecular long axes tunes properties such as hyperpolarizability,