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The RF voltage is applied to all trap segments with opposite phases on adjacent rods and is mixed with typically 5 V DC voltage on the endcap segments.
Close examination of adjacent rods (Fig. 3) reveals that the rods are aligned to one another, i.e., no relative rotations observed around the growth axis, which suggests that the rods have epitaxial relations with the substrate.
This is most clearly seen in Figure 2c, where only some small spots in the sample (see arrows in the figure) are not coated by Ag due to shadowing from adjacent rods), and also in Figure 2g where Ag can be seen forming a quasi-conformal coating all over the surface of a ZnO rod.
φ m is the maximum bias angle of adjacent rods.
If adjacent rods packed at an angle, then the resulting fiber would be a super helix of CMPs where fiber thickness matches the length of a peptide.
In order to minimize signal cross-talk of adjacent rods and cones, the excitation power was lowered to ~5 mW (compared to the 10 mW used for the experiments shown in Fig. 3).
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In addition, all axial distances between any adjacent rod lenses are the same, i.e., only one type of spacer is needed for the assembly of the relay system.
Analysis of the parallel interactions between adjacent myosin rods revealed a staggering of 14.3 nm and 43 nm, corresponding roughly to the 98aa and 295aa (3×98aa+skip residue).
Adjacent myosin rods are connected via M-bridges, forming a regular hexagonal lattice [ 4].
Similarly, H2 formed a triple-helix with a Tm of 50 °C and was shown by TEM to form plates similar to H4. Increasing the hydrophobicity of a collagen sequence by adding an additional hydrophobic triplet (ppphhhpppp) was also predicted in DLA simulations to produce disclike structures with variable thickness due to staggered interactions between adjacent monomer rods.
The feeding apparatus consisted of a feeding pocket and one adjacent feeding rod comprised of 20 microtubules organized in four rows 4-6-6-4 4-6-6-4 4-6-6-4 4-6-6-4
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