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While electron density is weaker in this region of the Sir3 BAH-NCP structure, it appears that multiple arginines (R28, R29, R30, R32, and R34) line the acidic patch groove to make charged interactions with the NCP surface.
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First, we consider the plasma density is weak.
Therefore, the effect of these variables on Density is weak and can be neglected.
Although the dynamic mechanism can affect the ionospheric electron density, it mainly transports the ion and electron, and its influence on the total electron density is weak.
This shows that the coupling impedance in the lower plasma density is weak and growth rate remains constant in this limit.
Because the electron density is weak and the coordination distance of >2.8 Å is longer than would be expected for Na+, we interpret this density as a water molecule.
Third, the variability in the exponent β suggests that the negative dependence of reproductive investment on parasite density is weak or may be confounded by other factors such as immune responses.
The study of the influence of different kinetic parameters temparature, surface roughness, etc) on the methanol electrooxidation showed, in particular, that the current densities are weaker for electrodes having a large active surface.
We expect that the sheet current densities are weak or absent where there are no currents (e.g. in non-polar regions) and not wildly fluctuating.
Electron density is present at S1 in an ion omit map, compatible with the presence of an ion, although the density at S1 is weaker relative to the ion densities at S2 S4, as if the occupancy at S1 is reduced.
Note that the density of electrons is weaker at the center of the "boron ring .b Quasi-planarCsstructure of B12H8, which is the energetically preferred configuration for B12with 4 H2molecules, attached to it.c A contour plot of NICS x,y) for B12H6in plane (left) and at 1 Å above the planar molecule (right).
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