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To examine this correlation, a histogram of SNR for minimally observed spheres and for non-observed spheres is present, one for each system in Fig. 2.
Stoffyn-Egli and Buckley (1992) also observed spheres on the outer surface of rusticles that resembled bacteria associated with γ-FeOOH.
Fig. 2 Histograms of the SNR of the positively observed spheres in red and positively non-observed spheres in blue.
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The observation scores recorded by the three human observers were aggregated to generate a detectability score of "sphere observed," "sphere not observed," or "sphere neither observed nor not observed".
We observed sphere-like particles and porous structure of α-NiS with an approximate average size of 0.1 0.2 μm on the surface of the α-NiS film at the annealing temperature 400 °C in Fig. 2c.
After 2 weeks in culture (cell passage 1), in N2 medium we observed sphere formation combined with monolayer of polyhedral- and spindle-shaped cells, arrowheads).
We observed sphere-forming capacity and clonogenicity in all the 10 analysed samples in SF media, as previously reported (Piccirillo et al, 2009b; Fael Al-Mayhani et al, 2009).
When grad student Rob Deegan videotaped a solution of tiny spheres in distilled water, they observed the spheres travel and accumulate into a ring, just as predicted.
A cutoff at 0.45 μm was observed for spheres, corroborating the diameter of spheres as ≤0.45 μm.
Evidence of proliferation was observed as spheres could be passaged and new spheres were observed to form.
The difference is attributed to the fact that the speed up observed for spheres is dictated by size exclusion of the particles at the boundary, while rods slow down due to increasing alignment at the boundary.
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