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For the other samples, we observe a steady increase of α with the temperature.
In these samples we observe a systematic reduction of heats of reaction, maximum reaction temperatures, and reaction propagation velocities as the volume fraction of reactive material is reduced.
For mono-layer samples, we observe a transition from 2D Mott VRH to Efros-Shklovskii VRH with increasing the fluorine content.
For all the samples we observe electron dense regions close to the cell membrane (Figure 3A and 3B) and in the cytoplasm (Figure 3C and 3D).
However, in our samples, we observe within the domes on the planar sample (94% of all islands, height: 20.1 ± 0.1 nm) a similar size distribution as for the domes on the patterned samples.
While there is some variation in the distribution of pores/vesicles in the samples, we observe that the microcrack density exerts an important control on the porosity and density, as illustrated by the correlation between crack area per unit volume and connected porosity presented as Figure 8B.
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As shown in Fig. 1c, the brightest BQDs in the two samples we observed are quite different in PL spectrum.
In both groups of samples we observed significant influence of liquid metal on the tensile properties, in particular reduction of total elongation.
In studied samples we observed the increase of the clusters sizes, changes in the mean lattice parameters a0, c0, and decay of disorder with increasing annealing temperature.
In non-tg samples we observed apparent axonal mGluR5 immunolabeling through the cortical layers presumably on pyramidal cell axons.
In LPS and CpG-stimulated adult samples, we observed a further increase in HLA DR expression at the surface of monocytes, mDCs and pDCs.
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Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com