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As evidenced in Fig. 2, the distribution is narrow.
The particle size is about 20-80 nm, and the size distribution is narrow.
The nanoclusters exhibit a spherical shape, and the size distribution is narrow showing a mean size of 2.8 ± 0.5 nm.
The NC size distribution is narrow with the standard deviation being less than 20% of the mean NC size.
Nevertheless, we confirm that the Ep distribution is narrow with an upper-energy limit at about 2 MeV.
In a system with homogeneous regime, the bubble-size distribution is narrow and a uniform bubble size, generally in the range 1 7 mm, is found.
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The histogram distribution is narrower for NN than for DGA.
The bubble Sauter diameter decreases and the bubble size distribution is narrower.
The β value of LRS (2.5) distribution is narrower than those of both HRS (1.84) and IRS (1.1), as listed values in Table 1.
This happens faster for the stiff systems, as the velocity distribution is narrower (Figure 9) than for the soft systems (Figure 10).
For example, one may argue that between r = 0 cm and 3.5 cm, the finite speed peak in the speed distribution is narrower compared to r in the range 3.5 cm to 7 cm.
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