The cohesive energies of all the considered boron nanowires are negative and have the absolute value larger than 6.70 eV/atom. This indicates that the dispersive B atoms prefer to bind together and form novel MM-102 supplier nanostructures, which can be seen from literatures about the multi-shaped one-dimensional nanowires [21–27]. Simultaneously, by comparison, the cohesive energies of the considered boron nanowires are a little smaller than those of the bulk α-B and β-B, which are the two most stable of the various B bulks. Therefore, we conclude that all these under-considered Adavosertib order boron nanowires are chemically stable.

However, due to the relatively higher cohesive energy, some of the considered boron nanowires may be metastable, and experimental researchers need to seek the path of synthesizing these materials. Nevertheless, the typical one-dimensional structural characteristic and the attractive electronic and magnetic properties, INCB024360 cell line as shown below, may stimulate

experimental efforts in searching for a synthesizing path of this material. Figure 1 Optimized configurations of the considered boron nanowires (red circles). (a) α-a [100], (b) α-b [010], (c) α-c [001], (d) β-a [100], (e) β-b [010], and (f) β-c [001]. Herein, for the same configuration, the left and right are respectively corresponding to the side and top views. Table 1 Cohesive energies and total magnetic moments of considered boron nanowires and of bulk α-B and β-B Nanostructure E c (eV/atom) M (μB) α-a [100] −6.88 0.02 α-b [010] −6.94 0.00 α-c [001] −6.84 1.98 β-a [100] −6.75 0.00 β-b [010] Non-specific serine/threonine protein kinase −6.74 0.00 β-c [001] −6.76 2.62 α-B −7.42 0.00 β-B −7.39 0.00 To lend further understanding of the nature of the boron nanowires considered above, we studied the electronic structures of all configurations using

the spin-polarized calculations. The calculated total magnetic moments of the six nanowires are listed in the second column of Table 1. It is obvious that for the three boron nanowires obtained from the unit cell of α-B, the nanowires α-a [100] and α-b [010] have the total magnetic moments of approximately equal to zero, while the nanowire α-c [001] has a distinctly different total magnetic moment of 1.98 μB. Moreover, for the three boron nanowires obtained from the unit cell of β-B, the same trend about the total magnetic moments occurs. The nanowires β-a [100] and α-b [010] both have the total magnetic moments also approximately equal to zero, and the nanowire β-c [001] has the total magnetic moments of 2.62 μB. Additionally, in Table 1, we also presented the calculated total magnetic moments of bulk α-B and β-B. Thus, these results indicate that both of the two kinds of boron bulks have no magnetism, with the total magnetic moments equal to zero. For the two magnetic nanowires, α-c [001] and β-c [001], we also set the initial spin configurations to the antiferromagnetic (AFM) order.