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Ray A. Plant genetics: RNA cache or genome trash? Nature ;E; discussion E2. A journal article with 2 authors.
Stroebel D, Paoletti P. Neuroscience: A structure to remember. Nature ;—3. A journal article with 3 authors. Detecting sedimentary cycles using autocorrelation of grain size. Sci Rep ; A journal article with 7 or more authors. Parietal-eye phototransduction components and their potential evolutionary implications. Science ;— Grous A.
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Berlin, Heidelberg: Springer; Koch M, Pauls K. A band gap of approximately 1. There is a smaller gap for spin flip excitations from the Fermi level, which is approximately 0. Moreover, the SL magnetization does not depend on the number of monolayers. This has been verified by performing calculations with one monolayer of CrO 2 grown between 3, 7, and 11 monolayers of SnO 2. The Fermi level, E F , is set to zero in a , b , and c.
The Fermi level, E F , is set to zero. An investigation, related to strain effects along the z -direction for the rutile phase of CrO 2 , was made by simulating bulk rutile-CrO 2 , on top of tin dioxide, assuming for CrO 2 the lattice parameter a of SnO 2 , i. These results suggest a magnetization change when the SL is under strain or, in other words, when CrO 2 is compressed.
A similar behavior was found by Srivastava et al. Study of strain effects on the magnetic behavior. Our results showed that the interface effects due to the lattice mismatch do not change the chromium dioxide magnetism characteristics. In conclusion, the results of first-principles electronic structure calculations, within the spin density functional theory, carried out for CrO 2 n SnO 2 n SLs formed by alternating magnetic and non-magnetic layers of rutile-CrO 2 and rutile-SnO 2 , where the number of monolayers n was varied from 1 to 10, have been reported in this article.
As the FM rutile-CrO 2 is unstable at ambient temperature, and known to be stabilized when on top of SnO 2 , it is suggested that CrO 2 n SnO 2 n SLs may be applied to spintronic technologies since they provide efficient spin-polarized carriers. PB performed the ab initio calculations, participated in the analysis, and drafted the manuscript. LS and PB conceived of the study.
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All authors read and approved the final manuscript. National Center for Biotechnology Information , U. Journal List Nanoscale Res Lett v. Nanoscale Res Lett. Published online Feb Author information Article notes Copyright and License information Disclaimer.
Corresponding author. Pablo D Borges: moc. Received Aug 25; Accepted Feb Abstract In this article, using first-principles electronic structure calculations within the spin density functional theory, alternated magnetic and non-magnetic layers of rutile-CrO 2 and rutile-SnO 2 respectively, in a CrO 2 n SnO 2 n superlattice SL configuration, with n being the number of monolayers which are considered equal to 1, 2, Introduction A variety of heterostructures have been studied for spintronics applications, and they have proved to have a great potential for high-performance spin-based electronics [ 1 ].
Theoretical method All the calculations were based on the spin density functional theory. Open in a separate window. Figure 1.
Figure 2. Figure 3. Figure 4. Conclusions In conclusion, the results of first-principles electronic structure calculations, within the spin density functional theory, carried out for CrO 2 n SnO 2 n SLs formed by alternating magnetic and non-magnetic layers of rutile-CrO 2 and rutile-SnO 2 , where the number of monolayers n was varied from 1 to 10, have been reported in this article. Competing interests The authors declare that they have no competing interests.