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Magnetic properties of \(\hbox{Ni}_{13-n}\hbox{Al}_n\) clusters with n = 0–13

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Abstract

We report the magnetic properties of small \(\hbox{Ni}_{13-n}\hbox{Al}_n\) clusters with n = 0–13 calculated in the framework of density functional theory. The cluster magnetic moment decreases with the sequential substitution of Ni by Al atoms, which can be attributed to a greater degree of hybridization that forces the pairing of the electrons in the molecular orbitals of Ni and Al. For Ni7Al6, the complete quenching of the cluster magnetic moment appears to be due to the antiferromagnetic alignment of atomic spins as revealed by the spin density plots.

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Notes

  1. The binding energy per atom (E b) is defined as \(\hbox{E}_{\rm b}[\hbox{Ni}_{13-n}\hbox{Al}_n]=(-E[\hbox{Ni}_{13-n} \hbox{Al}_n]+{(\hbox{13-n})}E[\hbox{Ni}]+\hbox{n} E[\hbox{Al}])/(13).\)

  2. The spin gap is defined as \(\begin{array}{l} \delta_{l} = -[\epsilon^{majority}_{HOMO} - \epsilon^{minority}_{LUMO}]\\\delta_{2} = -[\epsilon^{minority}_{HOMO} - \epsilon^{majority}_{LUMO}]. \end{array}\)

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Acknowledgment

Helpful discussions with Prof. Dilip Kanhere and S Gowtham are acknowledged. MDD thanks H. P. T. Arts. and R. Y. K. Science College for providing computing facility and acknowledges partial financial assistance from the University Grant Commission and University of Pune, Pune, India. MAB thanks the Spanish Ministerio de Educación for grant CTQ2006-02976. MDD also gratefully acknowledges Michigan Tech. for providing local hospitality.

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Correspondence to M. D. Deshpande or Ravindra Pandey.

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Deshpande, M.D., Pandey, R., Blanco, M.A. et al. Magnetic properties of \(\hbox{Ni}_{13-n}\hbox{Al}_n\) clusters with n = 0–13. J Nanopart Res 12, 1129–1136 (2010). https://doi.org/10.1007/s11051-009-9654-6

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