- About this Journal ·
- Aims and Scope ·
- Article Processing Charges ·
- Author Guidelines ·
- Bibliographic Information ·
- Citations to this Journal ·
- Contact Information ·
- Editorial Board ·
- Editorial Workflow ·
- Free eTOC Alerts ·
- Publication Ethics ·
- Recently Accepted Articles ·
- Reviewers Acknowledgment ·
- Submit a Manuscript ·
- Subscription Information ·
- Table of Contents

ISRN Condensed Matter Physics

Volume 2012 (2012), Article ID 410326, 5 pages

http://dx.doi.org/10.5402/2012/410326

## A First Principle Calculation of Full-Heusler Alloy Co_{2}TiAl: LSDA+ Method

Department of Physics, Mizoram University, Aizawl 796004, India

Received 17 May 2012; Accepted 19 June 2012

Academic Editors: I. Galanakis, A. N. Kocharian, Y. Ohta, and A. D. Zaikin

Copyright © 2012 D. P. Rai and R. K. Thapa. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

#### Abstract

We performed the structure optimization of Co_{2}TiAl based on the generalized gradient approximation (GGA) and linearized augmented plane wave (LAPW) method. The calculation of electronic structure was based on the full-potential linear augmented plane wave (FP-LAPW) method and local spin density approximation exchange correlation LSDA+. We also studied the impact of the Hubbard potential or onsite Coulomb repulsion () on electronic structure; the values are varied within reasonable limits to study the resulting effect on the physical properties of Co_{2}TiAl system. The calculated density of states (DOS) shows that half-metallicity of Co_{2}TiAl decreases with the increase in values.

#### 1. Introduction

Semi-Heusler compound NiMnSb was the first found half-metal ferromagnets (HMFs) by using first principle calculation based on density functional theory [1]. Co_{2}TiAl is a ferromagnetic half-metal with an integral magnetic moment of 1 *μ*B/atom [2]. It has been widely used in magnetic recording tapes, spin valves, giant magnetoresistance (GMR), and so forth. In recent years, it attracts substantial interests because of the half-metallic property and the applicable potential for future spintronics. In half-metal, one spin channel is metallic and the other is insulating with 100% spin polarization at the Fermi level [3, 4]. The electronic and magnetic properties of Co_{2}MnAl [5] and Co_{2}CrSi [6] using local spin density approximation (LSDA) show the half-metallicity at the ground state. Rai and Thapa have also investigated the electronic structure and magnetic properties of - ( = Co, = Mn, = Ge, Sn) type Heusler compounds by using a first principle study and reported HMFs [7]. Rai et al. (2012) also studied the electronic and magnetic properties of Co_{2}CrAl and Co_{2}CrGa using both LSDA and LSDA+ and reported the increase in band gap, hybridization of *d-d* orbitals as well as *d-p* orbitals when treated with LSDA+ [8]. The Fermi level lies in the partially filled band of the majority spin, whereas in the minority spin, the Fermi energy falls in an exchange-split gap between the occupied band and the unoccupied band. Since the magnetic properties are highly spin polarized near the Fermi energy, it is therefore interesting to investigate the orbital contributions of the individual atoms to the magnetic moment of Co_{2}TiAl. The LDA+ approach in which a Hubbard repulsion term is added to the LDA is functional for strong correlation of d or f electrons. Indeed, it provides a good description of the electronic properties of a range of exotic magnetic materials, such as the Mott insulator KCuF_{3} [9] and the metallic oxide LaNiO_{2} [10]. Two main LDA+ schemes are in widespread use today: The Dudarev [11] approach in which an isotropic screened on-site Coulomb interaction is added and the Liechtenstein [9] approach in which the and exchange () parameters are treated separately. Both the choice of LDA+ schemes on the orbital occupation and subsequent properties [12], as well as the dependence of the magnetic properties on the value of [13], has recently been analyzed. It goes without saying that the Hubbard model [14] is of seminal importance in the study of modern condensed matter theory. It is believed that the Hubbard model can describe many properties of strongly correlated electronic systems. The discovery of high temperature superconductivity has enhanced the interest in a set of Hubbard-like models that are used to describe the strongly correlated electronic structure of transition metal oxides [15].

#### 2. Crystal Structure and Calculation

##### 2.1. Crystal Structure

Heusler compounds crystallize in the cubic L_{21} structure (space group ) [16]. Co (green) atoms are at the (1/4, 1/4, 1/4) and (3/4, 3/4, 3/4), Ti (red) at (1/2, 1/2, 1/2), and Al (blue) atoms at (0, 0, 0). The cubic L2_{1} structure consists of four interpenetrating fcc sublattices, two of which are equally occupied by Co. The two Co-site fcc sub-lattices combine to form a simple cubic sub-lattice as shown in Figure 1.

##### 2.2. Method

In this work, we have performed the full-potential linearized augmented plane wave (FP-LAPW) method accomplished by using the WIEN2K code [17] within LSDA and LSDA+ [9] schemes. We have calculated onsite Coulomb repulsion () based on Hubbard model. The standard Hubbard Hamiltonian [18] is of the form: where and creates (annihilates) an electron on site with spin or . A nearest neighbor is denoted by . is the onsite Coulomb repulsion between two electrons on the same site. The hybridization between nearest neighbor orbitals is denoted by , allowing the particles to hop to adjacent sites. The on-site energies are taken to be zero. Considering that the atoms are embedded in a polarizable surrounding, is the energy required to move an electron from one atom to another, far away, in that case. is equal to the difference of ionization potential () and electron affinity () of the solid. Removing an electron from a site will polarize its surroundings thereby lowering the ground state energy of the () electron system [19, 20]. Thus where are the ground state energy of () electron system.

To explore the effects of the on-site Coulomb energy on the electronic structures and the magnetic moments, different from 0.00 Ry up to 0.29 Ry for Co and 0.053 Ry for Ti were used in the LSDA+ calculations.

#### 3. Results and Discussions

We have studied Co_{2}TiAl using simple LSDA; that is, Ry as shown in Figure 2. The Fermi energy () is situated close to the valence band; there exists a small gap of 0.400 eV which is lower than the previously reported value of energy gap 0.456 eV [2] which was calculated by using GGA as given in Table 1. The robustness of half-metallicity in Co_{2}TiAl can be explained by the impact of on the DOS which is taken into consideration in LSDA+. We have plotted DOS for each value of which is shown in Figure 2, and it is seen that the majority-spin bands shift towards low energy and the minority-spin bands shift toward high energy side. In the minority-spin of valence and conduction bands, the maximum contribution to DOS is from the Co atoms. The DOS in majority-spin of conduction band is minimum for Co atoms. For a large , the minority-spin band of Co extends across the Fermi level and gap disappears in . As a result, the DOS is no longer half-metallic. The use of the LSDA+ method increases the width of the energy gap with increase in substantially up to some extent. The respective energy gaps for each value of are for Ry eV, for Ry eV, for Ry eV, and for Ry and Ry eV. Kandpal et al. calculated the energy gap of Co_{2}TiAl, 1.12 eV, using LDA+ [2]. In LSDA, the transition metal states are well separated from the states, whereas the LSDA+ method increases the energetic overlap between these states. In all cases, the gap is between the occupied and unoccupied transition metal states [21]. It can be seen that the bandwidth of the bands for the Co site is indeed smaller than for the Ti site as shown in Figures 2(a) and 2(b). The states on the Co sites are more localized and one can expect a larger on-site Coulomb interaction than that on the Ti site, which is in agreement with [22]. However, the half-metallicity is retained till some value of as shown in Figure 2. Therefore, the dependency of DOS on implies that the half-metallicity is robust sensitive to .

##### 3.1. Magnetic Properties

The calculated partial and total magnetic moments are summarized in Table 2. For Ry, LSDA+ gives the partial moment of 1.0605 *μ*B/atom for Co, −0.71433 *μ*B/atom for Ti, and the total moment was 0.9999 *μ*B/atom. Similarly, LSDA ( Ry) gives the orbital moment of 0.76070 for Co, −0.31578 *μ*B/atom for Ti, and 0.99999 *μ*B/atom for total system being in good agreement with the previously calculated orbital moment 1.00 *μ*B/atom reported by Kandpal [2]. The opposite signs of spin moments between Co and Ti indicate charge transfer from the Ti anion to the Co cation. With the increase of , the total magnetic moment as well as the moment of Co increases and the moment of Ti decreases as shown in Figures 3(a) and 3(b). The increase in magnetic moment is due the double occupancy which is a decreasing function of reported by F. Mancini and F. P. Mancini [23].

#### 4. Conclusion

In conclusion, we have performed FP-LAPW self-consistent calculations for ferromagnetic half-metal Co2TiAl within the LSDA and the LSDA+ schemes. The spin-orbit coupling included in the self-consistent calculations; the orbital magnetic moments are obtained from both the LSDA and the LSDA+ methods. It is found that the on-site Coulomb interaction dramatically enhanced the orbital moments. For Ry and Ry, the calculated total orbital moments are 0.99999 *μ*B/atom and 0.999 *μ*B/atom, respectively, being in good agreement with the previously reported result 1.00 *μ*B/atom [2]. The calculated energy gap was found to be 0.84 eV for Ry. It also appears that decreases double occupancy and hence increases local moments. Our calculated results of for Co and Ti are 0.29 Ry and 0.053 Ry; respectively, the corresponding magnetic moments is not the integral value (HM) that is, 2.258 *μ*_{B}. Also Figure 2 shows that does not lie at the middle of the gap at Ry and ; Ry thus the half metallicity does not exist. By using LSDA+, we have found that Co2TiAl is possible half-metal candidate having magnetic moment 0.99994 u_{B} at Ry. This value of integral magnetic moment supports the condition of half-metallicity. Due to these characteristics like integer value of magnetic moment, 100% spin polarization at and the energy gap at the Fermi level in spin-down channel make application of half-metallic ferromagnets very important. The Co-based Heusler alloys Co_{2} ( is transition elements and is the elements) are the most prospective candidates for the application in spintronics. This is due to a high Curie temperature beyond room temperature and the simple fabrication process such as dc-magnetron sputtering in Co_{2}.

#### Acknowledgments

D. P. RAI acknowledges DST inspire research fellowship and R. K. Thapa a research grant from UGC (New Delhi), India.

#### References

- R. A. de Groot, F. M. Mueller, P. G. van Engen, and K. H. J. Buschow, “New class of materials: half-metallic ferromagnets,”
*Physical Review Letters*, vol. 50, no. 25, pp. 2024–2027, 1983. View at Publisher · View at Google Scholar · View at Scopus - H. C. Kandpal,
*Computational studies on the structure and stabilities of magnetic inter-metallic compounds,dissertation zur Erlanggung des Grades [Doktor der Naturwissenschaften]*, am Fachbereich Chemie, Pharmazie und Geowissenschaften der Johannes Guttenberg-Universitat Mainz, 2006. - I. Zutić, J. Fabian, and S. Das Sarma, “Spintronics: fundamentals and applications,”
*Reviews of Modern Physics*, vol. 76, pp. 323–410, 2004. View at Publisher · View at Google Scholar - J. de Boeck, W. Van Roy, J. Das et al., “Technology and materials issues in semiconductor-based magnetoelectronics,”
*Semiconductor Science and Technology*, vol. 17, no. 4, pp. 342–354, 2002. View at Publisher · View at Google Scholar · View at Scopus - D. P. Rai, J. Hashemifar, M. Jamal et al., “Study of Co
_{2}MnAl Heusler alloy as half metallic ferromagnet,”*Indian Journal of Physics*, vol. 84, no. 6, pp. 717–721, 2010. View at Scopus - D. P. Rai, Sandeep, M. P. Ghimire, and R. K. Thapa, “Structural stabilities, elastic and thermodynamic properties of Scandium Chalcogenides via first-principles calculations,”
*Bulletin des Sciences Mathématiques*, vol. 34, pp. 1219–1222, 2011. - D. P. Rai and R. K. Thapa, “Electronic structure and magnetic properties of
*X*_{2}*YZ*(*X*= Co,*Y*= Mn,*Z*= Ge, Sn) type Heusler compounds by using a first principle study,”*Phase Transition: A Multinational Journal*, pp. 1–11, 2012. - D. P. Rai, Sandeep, M. P. Ghimire, and R. K. Thapa, “Electronic tructure and magnetic properties of Co
_{2}*YZ*(*Y*= Cr,*V*= Al, Ga) type Heusler compounds: A first Principle Study,”*International Journal of Modern Physics B*, vol. 26, pp. 1250071–1250083, 2012. - A. I. Liechtenstein, V. I. Anisimov, and J. Zaanen, “Density-functional theory and strong interactions: orbital ordering in Mott-Hubbard insulators,”
*Physical Review B*, vol. 52, no. 8, pp. R5467–R5470, 1995. View at Publisher · View at Google Scholar · View at Scopus - K. W. Lee and W. E. Pickett, “Infinite-layer LaNiO
_{2}: Ni^{1+}is not Cu^{2+},”*Physical Review B*, vol. 70, Article ID 165109, 2004. - S. L. Dudarev, G. A. Botton, S. Y. Savrasov, C. J. Humphreys, and A. P. Sutton, “Electron-energy-loss spectra and the structural stability of nickel oxide: an LSDA$+$U study,”
*Physical Review B*, vol. 57, no. 3, pp. 1505–1509, 1998. View at Scopus - E. R. Ylvisaker, W. E. Pickett, and K. Koepernik, “Anisotropy and magnetism in the LSDA$+$U method,”
*Physical Review B*, vol. 79, Article ID 035103, 2009. - S. Y. Savrasov, A. Toropova, M. I. Katsnelson, A. I. Lichtenstein, V. Antropovand, and G. Kotliar, “Electronic structure and magnetic properties of solids,”
*Zeitschrift Für Kristallographie*, vol. 220, pp. 473–488, 2005. View at Publisher · View at Google Scholar - J. Hubbard, “Electron correlations in narrow energy bands,”
*Proceedings of the Royal Society A*, vol. 276, pp. 238–257, 1963. View at Publisher · View at Google Scholar - P. W. Anderson, “The resonating valence bond state in La
_{2}CuO_{4}and superconductivity,”*Science*, vol. 235, no. 4793, pp. 1196–1198, 1987. View at Scopus - F. Heusler, “Über magnetische Manganlegierungen,”
*Verhandlungen der Deutschen Physikalischen Gesellschaft*, vol. 12, p. 219, 1903. - P. Blaha, K. Schwarz, G. K. H. Madsen, D. Kvasnicka, J. Luitz, and K. Schwarz, “An augmented plane wave plus local orbitals program for calculating crystal properties,”
*Wien2K User's Guide*, Technische Universität Wien, Wien, Austria, 2008. - L. M. Roth, “New method for linearizing many-body equations of motion in statistical mechanics,”
*Physical Review Letters*, vol. 20, pp. 1431–1434, 1968. - J. van den Brink, M. B. J. Meinders, and G. A. Sawatzky, “Influence of screening effects and inter-site Coulomb repulsion on the insulating correlation gap,”
*Physica B*, vol. 206-207, pp. 682–684, 1995. View at Scopus - K. H. G. Madsen and P. Novák, “Charge order in magnetite. An LDA$+$U study,”
*Europhysics Letters*, vol. 69, p. 777, 2005. - I. Galanakis, “Orbital magnetism in the half-metallic Heusler alloys,”
*Physical Review B*, vol. 71, Article ID 012413, 2005. - C. Ederer and M. Komelj, “Magnetic coupling in CoCr
_{2}O_{4}and MnCr_{2}O_{4}: an LSDA$+$U study,”*Physical Review B*, vol. 76, Article ID 064409, 9 pages, 2007. - F. Mancini and F. P. Mancini, “One dimensional extended Hubbard model in the atomic limit,”
*Cond. Mat. Str-El*, vol. 77, pp. 061120–061121, 2008.