Electronic structure and magnetism of Fe3-xVxX (X=Si, Ga, and Al) alloys by the KKR-CPA method

被引:364
作者
Bansil, A [1 ]
Kaprzyk, S
Mijnarends, PE
Tobola, J
机构
[1] Northeastern Univ, Dept Phys, Boston, MA 02115 USA
[2] Acad Min & Met, Fac Phys & Nucl Techn, PL-30073 Krakow, Poland
[3] Delft Univ Technol, Interfac Reactor Inst, NL-2629 JB Delft, Netherlands
[4] Northeastern Univ, Dept Phys, Boston, MA 02115 USA
来源
PHYSICAL REVIEW B | 1999年 / 60卷 / 19期
关键词
D O I
10.1103/PhysRevB.60.13396
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
We present first-principles charge- and spin-self-consistent electronic structure computations on the Heusler-type disordered alloys Fe3-xVxX for three different metalloids X = (Si, Ga, and Al). In these calculations we use the methodology based on the Korringa-Kohn-Rostoker formalism and the coherent-potential approximation generalized to treat disorder in multicomponent complex alloys. Exchange correlation effects are incorporated within the local spin density approximation. Total energy calculations for Fe3-xVxSi show that V substitutes preferentially on the Fe(B) site, not on the Fe(A,C) site, in agreement with experiment. Furthermore, calculations have been carried out for Fe3-xVxX alloys (with x = 0.25, 0.50, and 0.75), together with the end compounds Fe3X and Fe2VX, and the limiting cases of a single V impurity in Fe3X and a single Fe(B) impurity in Fe2VX. We delineate clearly how the electronic states and magnetic moments at various sites in Fe3-xVxX evolve as a function of the V content and the metalloid valence. Notably, the spectrum of Fe3-xVxX (X = Al and Ga) develops a pseudogap for the majority as well as minority spin states around the Fermi energy in the V-rich regime, which, together with local moments of Fe(B) impurities, may play a role in the anomalous behavior of the transport properties. The total magnetic moment in Fe3-xVxSi is found to decrease nonlinearly and the Fe(B) moment to increase with increasing x; this is in contrast to expectations of the "local environment" model, which holds that the total moment should vary linearly while the Fe(B) moment should remain constant. The common-band model, which describes the formation of bonding and antibonding states with different weights on the different atoms, however, provides insight into the electronic structure of this class of compounds. [S0163-1829(99)11543-1].
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页码:13396 / 13412
页数:17
相关论文
共 84 条
[21]  
FOEX G, 1938, J PHYS RADIUM, V9, P37
[22]   BRILLOUIN-ZONE INTEGRATION BY FOURIER QUADRATURE - SPECIAL POINTS FOR SUPERLATTICE AND SUPERCELL CALCULATIONS [J].
FROYEN, S .
PHYSICAL REVIEW B, 1989, 39 (05) :3168-3172
[23]   ELECTROINIC AND MAGNETIC-PROPERTIES OF X2MN1-XVXSI (X=FE AND CO) [J].
FUJII, S ;
ISHIDA, S ;
ASANO, S .
JOURNAL OF THE PHYSICAL SOCIETY OF JAPAN, 1994, 63 (05) :1881-1888
[24]   HYPERFINE FIELDS AND ELECTRONIC-STRUCTURES OF THE HEUSLER ALLOYS CO2MNAL, CO2MNGA, CO2MNSI, CO2MNGE, CO2MNSN [J].
FUJII, S ;
SUGIMURA, S ;
ISHIDA, S ;
ASANO, S .
JOURNAL OF PHYSICS-CONDENSED MATTER, 1990, 2 (43) :8583-8589
[25]   ELECTRONIC-STRUCTURE AND SITE PREFERENCE OF TRANSITION-METAL IMPURITIES IN FE3SI [J].
GARBA, EJD ;
JACOBS, RL .
JOURNAL OF PHYSICS F-METAL PHYSICS, 1986, 16 (10) :1485-1494
[26]   Electronic structure of possible 3d 'heavy-fermion' compound Fe2VAl [J].
Guo, GY ;
Botton, GA ;
Nishino, Y .
JOURNAL OF PHYSICS-CONDENSED MATTER, 1998, 10 (08) :L119-L126
[27]   ROLE OF THE LOCAL ENVIRONMENT IN DETERMINING THE SIZES OF THE MAGNETIC-MOMENTS IN FE3AL [J].
HAYDOCK, R ;
YOU, MV .
SOLID STATE COMMUNICATIONS, 1980, 33 (03) :299-302
[28]  
Heusler F., 1903, VERH DTSCH PHYS GES, V5, P219
[29]   MAGNETIZATION STUDIES OF BINARY AND TERNARY ALLOYS BASED ON FE3SI [J].
HINES, WA ;
MENOTTI, AH ;
BUDNICK, JI ;
BURCH, TJ ;
LITRENTA, T ;
NICULESCU, V ;
RAJ, K .
PHYSICAL REVIEW B, 1976, 13 (09) :4060-4068
[30]   CHEMICAL BONDING AND ELECTRONIC-STRUCTURE OF PD2SI [J].
HO, PS ;
RUBLOFF, GW ;
LEWIS, JE ;
MORUZZI, VL ;
WILLIAMS, AR .
PHYSICAL REVIEW B, 1980, 22 (10) :4784-4790