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Systematic Studies of Mechanism behind Thermal Expansion in Silicides for Data-driven Materials Design R. Ishimura 1 , S. Fujii 1 , M. Yoshiya 1, 2 , 1 Department of Adaptive Machine Systems, Osaka University, Osaka, JAPAN 2 Nanostructures Research Laboratory, Japan Fine Ceramics Center, Nagoya, JAPAN Upon attempting to improve energy conversion efficiency, attention has been paid to intermetallic materials, especially metal disilicides, for next-generation gas turbine engine due to their remarkable mechanical properties, oxidation resistance, and stability at elevated temperature. Unlike metals or alloys, it exhibits variety of crystal structures and interatomic bonding deviates from the average between metallic bonding and covalent bonding [1] . Their unique bonding, on the other hand, bring about difficulties to obtain systematic understanding of mechanism behind the properties. Coefficient of thermal expansion (CTE) of crystal lattice is one of the most important properties since difference in CTEs between a silicide blade and a neighboring layer causes fracture or spallation of the upper layer. According to the equation that defines Grüneisen parameter, , CTE, , is given by α= where Cv, , and KT, are heat capacity at constant volume, density, and bulk modulus, respectively [2] . While origins of other three properties are clear, the way to control Grüneisen parameter is as difficult as to control CTE itself according to the equation and thus dependence of CTE on materials is often attributed only to Grüneisen parameter with factors that determine CTE remain unclear. Besides, although impurity is often added to adjust lattice matching between phases to control microstructure, its impact on CTE remains unclear, disabling to predict the lattice matching at elevated temperature. In order to enable data-driven materials design with better CTE and to optimize CTE without deteriorating other properties for practical application at elevated temperature, candidates of factors that have influence on CTE needs to be determined. In this study, systematic calculations of CTEs of metal silicides including disilicides have been carried out by ab initio lattice dynamics within quasi-harmonic approximation using VASP and phonopy codes [3], [4] to obtain accurate forces between atoms and phonon states, respectively. Sufficiently good numerical accuracy was imposed in the calculations to obtain accurate free energy as functions of temperature and volume. Through determining equilibrium lattice constants as a function of temperature, CTE was derived as a function of temperature for a given crystal structure and chemical composition. Figure 1 shows crystal structures of MSi2 and M2Si where M denotes metallic 122 AMTC Letters Vol. 5 (2016) ©2016 Japan Fine Ceramics Center
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Page 1: Systematic Studies of Mechanism behind Thermal Expansion ...amtc6.com/wp-content/uploads/2018/10/amtc_5_059.pdf · CTEs in silicides decreases with increasing ratio of M-M bonding

Systematic Studies of Mechanism behind Thermal Expansion in Silicides for Data-driven Materials Design

R. Ishimura1, S. Fujii1, M. Yoshiya1, 2,

1 Department of Adaptive Machine Systems, Osaka University, Osaka, JAPAN

2 Nanostructures Research Laboratory, Japan Fine Ceramics Center, Nagoya, JAPAN

Upon attempting to improve energy conversion efficiency, attention has been

paid to intermetallic materials, especially metal disilicides, for next-generation gas

turbine engine due to their remarkable mechanical properties, oxidation resistance, and

stability at elevated temperature. Unlike metals or alloys, it exhibits variety of crystal

structures and interatomic bonding deviates from the average between metallic bonding

and covalent bonding [1]. Their unique bonding, on the other hand, bring about difficulties

to obtain systematic understanding of mechanism behind the properties.

Coefficient of thermal expansion (CTE) of crystal lattice is one of the most

important properties since difference in CTEs between a silicide blade and a neighboring

layer causes fracture or spallation of the upper layer. According to the equation that

defines Grüneisen parameter, , CTE, , is given by α= where Cv, , and KT,

are heat capacity at constant volume, density, and bulk modulus, respectively [2]. While

origins of other three properties are clear, the way to control Grüneisen parameter is as

difficult as to control CTE itself according to the equation and thus dependence of CTE

on materials is often attributed only to Grüneisen parameter with factors that determine

CTE remain unclear. Besides, although impurity is often added to adjust lattice matching

between phases to control microstructure, its impact on CTE remains unclear, disabling

to predict the lattice matching at elevated temperature. In order to enable data-driven

materials design with better CTE and to optimize CTE without deteriorating other

properties for practical application at elevated temperature, candidates of factors that have

influence on CTE needs to be determined.

In this study, systematic calculations of CTEs of metal silicides including

disilicides have been carried out by ab initio lattice dynamics within quasi-harmonic

approximation using VASP and phonopy codes [3], [4] to obtain accurate forces between

atoms and phonon states, respectively. Sufficiently good numerical accuracy was imposed

in the calculations to obtain accurate free energy as functions of temperature and volume.

Through determining equilibrium lattice constants as a function of temperature, CTE was

derived as a function of temperature for a given crystal structure and chemical

composition.

Figure 1 shows crystal structures of MSi2 and M2Si where M denotes metallic

122

AMTC Letters Vol. 5 (2016) ©2016 Japan Fine Ceramics Center

Page 2: Systematic Studies of Mechanism behind Thermal Expansion ...amtc6.com/wp-content/uploads/2018/10/amtc_5_059.pdf · CTEs in silicides decreases with increasing ratio of M-M bonding

element. Both of them have cubic

fluorite crystal structures with M

and Si occupying the opposite

sites. The ratio of M to Si are

different between the two,

resulting in different numbers of

M-M and Si-Si bondings. It brings

about the difference in

coordination numbers of M and Si,

with 8 Si around M in MSi2 and 4

Si around M in M2Si. Figure 2

compares CTEs of MSi2 and M2Si

for selected M. These results show

that there is negative correlation

between bulk modulus and the

CTEs, and this trend follows the

aforementioned equation. It also

shows that CTEs of MSi2 is

greater than that of M2Si in

general. These suggest that the

CTEs in silicides decreases with

increasing ratio of M-M bonding

to Si-Si bonding. However, additional calculations of CTEs for pure metals and Si show

that the CTEs of Si is smaller than that of metals, indicating that the CTEs of silicides are

not determined simply by the balance between bondings species in a unitcell. In addition,

it is revealed that the magnitude of influence of net charge on the CTEs is different

between the two classes of silicides, indicating that interatomic bonding specific to

silicides needs to be further analyzed for optimizing CTEs of disilicides for practical use.

Acknowledgment: This study is supported by Grant-in-Aid for Scientific Research on

Innovative Areas "Exploration of nanostructure-property relationships for materials

innovation" (Grant No. 25106005) from the Ministry of Education, Culture, Sports,

Science and Technology (MEXT), Japan.

References: [1] M Yamaguchi, et al., Kinzokukan kago_

butsu nyu_

mon, (2004) 117 [2]

E. Gruneisen, Handb. Phys., 10 (1926), 1. [3] G. Kresse, et al., Phys. Rev. B, 54 (1996),

11169 [4] A. Togo, et al., Phys. Rev. B, 78 (2008), 134106-1-9

FIG. 1. Crystal structures of silicides MSi2 and M2Si. Gray and blue balls are M atoms and Si respectively.

(a) MSi2 (b) M

2Si

FIG. 2. Relation between bulk modulus and CTE in MSi2 and M2Si.

123

AMTC Letters Vol. 5 (2016) ©2016 Japan Fine Ceramics Center


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