Shock-induced phase transitions of α-Ce3Al

A series of shock compression experiments on hexagonal α-Ce3Al have been carried out using a two-stage light gas gun. No phase transition was observed in the recovered sample shock compressed at 23.5 GPa. However, as the shock pressure was increased to 27.3 GPa, a face-centered cubic Ce3Al phase was detected in the samples recovered at ambient conditions. Furthermore, a Ce2Al phase was found in the 37.1 GPa shocked sample with a space group Fd-3m and lattice parameter a = 8.26(1) A. These Ce-based alloys may have potential industrial applications due to the heavy-fermion related properties.

[1]  Q. Si,et al.  Superconductivity in Ce- and U-Based ‘‘122’’ Heavy-Fermion Compounds , 2012, 1202.4114.

[2]  Yang Ding,et al.  Long-Range Topological Order in Metallic Glass , 2011, Science.

[3]  Yang Ding,et al.  Origin of pressure-induced polyamorphism in Ce75Al25 metallic glass. , 2010, Physical review letters.

[4]  E. Zaretsky Shock response of iron between 143 and 1275 K , 2009 .

[5]  H. J. Oh,et al.  Magnetic properties of heavy fermion system Ce1-xGdxCoSi3 , 2009 .

[6]  Y. Gupta,et al.  Inelastic deformation and phase transformation of shock compressed silicon single crystals , 2007 .

[7]  P. L. Lee,et al.  Polyamorphism in a metallic glass. , 2007, Nature materials.

[8]  N. Bourne,et al.  Soft recovery of polytetrafluoroethylene shocked through the crystalline phase II-III transition , 2007 .

[9]  R. Delaunay,et al.  Probing the transition in bulk Ce under pressure: a direct investigation by resonant inelastic X-ray scattering. , 2006, Physical review letters.

[10]  J. Taylor,et al.  Magnetic form factor of alpha-Ce: towards understanding the magnetism of cerium. , 2005, Physical review letters.

[11]  N. Ünlü,et al.  Reassessment of Al-Ce and Al-Nd binary systems supported by critical experiments and first-principles energy calculations , 2005 .

[12]  R. Delaunay,et al.  f-State occupancy at the gamma-alpha phase transition of Ce-Th and Ce-Sc alloys. , 2004, Physical review letters.

[13]  C. Greeff,et al.  Shock-induced α–ω transition in titanium , 2001 .

[14]  T. Mizushima,et al.  Heavy fermion behavior in Ce(NixPd1−x)2Si2 , 2001 .

[15]  Hongliang He,et al.  Shock-induced phase transition of -Si3N4 to c-Si3N4 , 2000 .

[16]  A. R. Kutsar,et al.  Isomorphic γ→α phase transition of cerium under shock compression , 1999 .

[17]  H. Okamoto Al-Ce (Aluminum-Cerium) , 1998 .

[18]  M. Andrecut,et al.  Calculation of the crystal field and paramagnetic susceptibility of Ce(Zn1-xCux)2 , 1995 .

[19]  W. Hsieh,et al.  Low Temperature Crystal Structures of Heavy-Fermion Compounds Ce3Al and Ce3Sn , 1993 .

[20]  J. Thompson,et al.  Low temperature crystal structure of Ce3Al , 1990 .

[21]  Willis,et al.  Thermodynamic behavior of the heavy-fermion compounds Ce3X (X=Al,In,Sn). , 1989, Physical review. B, Condensed matter.

[22]  T. Kasuya,et al.  MAGNETIC AND TRANSPORT PROPERTIES OF KONDO COMPOUND α-Ce3Al , 1987 .

[23]  D. J. Gillespie,et al.  HEAVY-FERMION, KONDO, SPIN GLASS-LIKE, AND ANTIFERROMAGNETIC BEHAVIOR IN (Ce,Gd)Al3 , 1987 .

[24]  M. Lavagna,et al.  The γ-α transition in cerium compounds , 1983 .

[25]  A. Takei,et al.  Effects of Oxygen Pressure on the Oxidation Behavior of Ni–20Cr Alloy , 1982 .

[26]  W. Nellis,et al.  Shock compression of aluminum, copper, and tantalum , 1981 .

[27]  P. W. Bridgman The Compressibility and Pressure Coefficient of Resistance of Ten Elements , 1927 .