Structural evolution during the sub-Tg relaxation of hyperquenched metallic glasses

We report the structural characteristics during the sub-Tg relaxation in hyperquenched La55Al25Ni20 glasses. The sub-Tg relaxation is associated with the structural change in intermediate range order, as manifested by the appearance of a prepeak in the x-ray diffraction spectrum. Such structural change could be the source of the Johari–Goldstein relaxation in metallic glasses. The mechanism governing the evolution of the prepeak is different between the glasses with the fictive temperature below 604 K and those above 604 K. Cooperative motion of atoms in La-centered clusters was further discussed in terms of the atomic bond deficiency model.

[1]  Y. Yue,et al.  Secondary Relaxation in Metallic Glass Formers: Its Correlation with the Genuine Johari-Goldstein Relaxation , 2009 .

[2]  Yat Li,et al.  A model of atom dense packing for metallic glasses with high-solute concentration , 2009 .

[3]  S. Poon,et al.  Diffusion in metallic glasses: Analysis from the atomic bond defect perspective , 2008 .

[4]  Y. Yue,et al.  Secondary relaxation behavior in a strong glass. , 2008, The journal of physical chemistry. B.

[5]  M. Demetriou,et al.  Merging of the α and β relaxations and aging via the Johari–Goldstein modes in rapidly quenched metallic glasses , 2008 .

[6]  S. Poon,et al.  Atomic bond deficiency as a structural defect in amorphous metals: Relevance to glass transitions , 2008 .

[7]  O. P. Rachek X-ray diffraction study of amorphous alloys Al–Ni–Ce–Sc with using Ehrenfest’s formula , 2006 .

[8]  Weihua Wang,et al.  Correlations between elastic moduli and properties in bulk metallic glasses , 2006 .

[9]  Hajime Tanaka Two-order-parameter model of the liquid–glass transition. III. Universal patterns of relaxations in glass-forming liquids , 2005 .

[10]  M Paluch,et al.  Classification of secondary relaxation in glass-formers based on dynamic properties. , 2004, The Journal of chemical physics.

[11]  J. Dyre,et al.  Minimal model for Beta relaxation in viscous liquids. , 2003, Physical review letters.

[12]  Stefano Mossa,et al.  Potential energy, relaxation, vibrational dynamics and the boson peak, of hyperquenched glasses , 2003 .

[13]  G. P. Johari Localized molecular motions of β-relaxation and its energy landscape , 2002 .

[14]  R. Nozaki,et al.  Dielectric relaxation processes in water-in-sorbitol mixtures , 2002 .

[15]  K. Ito,et al.  Merging of alpha and slow beta relaxation in supercooled liquids. , 2002, Physical review. E, Statistical, nonlinear, and soft matter physics.

[16]  Y. Yue,et al.  Determination of the fictive temperature for a hyperquenched glass , 2002 .

[17]  K. Ito,et al.  Non-Arrhenius Behavior of Secondary Relaxation in Supercooled Liquids , 2001, cond-mat/0110394.

[18]  Á. Alegría,et al.  Merging of the Dielectric α and β Relaxations in Glass-Forming Polymers , 2001 .

[19]  H. Wagner,et al.  Dielectric beta relaxations in the glassy state of salol , 1999 .

[20]  H. Wagner,et al.  Equilibrium and Non-Equilibrium Type β-Relaxations: D-Sorbitol versus o-Terphenyl , 1999 .

[21]  S. Corezzi,et al.  Dynamics of epoxies: a full dielectric analysis by wideband spectroscopy , 1998 .

[22]  R. Richert,et al.  Dipolar dynamics of low-molecular-weight organic materials in the glassy state , 1997 .

[23]  D. Fioretto,et al.  Influence of the glass transition on the secondary relaxation of an epoxy resin , 1997 .

[24]  T. Egami Structure studies by X-ray and neutron diffraction: how accurate are they? , 1994 .

[25]  Graham Williams Molecular aspects of multiple dielectric relaxation processes in solid polymers , 1979 .