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Related papers: The Thermally Reversing Window in Ternary GexPxS1-…

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Melt-quenched AsxGexSe1-2x glasses over the composition range, 0 < x < 0.26, are examined in Raman scattering, T-modulated Differential Scanning Calorimetry (MDSC), and 119Sn Mossbauer spectroscopy measurements. The non-reversing enthalpy…

Disordered Systems and Neural Networks · Physics 2007-05-23 Tao Qu , D. G. Georgiev , P. Boolchand , M. Micoulaut

The non-reversing enthalpy near Tg, DHnr, in bulk GexAsxS1-2x glasses is found to display a global minimum (~0) in the 0.11 < x < 0.15 range, the reversibility window. Furthermore, the DHnr term is found to age for glass compositions both…

Materials Science · Physics 2007-05-23 Tao Qu , P. Boolchand

A Raman profiling method is used to monitor growth of GexSe100-x melts and reveals a two step process of homogenization. Resulting homogeneous glasses show the non-reversing enthalpy at Tg, {\Delta}Hnr(x), to show a square-well like…

Disordered Systems and Neural Networks · Physics 2012-07-16 S. Bhosle , K. Gunasekera , P. Boolchand , M. Micoulaut

The structure of binary As_xS_{1-x} glasses is elucidated using modulated-DSC, Raman scattering, IR reflectance and molar volume experiments over a wide range (8%<x<41%) of compositions. We observe a reversibility window in the calorimetric…

Disordered Systems and Neural Networks · Physics 2009-11-13 Ping Chen , Chad Holbrook , P. Boolchand , D. G. Georgiev , K. A. Jackson , M. Micoulaut

Non-reversing relaxation enthalpies (DHnr) at glass transitions Tg(x) in the PxGexSe1-2x ternary display wide, sharp and deep global minima (~ 0) in the 0.09 < x < 0.145 range, within which Tgs become thermally reversing. In this…

Soft Condensed Matter · Physics 2015-05-13 S. Chakravarty , D. G. Georgiev , P. Boolchand , M. Micoulaut

Non-reversing relaxation enthalpies (DHnr) at glass transitions Tg(x) in the PxGexSe1-2x ternary display a wide, sharp and deep global minimum (~0) in the 0.09 < x < 0.145 range, within which Tg becomes thermally reversing. In the…

Disordered Systems and Neural Networks · Physics 2008-06-23 S. Chakravarty , D. G. Georgiev , P. Boolchand , M. Micoulaut

We examine enthalpy relaxation across the chalcogenide glass series GexSe1-x, prepared over close-by compositions using conventional melt-quenching technique. We estimate the timescale {\tau}(Tg) characterizing enthalpic relaxation near the…

Disordered Systems and Neural Networks · Physics 2015-05-05 Deepak Sharma , Sujatha Sampath , A. M. Awasthi

Raman scattering from binary GexSe1-x glasses under hydrostatic pressure shows onset of a steady increase in the frequency of modes of corner-sharing GeSe4 tetrahedral units when the external pressure P exceeds a threshold value Pc. The…

Disordered Systems and Neural Networks · Physics 2007-05-23 Fei Wang , Sergey Mamedov , P. Boolchand , B. Goodman , Meera Chandrasekhar

Raman scattering from binary GexSe1-x glasses under hydrostatic pressure shows onset of a steady increase in the frequency of modes of corner-sharing GeSe4 tetrahedral units when the external pressure P exceeds a threshold value Pc. The…

Soft Condensed Matter · Physics 2009-11-13 Fei Wang , S. Mamedov , P. Boolchand , B. Goodman , Meera Chandrasekhar

Long term aging is studied on several families of chalcogenide glasses including the Ge-Se, As-Se, Ge-P-Se and Ge-As-Se systems. Special attention is given to the As-Se binary, a system that displays a rich variety of aging behavior…

Disordered Systems and Neural Networks · Physics 2015-05-13 Ping Chen , P. Boolchand , D. G. Georgiev

Raman and calorimetric studies on Ge_xSe_{1-x} glasses have provided evidence for the existence of the intermediate phase (IP) in chalcogenide and other glasses. Here, we present X-Ray Absorption Near Edge Structure (XANES) measurements on…

Disordered Systems and Neural Networks · Physics 2009-09-29 F. Inam , G. Chen , D. N. Tafen , D. A. Drabold

Raman scattering on bulk AsxS1-x glasses showes that vibrational modes of As4S4 monomer first appear near x=0.38, and their concentration increases precipitously with increasing x, suggesting that the stoichiometric glass (x=0.40) is…

Materials Science · Physics 2007-05-23 D. G. Georgiev , P. Boolchand , K. A. Jackson

A theoretical and experimental study of the Intermediate Phase (IP) in GexSe1-x is presented. Based on ab initio molecular dynamics (MD) models of these glasses, a generic atomic picture of the IP is discussed thoroughly. X-Ray Absorption…

Disordered Systems and Neural Networks · Physics 2008-06-06 F. Inam , G. Chen , D. N. Tafen , D. A. Drabold

The Brillouin elastic free energy change $DF$ between thermally annealed and quenched $(Na_2O)_x(SiO_2)_{1-x}$ glasses is found to decrease linearly at $x > 0.23$ (floppy phase), and to nearly vanish at $x < 0.18$ (stressed- rigid phase).…

Materials Science · Physics 2007-05-23 Y. Vaills , T. Qu , M. Micoulaut , F. Chaimbault , P. Boolchand

The axiomatic theory of ideally glassy networks, which has proved effective in describing phase diagrams and many properties of chalcogenide, oxide, and even molecular glasses, is here broadened to describe both geometrical properties, such…

Disordered Systems and Neural Networks · Physics 2007-05-23 J. C. Phillips

Bulk glass formation occurs over a very small part of phase space, and "good" glasses (which form even at low quench rates ~ 10K/sec) select an even smaller part of that accessible phase space. An axiomatic theory provides the physical…

Soft Condensed Matter · Physics 2009-11-13 P. Boolchand , Mingji Jin , D. I. Novita , S. Chakravarty

A ternary liquid crystalline mixture was designed to obtain a tilted hexatic smectic phase in the glassy state. Structural, electro-optic, and dielectric properties of the mixture are investigated, and selected measurements are also…

Raman scattering, IR reflectance and modulated DSC measurements are performed on specifically prepared dry (AgI)x(AgPO3)1-x glasses over a wide range of compositions 0 < x < 0.60. A reversibility window is observed in the 0.095< x < 0.378…

Disordered Systems and Neural Networks · Physics 2008-08-11 Deassy I. Novita , P. Boolchand , Mohammed Malki , Matthieu Micoulaut

Liquid water and vitreous B$_2$O$_3$ are the endpoints of a continuous range of random networks in which hydrogen bonds gradually replace covalent bonds. Previous work has shown that glasses can be obtained by quenching in the range $x \le$…

Disordered Systems and Neural Networks · Physics 2009-11-23 Ralf Bruning , Justine B. Galbraith , Katherine E. Braedley , Jonathan Johnstone , Jaqcues Robichaud , Subramanian Balaji , Yahia Djaoued

We introduce a Raman profiling method to track homogenization of Ge$_x$Se$_{100-x}$ melts in real time, and show that 2 gram melts reacted at 950{\deg}C in high vacuum homogenize in 168 hours on a scale of 10{\mu}m. Homogenization of melts…

Disordered Systems and Neural Networks · Physics 2012-07-18 S. Bhosle , K. Gunasekera , P. Chen , P. Boolchand , M. Micoulaut , C. Massabrio
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