| Topological Origin of Fragility, Network Adaptation, and Rigidity and Stress Transitions in Especially Homogenized Nonstoichiometric Binary GexS100–x Glasses S Chakraborty, P Boolchand The Journal of Physical Chemistry B 118 (8), 2249-2263, 2014 | 56 | 2014 |
| Structural properties of Ge-S amorphous networks in relationship with rigidity transitions: An ab initio molecular dynamics study S Chakraborty, P Boolchand, M Micoulaut Physical Review B 96 (9), 094205, 2017 | 30 | 2017 |
| Designing heavy metal oxide glasses with threshold properties from network rigidity S Chakraborty, P Boolchand, M Malki, M Micoulaut The Journal of Chemical Physics 140 (1), 2014 | 19 | 2014 |
| Topology and glass structure evolution in (BaO) x ((B2O3) 32 (SiO2) 68) 100− x ternary—Evidence of rigid, intermediate, and flexible phases C Holbrook, S Chakraborty, S Ravindren, P Boolchand, JT Goldstein, ... The Journal of Chemical Physics 140 (14), 2014 | 16 | 2014 |
| Progress, challenges, and rewards in probing melt dynamics, configurational entropy change, and topological phases of group V‐and group IV‐based multicomponent sulfide glasses S Chakravarty, BS Almutairi, R Chbeir, S Chakraborty, M Bauchy, ... physica status solidi (b) 257 (11), 2000116, 2020 | 11 | 2020 |
| Glass homogeneity precursive to self-organization P Boolchand, S Bhosle, K Gunasekera, K Vignarooban, S Chakraborty Journal of Optoelectronics and Advanced Materials 13 (11), 1353, 2011 | 9 | 2011 |
| Linking molecular origin of melt fragility index with topological phases of network glasses VK Gogi, A Mandal, A Welton, S Bhosle, S Chakraborty, K Gunasekera, ... Journal of Non-Crystalline Solids 631, 122920, 2024 | 4 | 2024 |
| Topological origin of glass formation, rigidity and stress transitions, conductivity and fragility in specially homogeneous Heavy Metal Oxide and Chalcogenide systems S Chakraborty University of Cincinnati, 2014 | 2 | 2014 |
| Origin of the Raman active 490 cm-1 mode in binary As-S and Ge-S and ternary Ge-As-S glasses from compositional studies and Ab-initio Cluster calculations. S Chakravarty, R Chbeir, B Almutairi, S Chakraborty, K Jackson, ... Bulletin of the American Physical Society 65, 2020 | | 2020 |
| Topology and glass structure evolution in (BaO){sub x}((B {sub 2} O {sub 3}){sub 32}(SiO {sub 2}){sub 68}){sub 100− x} ternary—Evidence of rigid, intermediate, and flexible phases C Holbrook, S Chakraborty, S Ravindren, P Boolchand, JT Goldstein, ... Journal of Chemical Physics 140 (14), 2014 | | 2014 |
| Topology and glass structure evolution in (BaO) x ((B₂O₃) ₃₂ (SiO₂) ₆₈)(100-x) ternary--evidence of rigid, intermediate, and flexible phases. C Holbrook, S Chakraborty, S Ravindren, P Boolchand, JT Goldstein, ... The Journal of Chemical Physics 140 (14), 144506-144506, 2014 | | 2014 |
| Fragility, network adaptation, rigidity- and stress- transitions in homogenized binary GexS100-x glasses S Chakraborty, P Boolchand APS March Meeting Abstracts 2014, J29. 005, 2014 | | 2014 |
| Fragility, Intermediate Phase and Polaronic conductivity in heavy metal oxides S Chakraborty, K Gunasekera, P Boolchand, M Malki, M Micoulaut APS March Meeting Abstracts 2013, Y11. 015, 2013 | | 2013 |
| Boson mode, Intermediate Phase, and glass molecular structure of heavy metal Oxides S Chakraborty, P Boolchand APS March Meeting Abstracts 2012, Y7. 011, 2012 | | 2012 |
| Evidence of an Intermediate Phase in bulk alloy oxide glass sysem S Chakraborty, P Boolchand APS March Meeting Abstracts 2011, Y31. 008, 2011 | | 2011 |
