{"id":23,"date":"2023-11-04T18:43:42","date_gmt":"2023-11-04T18:43:42","guid":{"rendered":"https:\/\/www-cxcp1.tifrh.res.in\/~smarajit\/?page_id=23"},"modified":"2023-11-09T18:18:28","modified_gmt":"2023-11-09T18:18:28","slug":"publications","status":"publish","type":"page","link":"https:\/\/www.tifrh.res.in\/~smarajit\/?page_id=23","title":{"rendered":"Publications"},"content":{"rendered":"<p>[et_pb_section fb_built=&#8221;1&#8243; _builder_version=&#8221;4.23&#8243; _module_preset=&#8221;default&#8221; custom_padding=&#8221;3px|||||&#8221; global_colors_info=&#8221;{}&#8221;][et_pb_row _builder_version=&#8221;4.23&#8243; _module_preset=&#8221;default&#8221; border_width_bottom=&#8221;1px&#8221; border_color_bottom=&#8221;#e2e2e2&#8243; global_colors_info=&#8221;{}&#8221;][et_pb_column type=&#8221;4_4&#8243; _builder_version=&#8221;4.23&#8243; _module_preset=&#8221;default&#8221; global_colors_info=&#8221;{}&#8221;][et_pb_post_title meta=&#8221;off&#8221; featured_image=&#8221;off&#8221; _builder_version=&#8221;4.23&#8243; _module_preset=&#8221;default&#8221; global_colors_info=&#8221;{}&#8221;][\/et_pb_post_title][\/et_pb_column][\/et_pb_row][et_pb_row use_custom_gutter=&#8221;on&#8221; gutter_width=&#8221;2&#8243; _builder_version=&#8221;4.23&#8243; _module_preset=&#8221;default&#8221; global_colors_info=&#8221;{}&#8221;][et_pb_column type=&#8221;4_4&#8243; _builder_version=&#8221;4.23&#8243; _module_preset=&#8221;default&#8221; global_colors_info=&#8221;{}&#8221;][et_pb_code _builder_version=&#8221;4.23&#8243; _module_preset=&#8221;default&#8221; hover_enabled=&#8221;0&#8243; sticky_enabled=&#8221;0&#8243; custom_css_free_form=&#8221;ol li{line-height:2;margin-bottom: 20px;}||li p{display: inline;}&#8221;]<\/p>\n<ol reversed><!-- [et_pb_line_break_holder] --><\/p>\n<h4>Under Review\/Submitted Preprints<\/h4>\n<p><\/br><!-- [et_pb_line_break_holder] --><\/p>\n<li><pee align=\"justify\">Non-trivial activity dependence of static length scale and critical tests of active random first-order transition theory &#8211; K. Paul, S.K. Nandi and Smarajit Karmakar, arXiv:2111.09829 (2021).<\/pee><\/li>\n<p><!-- [et_pb_line_break_holder] --><\/p>\n<li><pee align=\"justify\">Cavitation instabilities in amorphous solids via secondary mechanical perturbations \u2013 U.A. Dattani, R. Sharma, Smarajit Karmakar, and P. Chaudhuri, arxiv:2303.04529 (2023).<\/pee><\/li>\n<p><!-- [et_pb_line_break_holder] --><\/p>\n<li><pee align=\"justify\">Activity-Induced Annealing leads to Ductile-to-Brittle Transition in Amorphous Solids &#8211; R. Sharma, Smarajit Karmakar, arXiv:2305.17545 (submitted 2023).<\/pee><\/li>\n<p><!-- [et_pb_line_break_holder] --><\/p>\n<li><pee align=\"justify\">Length-scale Dependence of Stokes-Einstien Breakdown in Active Glass-forming Liquids &#8211; A. Mutneja, Smarajit Karmakar, arXiv:2306.10229 (submitted 2023).<\/pee><\/li>\n<p><!-- [et_pb_line_break_holder] --><\/p>\n<li><pee align=\"justify\">Soft Matrix: Extracting Inherent Length Scales in Sheared Amorphous Solids &#8211; M. Adhikari, P. Chaudhuri, Smarajit Karmakar, V.V. Krishnan, N. Pingua, S. Sengupta, A. Sreekumari, V.V. Vasisht, arXiv:2306.04917 (under review PNAS Nexus 2023).<\/pee><\/li>\n<p><!-- [et_pb_line_break_holder] --><\/p>\n<li><pee align=\"justify\">Yielding transition of amorphous solids in the presence of aspherical impurities &#8211; A. Mutneja, B.P. Bhowmik, Smarajit Karmakar*, arXiv:2307.01002 (submitted 2023).<\/pee><\/li>\n<p><!-- [et_pb_line_break_holder] --><\/p>\n<li><pee align=\"justify\">Athermal quasistatic cavitation in amorphous solids: effect of random pinning &#8211; U.A. Dattani, Smarajit Karmakar, P. Chaudhuri, arXiv:2306.05348 (submitted 2023).<\/pee><\/li>\n<p><!-- [et_pb_line_break_holder] --><\/p>\n<li><pee align=\"justify\">Quantum fluctuations lead to glassy electron dynamics in a good metal \u2013 S.K. Ojha, S. Hazra, S. Bera, S.K. Gogoi, P. Mandal, J. Maity, A. Gloskovskii, C Schlueter, Smarajit Karmakar, M. Jain, S. Banerjee, V. Gopalan, S. Middey (under review Nature 2023) arXiv:2306.14464.<\/pee><\/li>\n<p><!-- [et_pb_line_break_holder] --><\/p>\n<h4>Peer-reviewed Publications<\/h4>\n<p><\/br><!-- [et_pb_line_break_holder] --><\/p>\n<li><pee align=\"justify\">Soft-Pinning: Experimental Validation of Static Correlations in Supercooled Molecular Glass-forming Liquids &#8211; R. Das, B.P. Bhowmik, A.B. Puthirath, T.N. Narayanan, Smarajit Karmakar, Natl. Acad. Sci. Nexus (USA) 2 (9) pgad277(2023).<\/pee><\/li>\n<p><!-- [et_pb_line_break_holder] --><\/p>\n<li><pee align=\"justify\">Dynamic Heterogeneity in active glass-forming liquids in qualitatively different compared to its equilibrium behaviour &#8211; K. Paul, A. Mutneja, S.K. Nandi and Smarajit Karmakar, Natl. Acad. Sci. (USA) 120 (34), e2217073120 (2023).<\/pee><\/li>\n<p><!-- [et_pb_line_break_holder] --><\/p>\n<li><pee align=\"justify\">Enhanced Vibrational Stability in Glass Droplets \u2013 S. Chakraborty, V.V. Krishnan, K. Ramola and Smarajit Karmakar*, Natl. Acad. Sci. Nexus (USA) 2 (9) pgad289 (2023).<\/pee><\/li>\n<p><!-- [et_pb_line_break_holder] --><\/p>\n<li><pee align=\"justify\">A Novel Method to Probe the Pronounced Growth of Correlation Lengths in an Active Glass-forming Liquids using Elongated Probe &#8211; A Mutneja, S Karmakar, Physical Review E Letters 108 (2) L022601 (2023).<\/pee><\/li>\n<p><!-- [et_pb_line_break_holder] --><\/p>\n<li><pee align=\"justify\">Dependence of the glass transition and jamming densities on spatial dimension &#8211; Adhikari, Smarajit Karmakar, S. Sastry, Physical Review Letters 131, 168202 (2023)<\/pee><\/li>\n<p><!-- [et_pb_line_break_holder] --><\/p>\n<li><pee align=\"justify\">Annealing effects of multidirectional oscillatory shear in model glass formers &#8211; V.V. Krishnan, K. Ramola, and Smarajit Karmakar, Physical Review Applied 19, 024004 (2023).<\/pee><\/li>\n<p><!-- [et_pb_line_break_holder] --><\/p>\n<li><pee align=\"justify\">Quantifying Dynamical Heterogeneity Length Scales of Interface Water across Model Membrane Phase Transition &#8211; S Malik, Smarajit Karmakar, and A Debnath, Journal of Chemical Physics 158, 091103 (2023).<\/pee><\/li>\n<p><!-- [et_pb_line_break_holder] --><\/p>\n<li><pee align=\"justify\">Relaxation time scales of interfacial water upon fluid to ripple to gel phase transitions of bilayers \u2013 S Malik, Smarajit Karmakar and A Debnath, Journal of Chemical Physics 158, 114503 (2023).<\/pee><\/li>\n<p><!-- [et_pb_line_break_holder] --><\/p>\n<li><pee align=\"justify\">Giant electroviscous effects in a ferroelectric nematic liquid crystal &#8211; MP Kumar, J Karcz, P Kula, S Karmakar, S Dhara, Physical Review Applied 19 (4) 044082 (2023).<\/pee><\/li>\n<p><!-- [et_pb_line_break_holder] --><\/p>\n<li><pee align=\"justify\">Kinetic Fragility Directly Correlates with the Many-body Static Amorphous Order in Glass-Forming Liquids &#8211; I Tah, Smarajit Karmakar, Physical Review Materials 6 (3) 035601 (2022).<\/pee><\/li>\n<p><!-- [et_pb_line_break_holder] --><\/p>\n<li><pee align=\"justify\">Universal mechanical instabilities in the energy landscape of amorphous solids: Evidence from athermal quasistatic expansion &#8211; UA Dattani, S Karmakar, P Chaudhuri Physical Review E 106 (5), 055004 (2022).<\/pee><\/li>\n<p><!-- [et_pb_line_break_holder] --><\/p>\n<li><pee align=\"justify\">Thermodynamics and its correlation with dynamics in a mean-field model and pinned systems: A comparative study using two different methods of entropy calculation &#8211; U.k. Nandi, P. Patel, M. Moid, M.K. Nandi, S. Sengupta, Smarajit Karmakar, P.K. Maiti, C. Dasgupta, S.M. Bhattacharyya, The Journal of Chemical Physics, 156, 014503 (2022).<\/pee><\/li>\n<p><!-- [et_pb_line_break_holder] --><\/p>\n<li><pee align=\"justify\">Universal non-Debye low-frequency vibrations in sheared amorphous solids &#8211; Vishu V Krishnan, Kabir Ramola, and Smarajit Karmakar, Soft Matter 18, 3395 (2022).<\/pee><\/li>\n<p><!-- [et_pb_line_break_holder] --><\/p>\n<li><pee align=\"justify\">Enhanced Phonon Peak in Four-point Dynamic Susceptibility in the Supercooled active Glass-forming Liquids &#8211; S. Dey. A. Mutneja, and Smarajit Karmakar, Soft Matter 18, 7309 (2022).<\/pee><\/li>\n<p><!-- [et_pb_line_break_holder] --><\/p>\n<li><pee align=\"justify\">Dynamics of Rod like Particles in Supercooled Liquids&#8211;Probing Dynamic Heterogeneity and Amorphous Order \u2013 Anoop Mutneja and Smarajit Karmakar, Physical Review Applied 16 (3), 034022 (2021).<\/pee><\/li>\n<p><!-- [et_pb_line_break_holder] --><\/p>\n<li><pee align=\"justify\">Translational dynamics of rod-like probe in supercooled liquids: an experimentally realisable method to study Stokes-Einstein breakdown, dynamic heterogeneity, and amorphous order, Anoop Mutneja and Smarajit Karmakar, Soft Matter 17, 5738 (2021).<\/pee><\/li>\n<p><!-- [et_pb_line_break_holder] --><\/p>\n<li><pee align=\"justify\">Spatial Dimensionality Dependence of Heterogeneity, Breakdown of the Stokes\u2013Einstein Relation, and Fragility of a Model Glass-Forming Liquid- M. Adhikari, Smarajit Karmakar, S. Sastry, The Journal of Physical Chemistry B 125, 10232 (2021).<\/pee><\/li>\n<p><!-- [et_pb_line_break_holder] --><\/p>\n<li><pee align=\"justify\">Understanding Slow and Heterogeneous Dynamics in Model Supercooled Glass-forming Liquids \u2013 I Tah, A Mutneja, and Smarajit Karmakar, ACS Omega 6(11), 7229 (2021) (Invited Review Article).<\/pee><\/li>\n<p><!-- [et_pb_line_break_holder] --><\/p>\n<li><pee align=\"justify\">Cavity formation in deformed amorphous solids on the nanoscale \u2013 K Paul, R Dasgupta, J Horbach and Smarajit Karmakar*, Physical Review Research 2, 042012 (2020).<\/pee><\/li>\n<p><!-- [et_pb_line_break_holder] --><\/p>\n<li><pee align=\"justify\">Time Scales of Fickian Diffusion and Lifetime of Dynamic Heterogeneity \u2013 R Das, C. Dasgupta and Smarajit Karmakar*, Frontiers in Physics 8, 210 (2020).<\/pee><\/li>\n<p><!-- [et_pb_line_break_holder] --><\/p>\n<li><pee align=\"justify\">Signature of Dynamical heterogeneity in Spatial correlations of particle displacement and its Temporal evolution in Supercooled liquids, I. Tah and Smarajit Karmakar*, Physical Review Research, 2, 022067 (2020).<\/pee><\/li>\n<p><!-- [et_pb_line_break_holder] --><\/p>\n<li><pee align=\"justify\">Cusp singularities in Hessian element distributions of amorphous media &#8211; VV Krishnan, Smarajit Karmakar, K Ramola, Physical Review Research 2, 042025 (2020).<\/pee><\/li>\n<p><!-- [et_pb_line_break_holder] --><\/p>\n<li><pee align=\"justify\">Dynamic coupling of hydration layer to a fluid phospholipid membrane: intermittency and multiple time-scale relaxations &#8211; A Srivastava, S Malik, Smarajit Karmakar, and A Debnath, Physical Chemistry Chemical Physics, 22, 21158 (2020).<\/pee><\/li>\n<p><!-- [et_pb_line_break_holder] --><\/p>\n<li><pee align=\"justify\">Effect of pinning on the Yielding Transition of Amorphous Solids \u2013 BP. Bhowmik, P. Chaudhuri and Smarajit Karmakar*, Physical Review Letters 123, 185501 (2019).<\/pee><\/li>\n<p><!-- [et_pb_line_break_holder] --><\/p>\n<li><pee align=\"justify\">Particle pinning suppresses spinodal criticality in the shear banding instability &#8211; BP. Bhowmik, Smarajit Karmakar, I Procaccia, and C Rainone &#8211; Physical Review E 100, 052110 (2019).<\/pee><\/li>\n<p><!-- [et_pb_line_break_holder] --><\/p>\n<li><pee align=\"justify\">Quantification of patio-temporal scales of dynamical heterogeneity of water near lipid membranes above supercooling &#8211; A Srivastava, Smarajit Karmakar, and A Debnath. Soft Matter 15, 9805 (2019).<\/pee><\/li>\n<p><!-- [et_pb_line_break_holder] --><\/p>\n<li><pee align=\"justify\">Role of \u03b1 and \u03b2 Relaxation in Collapsing Dynamics of Polymer Chain in Supercooled Glass-forming Liquids \u2013 M. Mukherjee, J. Mondal and Smarajit Karmakar*, Chem. Phys. 150, 114503 (2019).<\/pee><\/li>\n<p><!-- [et_pb_line_break_holder] --><\/p>\n<li><pee align=\"justify\">Non-Gaussianity of van Hove Function and Dynamic Heterogeneity Length Scale \u2013 BP Bhowmik, I Tah and Smarajit Karmakar*, Rev. E 98, 022122 (2018).<\/pee><\/li>\n<p><!-- [et_pb_line_break_holder] --><\/p>\n<li><pee align=\"justify\">Glass Transition in Supercooled Liquids with Medium Range Crystalline Order \u2013 I Tah, S Sengupta, S Sastry, C Dasgupta and Smarajit Karmakar*, Rev. Lett. 121, 085703 (2018).<\/pee><\/li>\n<p><!-- [et_pb_line_break_holder] --><\/p>\n<li><pee align=\"justify\">Possible Universal Relation Between Short time \u03b2 Relaxation and Long time \u03b1 Relaxation in Glass-forming Liquids. \u2013 R. Das, I. Tah and Smarajit Karmakar*, Chem. Phys. 149, 024501 (2018).<\/pee><\/li>\n<p><!-- [et_pb_line_break_holder] --><\/p>\n<li><pee align=\"justify\">Plastic deformation of a permanently bonded network: Stress relaxation by pleats &#8211; S. Ganguly, D. Das, J. Horbach, P. Sollich, Smarajit Karmakar, S. Sengupta, Chem. Phys. 149, 184503 (2018).<\/pee><\/li>\n<p><!-- [et_pb_line_break_holder] --><\/p>\n<li><pee align=\"justify\">Do Thermodynamically Stable rigid solids exist? \u2013 P. Nath, S. Ganguly, J. Horbach, P. Sollich, Smarajit Karmakar and S. Sengupta, Nat\u2019l. Acad. Sci. 115, E4322 (2018).<\/pee><\/li>\n<p><!-- [et_pb_line_break_holder] --><\/p>\n<li><pee align=\"justify\">Block Analysis for the Calculation of Dynamic and Static Length Scales in Glass-Forming Liquids \u2013 S Chakrabarty, I Tah, Smarajit Karmakar* and C Dasgupta Phys. Lett. 119 (20) 205502 (2017).<\/pee><\/li>\n<p><!-- [et_pb_line_break_holder] --><\/p>\n<li><pee align=\"justify\">Equilibrium and Dynamic Pleating of a Crystalline bonded Network \u2013 S Ganguly, P Nath, J Horbach, P Sollich, Smarajit Karmakar*, and S Sengupta, Journal of Chem. Phys. 146 (12), 124501 (2017).<\/pee><\/li>\n<p><!-- [et_pb_line_break_holder] --><\/p>\n<li><pee align=\"justify\">Pinning Susceptibility: A Novel Method to Study Growth of Amorphous Order in Glass-forming Liquids \u2013 R Das, S Chakrabarty, and Smarajit Karmakar*, Soft Matter 13, 6929-6937 (2017).<\/pee><\/li>\n<p><!-- [et_pb_line_break_holder] --><\/p>\n<li><pee align=\"justify\">An Overview on Short and Long Time Relaxations in Glass-forming Supercooled Liquids \u2013 Smarajit Karmakar*, Journal of Physics: Conference Series 759 (1), 012008 (2016).<\/pee><\/li>\n<p><!-- [et_pb_line_break_holder] --><\/p>\n<li><pee align=\"justify\">Understanding the Dynamics of supercooled liquids with Random Pinning within the Random First Order Transition Theory \u2013 S Chakrabarty, R Das, Smarajit Karmakar*, C Dasgupta, Chem. Phys. 145, 034507 (2016).<\/pee><\/li>\n<p><!-- [et_pb_line_break_holder] --><\/p>\n<li><pee align=\"justify\">Understanding Stokes-Einstein in Supercooled Liquids using Random Pinning \u2013 BP Bhowmik, R Das and Smarajit Karmakar*, Stat. Mech. : Theory and Experiments 074003 (2016).<\/pee><\/li>\n<p><!-- [et_pb_line_break_holder] --><\/p>\n<li><pee align=\"justify\">Excess Vibrational Density of States and the Brittle to Ductile Transition in Crystalline and Amorphous Solids \u2013 JS Babu, C Mondal, S Sengupta, Smarajit Karmakar*, Soft Matter 12(4), 1210 (2016).<\/pee><\/li>\n<p><!-- [et_pb_line_break_holder] --><\/p>\n<li><pee align=\"justify\">Short-time \u03b2-relaxation in glass-forming liquids is cooperative in nature \u2013 Smarajit Karmakar*, C Dasgupta, S Sastry, Rev. Lett. 116, 085701 (2016).<\/pee><\/li>\n<p><!-- [et_pb_line_break_holder] --><\/p>\n<li><pee align=\"justify\">The Static lengthscale characterizing the glass transition at lower temperatures- R Gutierrez, Smarajit Karmakar, YG. Pollak and I Procaccia, Lett. 111(5), 56009 (2016).<\/pee><\/li>\n<p><!-- [et_pb_line_break_holder] --><\/p>\n<li><pee align=\"justify\">Length scales in glass forming liquids and related systems&#8221; by Smarajit Karmakar, C Dasgupta, S Sastry, Report on Progress in Physics 79, 016601 (2015).<\/pee><\/li>\n<p><!-- [et_pb_line_break_holder] --><\/p>\n<li><pee align=\"justify\">Vanishing of configurational entropy may not imply an ideal glass transition in randomly pinned liquids- S Chakrabarty, Smarajit Karmakar*, C Dasgupta, Natl. Acad. Sci. (USA), 201512745 (2015).<\/pee><\/li>\n<p><!-- [et_pb_line_break_holder] --><\/p>\n<li><pee align=\"justify\">Dynamics of glass forming liquids with randomly pinned particles &#8211; S Chakrabarty, Smarajit Karmakar*, C Dasgupta, Scientific reports 5 (2015).<\/pee><\/li>\n<p><!-- [et_pb_line_break_holder] --><\/p>\n<li><pee align=\"justify\">Glass-like slow dynamics in a colloidal solid with multiple ground states &#8211; C Mondal, Smarajit Karmakar, S Sengupta, The Journal of Physical Chemistry B 119 (34), 10902\u201310910 (2015).<\/pee><\/li>\n<p><!-- [et_pb_line_break_holder] --><\/p>\n<li><pee align=\"justify\">Distribution of diffusion coefficients and connection to Stokes-Einstein Violation in Super cooled liquids \u2013 S Sengupta and Smarajit Karmakar*, The Journal of Chemical Physics 140 (22), 224505 (2014).<\/pee><\/li>\n<p><!-- [et_pb_line_break_holder] --><\/p>\n<li><pee align=\"justify\">Growing Length Scales at the Glass Transition &#8211; Smarajit Karmakar, C Dasgupta and S Sastry, Annual Review of Condensed Matter Physics 5, 1 (2013).<\/pee><\/li>\n<p><!-- [et_pb_line_break_holder] --><\/p>\n<li><pee align=\"justify\">Comparison of Static Length Scales Characterizing the Glass Transition &#8211; G Biroli, Smarajit Karmakar*, and I Procaccia, Rev. Lett. 111, 165701 (2013).<\/pee><\/li>\n<p><!-- [et_pb_line_break_holder] --><\/p>\n<li><pee align=\"justify\">Breakdown of the Stokes-Einstein relation in two, three and four dimensions \u2013 S Sengupta, Smarajit Karmakar, C Dastupta and S Sastry, Chem. Phys. 138, 12A548 (2013).<\/pee><\/li>\n<p><!-- [et_pb_line_break_holder] --><\/p>\n<li><pee align=\"justify\">Random Pinning Glass Model \u2013 Smarajit Karmakar and G Parisi, Nat. Acad. Sci. (USA) 110, 2752 (2013).<\/pee><\/li>\n<p><!-- [et_pb_line_break_holder] --><\/p>\n<li><pee align=\"justify\">Finite Size Scaling for the Glass Transition: The Role of a Static Length Scale &#8211; Smarajit Karmakar* and I Procaccia, Physical Review E 86, 061502 (2012).<\/pee><\/li>\n<p><!-- [et_pb_line_break_holder] --><\/p>\n<li><pee align=\"justify\">The nature of the \u03b2-peak in the loss modulus of amorphous solids \u2013 Y Cohen, Smarajit Karmakar, I Procaccia, and K Samwer, EPL (Europhysics Letters) 100, 36003 (2012).<\/pee><\/li>\n<p><!-- [et_pb_line_break_holder] --><\/p>\n<li><pee align=\"justify\">Relaxation Mechanisms in Glassy Dynamics: the Arrhenius and Fragile Regimes &#8211; HGE. Hentschel, Smarajit Karmakar, I Procaccia and J Zylberg, Rev. E 85, 061501 (2012).<\/pee><\/li>\n<p><!-- [et_pb_line_break_holder] --><\/p>\n<li><pee align=\"justify\">Adam-Gibbs relation for glass-forming liquids in 2, 3 and 4 dimensions \u2013 S Sengupta, Smarajit Karmakar, C Dasgupta and S Sastry, Physical Review Letters 109, 095705 (2012).<\/pee><\/li>\n<p><!-- [et_pb_line_break_holder] --><\/p>\n<li><pee align=\"justify\">Universality of Plastic Instability in Strained Amorphous Solids \u2013 R Dasgupta, Smarajit Karmakar, I Procaccia, Physical Review Letters 108, 075701 (2012).<\/pee><\/li>\n<p><!-- [et_pb_line_break_holder] --><\/p>\n<li><pee align=\"justify\">An Athermal Brittle to Ductile Transition in Amorphous Solids- O Dauchot, Smarajit Karmakar, I Procaccia, and J Zylberg \u2013 Physical Review E 84, 046105 (2011).<\/pee><\/li>\n<p><!-- [et_pb_line_break_holder] --><\/p>\n<li><pee align=\"justify\">Direct Estimate of the Static Length-Scale Accompanying the Glass Transition &#8211; Smarajit Karmakar, E Lerner, and I Procaccia, Physica A, 391, 1001 (2012).<\/pee><\/li>\n<p><!-- [et_pb_line_break_holder] --><\/p>\n<li><pee align=\"justify\">Do Athermal Amorphous Solids Exist? &#8211; H.G.E. Hentschel, Smarajit Karmakar, E Lerner, I Procaccia \u2013 Physical Review E 83, 061101 (2011).<\/pee><\/li>\n<p><!-- [et_pb_line_break_holder] --><\/p>\n<li><pee align=\"justify\">Effect of the Inter-particle Potential on the Yield Stress of Amorphous Solid \u2013 Smarajit Karmakar, E Lerner, I Procaccia, and J Zylberg \u2013 Physical Review E 83, 046106 (2011).<\/pee><\/li>\n<p><!-- [et_pb_line_break_holder] --><\/p>\n<li><pee align=\"justify\">Statistical Physics of the Yielding Transition in Amorphous Solids \u2013 Smarajit Karmakar, E Lerner and I Procaccia &#8211; Physical Review E Rapid Comm. 82, 055103(R) (2010).<\/pee><\/li>\n<p><!-- [et_pb_line_break_holder] --><\/p>\n<li><pee align=\"justify\">Statistical Physics of Elasto-Plastic Steady States in Amorphous Solids: Finite Temperatures and Strain Rates &#8211; Smarajit Karmakar, E Lerner, I Procaccia, J Zylberg \u2013 Physical Review E. 82, 031301 (2010).<\/pee><\/li>\n<p><!-- [et_pb_line_break_holder] --><\/p>\n<li><pee align=\"justify\">Time Scales in the Theory of Elasto-Plasticity of Amorphous Solids &#8211; L Boue, P Harrowell, Smarajit Karmakar, E Lerner, I Procaccia, I Regev, J Zylberg &#8211; arXiv:0911.4646.<\/pee><\/li>\n<p><!-- [et_pb_line_break_holder] --><\/p>\n<li><pee align=\"justify\">Athermal Nonlinear Elastic Constants of Amorphous Solids &#8211; Smarajit Karmakar, E Lerner, and I Procaccia, Physical Review E 82, 02615 (2010).<\/pee><\/li>\n<p><!-- [et_pb_line_break_holder] --><\/p>\n<li><pee align=\"justify\">Plasticity-Induced Anisotropy in Amorphous Solids: The Bauschinger Effect \u2013 Smarajit Karmakar, E Lerner, I Procaccia, Physical Review E. 82, 02614 (2010).<\/pee><\/li>\n<p><!-- [et_pb_line_break_holder] --><\/p>\n<li><pee align=\"justify\">Comment on \u201cScaling Analysis of Dynamic &#8230;.. Liquid\u201d by Stein and Andersen \u2013 Smarajit Karmakar, C Dasgupta, S Sastry, Physical Review Letters 105, 019801 (2010).<\/pee><\/li>\n<p><!-- [et_pb_line_break_holder] --><\/p>\n<li><pee align=\"justify\">Analysis of dynamic heterogeneity in a glass former from the spatial correlations of mobility &#8211; Smarajit Karmakar, C Dasgupta, S Sastry, Physical Review Letters 105, 015701 (2010).<\/pee><\/li>\n<p><!-- [et_pb_line_break_holder] --><\/p>\n<li><pee align=\"justify\">Predicting plastic flow events in athermal shear-strained amorphous solids \u2013 Smarajit Karmakar, A Lemaitre, E Lerner and I Procaccia, Physical Review Letters, 104, 215502 (2010).<\/pee><\/li>\n<p><!-- [et_pb_line_break_holder] --><\/p>\n<li><pee align=\"justify\">Size of Plastic Events in Strained Amorphous Solids at Finite Temperatures \u2013 HGE. Hentschel, Smarajit Karmakar, E Lerner, I Procaccia, Physical Review Letters, 104, 025501 (2010).<\/pee><\/li>\n<p><!-- [et_pb_line_break_holder] --><\/p>\n<li><pee align=\"justify\">Growing length and time scales in glass forming liquids &#8211; Smarajit Karmakar, C Dasgupta, and S Sastry, Nat. Acad. Sci. (USA) 106, 3675 (2009).<\/pee><\/li>\n<p><!-- [et_pb_line_break_holder] --><\/p>\n<li><pee align=\"justify\">Signatures of Dynamical Heterogeneity in the Structure of Glassy Free-energy Minima \u2013 P Chaudhuri, Smarajit Karmakar and C Dasgupta, Physical Review Letters 100, 125701 (2008).<\/pee><\/li>\n<p><!-- [et_pb_line_break_holder] --><\/p>\n<li><pee align=\"justify\">Equilibrium Glassy Phase in a Polydisperse Hard-Sphere System &#8211; P Chaudhuri, Smaraji Karmakar, C Dasgupta, HR Krishnamurthy, and AK Sood &#8211; Physical Review Letters 95, 248301 (2005).<\/pee><\/li>\n<p><!-- [et_pb_line_break_holder] --><\/p>\n<li><pee align=\"justify\">Physics of Disordered Systems &#8211; Smarajit Karmakar, Resonance 27 (1), 19-38 (2022).<\/pee><\/li>\n<p><!-- [et_pb_line_break_holder] --><\/p>\n<li><pee align=\"justify\">Interplay of Disorder and Fluctuations in Physical Systems &#8211; Celebrating the Science of Giorgio Parisi, Physics Nobel laureate 2021, &#8211; S.K. Nandi and Smarajit Karmakar, Physics News 4 (2022).<\/pee><\/li>\n<p><!-- [et_pb_line_break_holder] --><\/ol>\n<p>[\/et_pb_code][\/et_pb_column][\/et_pb_row][\/et_pb_section]<\/p>\n","protected":false},"excerpt":{"rendered":"","protected":false},"author":1,"featured_media":0,"parent":0,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"","meta":{"_et_pb_use_builder":"on","_et_pb_old_content":"","_et_gb_content_width":"","footnotes":""},"class_list":["post-23","page","type-page","status-publish","hentry"],"_links":{"self":[{"href":"https:\/\/www.tifrh.res.in\/~smarajit\/index.php?rest_route=\/wp\/v2\/pages\/23","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/www.tifrh.res.in\/~smarajit\/index.php?rest_route=\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/www.tifrh.res.in\/~smarajit\/index.php?rest_route=\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/www.tifrh.res.in\/~smarajit\/index.php?rest_route=\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/www.tifrh.res.in\/~smarajit\/index.php?rest_route=%2Fwp%2Fv2%2Fcomments&post=23"}],"version-history":[{"count":7,"href":"https:\/\/www.tifrh.res.in\/~smarajit\/index.php?rest_route=\/wp\/v2\/pages\/23\/revisions"}],"predecessor-version":[{"id":60,"href":"https:\/\/www.tifrh.res.in\/~smarajit\/index.php?rest_route=\/wp\/v2\/pages\/23\/revisions\/60"}],"wp:attachment":[{"href":"https:\/\/www.tifrh.res.in\/~smarajit\/index.php?rest_route=%2Fwp%2Fv2%2Fmedia&parent=23"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}