{"id":21,"date":"2023-11-04T18:01:42","date_gmt":"2023-11-04T18:01:42","guid":{"rendered":"https:\/\/www-cxcp1.tifrh.res.in\/~saroj\/?page_id=21"},"modified":"2026-03-13T03:30:39","modified_gmt":"2026-03-13T03:30:39","slug":"publications","status":"publish","type":"page","link":"https:\/\/www.tifrh.res.in\/~saroj\/publications\/","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;5px|||||&#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; title_font=&#8221;|600|||||||&#8221; title_text_color=&#8221;#007FE0&#8243; global_colors_info=&#8221;{}&#8221;][\/et_pb_post_title][\/et_pb_column][\/et_pb_row][et_pb_row _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_text _builder_version=&#8221;4.23&#8243; _module_preset=&#8221;default&#8221; inline_fonts=&#8221;Martel Sans,Advent Pro&#8221; global_colors_info=&#8221;{}&#8221;]<\/p>\n<div class=\"tifrhcontent\">\n<div class=\"manu-pagecontent-wrap\">\n<h4>Submitted<\/h4>\n<ul>\n<li>A <span style=\"font-size: 14px;\"><span><\/span><\/span>constitutive model for discontinuous shear thickening in epithelial tissues, Tanmoy Ghosh, Kabir Ramola, And Saroj Kumar Nandi, <a href=\"https:\/\/arxiv.org\/abs\/2602.20886\">arXiv: 2602.20886<\/a><\/li>\n<li><span style=\"font-size: 14px;\"><span>Active Inhomogeneous Mode-Coupling Theory (aIMCT) for Dense Systems of Self-Propelled Particles, Soumitra Kolya, Puneet Pareek, and Saroj Kumar Nandi, <a href=\"https:\/\/arxiv.org\/abs\/2410.15928\">arXiv:2410.15928<\/a><\/span><\/span><\/li>\n<li><span style=\"font-size: 14px;\">Non-trivial activity dependence of static length scale and critical tests of active random first-order transition theory, Kallol Paul, Saroj Kumar Nandi, and Smarajit Karmakar, <\/span><a href=\"https:\/\/arxiv.org\/abs\/2111.09829\" style=\"font-size: 14px;\">arXiv:2111.09829<\/a><\/li>\n<\/ul>\n<h4><span style=\"font-family: ABeeZee; font-weight: normal;\">Publications<\/span><\/h4>\n<ol>\n<li><span>Scaling the glassy dynamics of active particles: Tunable fragility and reentrance, Puneet Pareek, Peter Sollich, Saroj Kumar Nandi, and Ludovic Berthier, <a href=\"https:\/\/www.pnas.org\/doi\/10.1073\/pnas.2516624123\">Proc. Natl. Acad. Sci. (USA), <strong>123<\/strong>, e2516624123 (2026)<\/a><\/span><\/li>\n<li>Fluctuation-dominated phase ordering in the one dimensional Truncated Inverse Distance Square Ising (TIDSI) model, Souvik Sadhukhan, Mustansir Barma, and Saroj Kumar Nandi, <a href=\"https:\/\/journals.aps.org\/pre\/abstract\/10.1103\/5l43-3rl9\">Phys. Rev. E <strong>112<\/strong>, 024114 (2025)<\/a><\/li>\n<li class=\"heading-lg-bold mb-2\">Growing length and time scales in activity-mediated glassy dynamics in confluent cell monolayers<span style=\"font-size: 14px;\">, Souvik Sadhukhan, Chandan Dasgupta, and Saroj Kumar Nandi, <a href=\"https:\/\/journals.aps.org\/pre\/abstract\/10.1103\/PhysRevE.111.054416\">Phys. Rev. E <strong>111<\/strong>, <span>054416 (2025)<\/span><\/a><\/span><\/li>\n<li><span>An elastoplastic model approach for the relaxation dynamics of active glasses, Tanmoy Ghosh, Peter Sollich, and Saroj Kumar Nandi, <a href=\"https:\/\/pubs.rsc.org\/en\/content\/articlelanding\/2025\/sm\/d4sm01394h\">Soft Matter <strong>21<\/strong>, 3047 (2025).<\/a><\/span><span style=\"font-size: 14px;\"><\/span><\/li>\n<li><span style=\"font-size: 14px;\">The structure-dynamics feedback mechanism governs the glassy dynamics in epithelial monolayers, Satyam Pandey, Soumitra Kolya, Padmashree D, Souvik Sadhukhan, Tamal Das, and Saroj Kumar Nandi, <a href=\"https:\/\/pubs.rsc.org\/en\/content\/articlehtml\/2025\/sm\/d4sm01059k\">Soft Matter <strong>21<\/strong>, 269 (2025).<\/a><\/span><\/li>\n<li>Motility driven glassy dynamics in confluent epithelial monolayers, Souvik Sadhukhan, Manoj Kumar Nandi, Satyam Pandey, Matteo Paoluzzi, Chandan Dasgupta, Nir Gov, Saroj Kumar Nandi<span style=\"color: #000000;\">, <\/span><a href=\"https:\/\/pubs.rsc.org\/en\/content\/articlelanding\/2024\/sm\/d4sm00352g\">Soft Matter, <strong>20<\/strong>, 6160 (2024).<\/a><\/li>\n<li><span style=\"font-size: 14px;\">A shape-driven reentrant jamming transition in confluent monolayers of synthetic cell-mimics, Pragya Arora, Souvik Sadhukhan, Saroj Kumar Nandi, Dapeng Bi, A K Sood, Rajesh Ganapathy, <\/span><a href=\"https:\/\/www.nature.com\/articles\/s41467-024-49044-z\" style=\"font-size: 14px;\">Nat. Commun. <strong>15<\/strong>, 5645 (2024).<\/a><\/li>\n<li><span style=\"color: #4f4f4f;\">A perspective on active glassy dynamics in biological systems<\/span><em style=\"font-family: inherit; font-size: medium;\">, <\/em>Souvik Sadhukhan, Subhodeep Dey, Smarajit Karmakar, and Saroj Kumar Nandi, <a href=\"https:\/\/link.springer.com\/article\/10.1140\/epjs\/s11734-024-01188-1\" target=\"_blank\" rel=\"noopener\">Eur. Phys. J. Spec. Top. <strong>233<\/strong>, 3193 (2024)<\/a><\/li>\n<li><span style=\"font-family: inherit; font-weight: normal;\">Stretched exponential to power-law: crossover of relaxation in a kinetically constrained model<\/span><span style=\"color: #333333;\">, Sukanta Mukherjee, Puneet Pareek, Mustansir Barma, and\u00a0Saroj Kumar Nandi<\/span>, <span style=\"font-size: 14px; font-family: inherit; color: rgba(9, 119, 188, 0.96);\"><a href=\"https:\/\/iopscience.iop.org\/article\/10.1088\/1742-5468\/ad1f55\/meta\" style=\"color: rgba(9, 119, 188, 0.96);\">J. Stat. Mech. (2024) 023205<\/a><\/span><\/li>\n<li><em><span style=\"font-size: medium;\">Different glassy characteristics ar<\/span>e related to either caging or dynamical heterogeneity<\/em>,\u00a0Puneet Pareek, Monoj Adhikari, Chandan Dasgupta, and\u00a0Saroj Kumar Nandi, <a href=\"https:\/\/pubs.aip.org\/aip\/jcp\/article\/159\/17\/174503\/2919300\/Different-glassy-characteristics-are-related-to\"><em>J. Chem. Phys.<\/em><span><strong> 159<\/strong>, 17450<span style=\"color: #2d9bef;\">3 (2023)<\/span><\/span><\/a>.<\/li>\n<li><em>Dynamic heterogeneity in active glasses is inherently different from its equilibrium behaviour<\/em>, Kallol Paul, Anoop Mutneja, Saroj Kumar Nandi, and Smarajit Karmakar, <a href=\"https:\/\/www.pnas.org\/doi\/10.1073\/pnas.2217073120\">PNAS <strong>120<\/strong>, e2217073120 (2023)<\/a>.\n<div class=\"page\" title=\"Page 1\"><\/div>\n<\/li>\n<li><em>On the origin of universal cell shape variability in confluent epithelial monolayers<\/em>,\u00a0Souvik Sadhukhan and Saroj Kumar Nandi, <a href=\"https:\/\/elifesciences.org\/articles\/76406\">eLife, <b>11<\/b>:e76406 (2022)<\/a>.<\/li>\n<li><em>Affinity and valence impact the extent and symmetry of phase separation of multivalent proteins<\/em>,\u00a0Saroj Kumar Nandi, Daniel \u00d6sterle,\u00a0Meta Heidenreich, Emmanuel D. Levy, Samuel A. Safran,\u00a0<a href=\"https:\/\/journals.aps.org\/prl\/abstract\/10.1103\/PhysRevLett.129.128102\">Phys. Rev. Lett. <b>129<\/b>, 128102 (2022)<\/a>.<\/li>\n<li><em>The random first-order transition theory of active glass in the high-activity regime<\/em>, Rituparno Mandal, Saroj Kumar Nandi, Chandan Dasgupta, Peter Sollich, and Nir S. Gov, \u00a0<a href=\"https:\/\/iopscience.iop.org\/article\/10.1088\/2399-6528\/ac9c47\/meta\"><em>J. Phys. Commun.<\/em> <b>6<\/b> 115001 (2022)<\/a>.<\/li>\n<li><em>Interplay of Disorder and Fluctuations in Physical Systems \u2013 Celebrating the Science of Giorgio Parisi, Physics Nobel Laureate 2021<\/em>, Saroj Kumar Nandi and Smarajit Karmakar, <a href=\"https:\/\/www.tifr.res.in\/~ipa1970\/news\/514\/V51-4_A1.pdf\">Physics News, 54, 4 (2021)<\/a>.<\/li>\n<li><em>Theory and simulation for equilibrium glassy dynamics in cellular Potts model of confluent biological tissue<\/em>, Souvik Sadhukhan and Saroj Kumar Nandi,\u00a0<a href=\"https:\/\/journals.aps.org\/pre\/abstract\/10.1103\/PhysRevE.103.062403\">Phys. Rev. E\u00a0<b>103<\/b>, 062403 (2021)<\/a>.<\/li>\n<li><em>Size-stretched exponential relaxation in a model with arrested states<\/em>, Vaibhav Gupta, Saroj Kumar Nandi, and Mustansir Barma, <a href=\"https:\/\/journals.aps.org\/pre\/abstract\/10.1103\/PhysRevE.102.022103\">Phys. Rev. E <b> 102 <\/b>, 022103 (2020)<\/a>.<\/li>\n<li><em>Designer protein assemblies with tunable phase diagrams in living cells<\/em>, Meta Heidenreich, Joseph M. Georgeson, Emanuele Locatelli, Lorenzo Rovigatti, Saroj Kumar Nandi, Avital Steinberg, Yotam Nadav, Eyal Shimoni, Samuel A. Safran, Jonathan P. K. Doye &amp; Emmanuel D. Levy <a href=\"https:\/\/www.nature.com\/articles\/s41589-020-0576-z\" target=\"_blank\" rel=\"noopener\"> Nat. Chem. Biol. <b>16<\/b>, 939, (2020) <\/a>.<\/li>\n<li><em>Effective temperature of active fluids and sheared soft glassy materials<\/em>, Saroj Kumar Nandi and Nir S. Gov, <a href=\"https:\/\/rd.springer.com\/article\/10.1140\/epje\/i2018-11731-7\" target=\"_blank\" rel=\"noopener\">Euro. Phys. J. E, <b>41<\/b>, 117 (2018)<\/a>.<\/li>\n<li><em>A Random First Order Transition Theory for active glassy systems <\/em>, Saroj Kumar Nandi, R. Mandal, P. Bhuyan, C. Dashupta, M. Rao and Nir S. Gov, <a href=\"https:\/\/www.pnas.org\/content\/115\/30\/7688\" target=\"_blank\" rel=\"noopener\">Proc. Natl. Acad. Sci. (USA), <strong>115<\/strong>, 7688 (2018)<\/a>.<\/li>\n<li><em> Protein gradients in single cells induced by their coupling to \u201cmorphogen\u201d-like diffusion<\/em>, Saroj Kumar Nandi and Sam A. Safran, <a href=\"https:\/\/aip.scitation.org\/doi\/10.1063\/1.5021086\" target=\"_blank\" rel=\"noopener\">J. Chem. Phys. <strong>148 <\/strong>, 205101 (2018)<\/a>. \u2014 The paper was selected as feature article, cover image and highlighted in\u00a0<a href=\"https:\/\/aip.scitation.org\/doi\/10.1063\/1.5040347\" target=\"_blank\" rel=\"noopener\">AIP Scilight<\/a><\/li>\n<li><em> Activity-dependent self-regulation of viscous length scales in biological systems<\/em>, Saroj Kumar Nandi, <a href=\"https:\/\/journals.aps.org\/pre\/abstract\/10.1103\/PhysRevE.97.052404\" target=\"_blank\" rel=\"noopener\">Phys. Rev. E. <strong>97<\/strong>, 052404 (2018)<\/a><\/li>\n<li><em>Nonequilibrium mode-coupling theory for dense active systems of self-propelled particles<\/em>, Saroj Kumar Nandi and Nir S. Gov, <a href=\"https:\/\/pubs.rsc.org\/en\/content\/articlelanding\/2017\/sm\/c7sm01648d#!divAbstract\" target=\"_blank\" rel=\"noopener\">Soft Matter <b>13<\/b>, 7609 (2017)<\/a><\/li>\n<li><em>Spinodals with Disorder: from Avalanches in Random Magnets to Glassy Dynamics<\/em>, Saroj Kumar Nandi, Giulio Biroli and Gilles Tarjus, <a href=\"https:\/\/journals.aps.org\/prl\/abstract\/10.1103\/PhysRevLett.116.145701\" target=\"_blank\" rel=\"noopener\">Phys. Rev. Lett. <b>116<\/b>, 145701 (2016)<\/a><\/li>\n<li><em>The glass susceptibility: growth kinetics and saturation under shear<\/em>, Saroj Kumar Nandi and Sriram Ramaswamy, <a href=\"https:\/\/journals.aps.org\/pre\/abstract\/10.1103\/PhysRevE.94.012607\" target=\"_blank\" rel=\"noopener\">Phys. Rev. E <b>94<\/b>, 012607 (2016)<\/a><\/li>\n<li><em>Understanding the approximations of mode-coupling theory for sheared steady states of colloids<\/em>, Saroj Kumar Nandi, <a href=\"https:\/\/journals.aps.org\/pre\/abstract\/10.1103\/PhysRevE.92.042306\" target=\"_blank\" rel=\"noopener\">Phys. Rev. E <b>92<\/b>, 042306 (2015)<\/a><\/li>\n<li><em>Critical dynamical heterogeneities close to continuous second-order glass transitions<\/em>, Saroj Kumar Nandi, Giulio Biroli, Jean-Philippe Bouchaud, Kunimasa Miyazaki and David R. Reichman, <a href=\"https:\/\/journals.aps.org\/prl\/abstract\/10.1103\/PhysRevLett.113.245701\" target=\"_blank\" rel=\"noopener\">Phys. Rev. Lett. <b>113<\/b>, 245701 (2014)<\/a><\/li>\n<li><em>Yielding and large deviations in micellar gels: a model <\/em>, Saroj Kumar Nandi, Bulbul Chakraborty, A. K. Sood and Sriram Ramaswamy, <a href=\"https:\/\/iopscience.iop.org\/article\/10.1088\/1742-5468\/2013\/02\/P02027\/meta\" target=\"_blank\" rel=\"noopener\">J. Stat. Mech. (2013) P02027<\/a><\/li>\n<li><em>How Do Glassy Domains Grow?<\/em>, Saroj Kumar Nandi and Sriram Ramaswamy, <a href=\"https:\/\/journals.aps.org\/prl\/abstract\/10.1103\/PhysRevLett.109.115702\" target=\"_blank\" rel=\"noopener\">Phys. Rev. Lett. <b>109<\/b>, 115702 (2012)<\/a><\/li>\n<li><em>The mode-coupling glass transition in a fluid confined by a periodic potential<\/em>, Saroj Kumar Nandi, Sarika Maitra Bhattacharyya and Sriram Ramaswamy, <a href=\"https:\/\/journals.aps.org\/pre\/abstract\/10.1103\/PhysRevE.84.061501\" target=\"_blank\" rel=\"noopener\">Phys. Rev. E <b>84<\/b>, 061501 (2011)<\/a><\/li>\n<li><em>Comment on \u201cLayering transition in confined molecular thin films: Nucleation and growth\u201d<\/em>, Saroj Kumar Nandi, <a href=\"https:\/\/journals.aps.org\/prb\/abstract\/10.1103\/PhysRevB.74.167401\" target=\"_blank\" rel=\"noopener\">Phys. Rev. B <b>74<\/b>, 167401 (2006)<\/a><\/li>\n<\/ol>\n<\/div>\n<\/div>\n<p>[\/et_pb_text][\/et_pb_column][\/et_pb_row][\/et_pb_section]<\/p>\n","protected":false},"excerpt":{"rendered":"<p>Submitted A constitutive model for discontinuous shear thickening in epithelial tissues, Tanmoy Ghosh, Kabir Ramola, And Saroj Kumar Nandi, arXiv: 2602.20886 Active Inhomogeneous Mode-Coupling Theory (aIMCT) for Dense Systems of Self-Propelled Particles, Soumitra Kolya, Puneet Pareek, and Saroj Kumar Nandi, arXiv:2410.15928 Non-trivial activity dependence of static length scale and critical tests of active random first-order [&hellip;]<\/p>\n","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-21","page","type-page","status-publish","hentry"],"_links":{"self":[{"href":"https:\/\/www.tifrh.res.in\/~saroj\/wp-json\/wp\/v2\/pages\/21","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/www.tifrh.res.in\/~saroj\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/www.tifrh.res.in\/~saroj\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/www.tifrh.res.in\/~saroj\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/www.tifrh.res.in\/~saroj\/wp-json\/wp\/v2\/comments?post=21"}],"version-history":[{"count":36,"href":"https:\/\/www.tifrh.res.in\/~saroj\/wp-json\/wp\/v2\/pages\/21\/revisions"}],"predecessor-version":[{"id":350,"href":"https:\/\/www.tifrh.res.in\/~saroj\/wp-json\/wp\/v2\/pages\/21\/revisions\/350"}],"wp:attachment":[{"href":"https:\/\/www.tifrh.res.in\/~saroj\/wp-json\/wp\/v2\/media?parent=21"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}