{"id":3807,"date":"2019-06-24T02:40:47","date_gmt":"2019-06-23T21:10:47","guid":{"rendered":"http:\/\/www.demo.onlypixels.com\/iisc-phy-bid\/?p=3807"},"modified":"2026-04-28T01:36:41","modified_gmt":"2026-04-27T20:06:41","slug":"superconductivity-in-low-dimensional-systems","status":"publish","type":"post","link":"https:\/\/physics.iisc.ac.in\/~aveek_bid\/superconductivity-in-low-dimensional-systems\/","title":{"rendered":"Superconductivity in low-dimensional systems"},"content":{"rendered":"\n<p>Low-dimensional superconductors \u2014 systems whose size is comparable to or smaller than the superconducting coherence length or penetration depth \u2014 display physics profoundly different from their bulk counterparts. Quantum fluctuations, disorder, and reduced dimensionality conspire to produce emergent phases, anomalous metallic states, and exotic vortex physics. We study these effects in atomically thin van der Waals crystals, disordered thin films, and oxide interfaces.<\/p>\n\n\n\n<p><\/p>\n\n\n\n<p>Some representative results from our group:<\/p>\n\n\n\n<hr class=\"wp-block-separator has-alpha-channel-opacity\"\/>\n\n\n\n<h3 class=\"wp-block-heading\">Superconductivity in atomically thin NbSe\u2082 and van der Waals heterostructures<\/h3>\n\n\n\n<p>Few-layer NbSe\u2082 is a rich platform for studying the interplay between charge order, superconductivity, dimensionality, and spin-orbit coupling. In suspended, ultrathin 2H-NbSe\u2082 devices fabricated on piezoelectric substrates \u2014 allowing independent tuning of thickness, disorder, and strain \u2014 we observed for the first time a dynamically modulated quantum phase transition between two distinct charge density wave (CDW) phases. The conductance fluctuates between two precise values separated by a quantum of conductance, a signature that disappears in disordered or on-substrate devices and arises from a dynamical phase transition between competing CDW states driven by strain.<\/p>\n\n\n\n<p>Moving to the superconducting phase, we used vortex dynamics as a probe of dimensionality. By studying the vortex-solid\/glass to vortex-fluid transition in both 2D and 3D NbSe\u2082 devices through magnetoresistance and nonlinear current-voltage characteristics, we extracted the dynamical critical exponents independently from both measurements. The H-T phase diagrams of 2D and 3D devices are found to be significantly different near the critical point, while both follow universal scaling relations \u2014 establishing that critical vortex dynamics are valid across dimensionalities but with distinct universality.<\/p>\n\n\n\n<p>We then asked whether the exotic Ising superconductivity of monolayer NbSe\u2082 \u2014 where broken inversion symmetry locks spins out-of-plane, producing an anomalously large in-plane upper critical field \u2014 could be extended to thicker, more robust crystals. By proximity-coupling few-layer NbSe\u2082 (~15 nm) to a graphene monolayer in a van der Waals heterostack, we showed that the graphene overlay effectively re-breaks the inversion symmetry of the NbSe\u2082, restoring 2D-Ising superconductivity in a system that would otherwise behave as a 3D superconductor. Finally, using low-frequency conductance fluctuation spectroscopy on a MoS\u2082\/NbSe\u2082 van der Waals heterostructure, we showed that the superconducting transition in this system is percolative, with non-Gaussian fluctuation statistics near the transition temperature revealing long-range correlations absent in either constituent material alone.<\/p>\n\n\n\n<p>H. K. Kundu, S. Ray, K. Dolui, V. Bagwe, P. R. Choudhury, S. B. Krupanidhi, T. Das, P. Raychaudhuri, Aveek Bid \u2014 <a href=\"https:\/\/journals.aps.org\/prl\/abstract\/10.1103\/PhysRevLett.119.226802\">Phys. Rev. Lett. 119, 226802 (2017)<\/a><br>H. K. Kundu, K. R. Amin, J. Jesudasan, P. Raychaudhuri, S. Mukerjee, Aveek Bid <br>P. Baidya, D. Sahani, H. K. Kundu, S. Kaur, P. Tiwari, V. Bagwe, J. Jesudasan, A. Narayan, P. Raychaudhuri, Aveek Bid <br>H. K. Kundu, S. Kaur, V. Bagwe, J. Jesudasan, P. Raychaudhuri, Aveek Bid <\/p>\n\n\n\n<hr class=\"wp-block-separator has-alpha-channel-opacity\"\/>\n\n\n\n<h3 class=\"wp-block-heading\">Emergent phases at oxide interfaces and in disordered 2D superconductors<\/h3>\n\n\n\n<p>The quasi-two-dimensional electron gas (q-2DEG) formed at oxide heterointerfaces such as LaAlO\u2083\/SrTiO\u2083 and LaScO\u2083\/SrTiO\u2083 is a remarkable system in which superconductivity, ferromagnetism, and strong spin-orbit coupling coexist and compete. Using resistance fluctuation spectroscopy and its higher-order statistics \u2014 a technique sensitive to the spatial correlations of the superconducting order parameter \u2014 we mapped the phase diagram of the LaAlO\u2083\/SrTiO\u2083 interface in the magnetic field\u2013spin-orbit interaction energy plane. We found that the relative variance of resistance fluctuations increases by orders of magnitude below the spin-orbit field B<sub>SO<\/sub>, and a non-Gaussian component appears for fields below the upper critical field B<sub>C2<\/sub>. Theoretical calculations confirm that this non-Gaussian noise arises from the percolative nature of the superconducting transition, and allow us to quantify the competing roles of Zeeman energy, spin-orbit interaction energy, and pairing potential in shaping the phase diagram. A complementary study of carrier dynamics at the LaAlO\u2083\/SrTiO\u2083 interface revealed a gate-voltage-tunable Lifshitz transition separating two regimes with strikingly different noise characteristics \u2014 single-band semiconductor-like fluctuations at low carrier density, and inter-band scattering dominated noise above the Lifshitz transition.<\/p>\n\n\n\n<p>Extending this program to the LaScO\u2083\/SrTiO\u2083 interface and to disordered NbN thin films, we uncovered an extraordinarily rich phase diagram that cannot be accommodated within any existing theoretical framework. Close to the superconducting transition temperature, the system hosts a superconducting quantum critical point of the infinite-randomness type, with a dynamical exponent \u03bdz that diverges logarithmically \u2014 consistent with the quantum Griffiths phase scenario. However, below a crossover temperature T*, this quantum critical point is unexpectedly destroyed: the Griffiths phase is suppressed, and the effective dynamical exponent diverges as a power law in temperature rather than logarithmically. This concealment of the quantum Griffiths phase, and the associated destruction of the infinite-randomness critical point, are entirely at odds with existing theoretical predictions and challenge the very concept of a vanishing energy scale at a superconducting quantum critical point in two dimensions.<\/p>\n\n\n\n<p>G. N. Daptary, H. K. Kundu, P. Kumar, A. Dogra, N. Mohanta, A. Taraphder, Aveek Bid <br>G. N. Daptary, P. Kumar, A. Dogra, Aveek Bid <br>S. Kaur, H. K. Kundu, S. Kumar, A. Dogra, R. Narayanan, T. Vojta, Aveek Bid <\/p>\n\n\n\n<p><\/p>\n","protected":false},"excerpt":{"rendered":"<p>Low-dimensional superconductors \u2014 systems whose size is comparable to or smaller than the superconducting coherence length or penetration depth \u2014 display physics profoundly different from their bulk counterparts. Quantum fluctuations, disorder, and reduced dimensionality conspire to produce emergent phases, anomalous metallic states, and exotic vortex physics. We study these effects in atomically thin van der [&hellip;]<\/p>\n","protected":false},"author":1,"featured_media":3808,"comment_status":"open","ping_status":"open","sticky":false,"template":"","format":"standard","meta":{"footnotes":""},"categories":[41],"tags":[],"class_list":["post-3807","post","type-post","status-publish","format-standard","has-post-thumbnail","hentry","category-research"],"_links":{"self":[{"href":"https:\/\/physics.iisc.ac.in\/~aveek_bid\/wp-json\/wp\/v2\/posts\/3807","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/physics.iisc.ac.in\/~aveek_bid\/wp-json\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/physics.iisc.ac.in\/~aveek_bid\/wp-json\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/physics.iisc.ac.in\/~aveek_bid\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/physics.iisc.ac.in\/~aveek_bid\/wp-json\/wp\/v2\/comments?post=3807"}],"version-history":[{"count":21,"href":"https:\/\/physics.iisc.ac.in\/~aveek_bid\/wp-json\/wp\/v2\/posts\/3807\/revisions"}],"predecessor-version":[{"id":4965,"href":"https:\/\/physics.iisc.ac.in\/~aveek_bid\/wp-json\/wp\/v2\/posts\/3807\/revisions\/4965"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/physics.iisc.ac.in\/~aveek_bid\/wp-json\/wp\/v2\/media\/3808"}],"wp:attachment":[{"href":"https:\/\/physics.iisc.ac.in\/~aveek_bid\/wp-json\/wp\/v2\/media?parent=3807"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/physics.iisc.ac.in\/~aveek_bid\/wp-json\/wp\/v2\/categories?post=3807"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/physics.iisc.ac.in\/~aveek_bid\/wp-json\/wp\/v2\/tags?post=3807"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}