{"id":22,"date":"2012-09-05T11:22:33","date_gmt":"2012-09-05T15:22:33","guid":{"rendered":"https:\/\/people.clas.ufl.edu\/template\/?page_id=22"},"modified":"2026-03-20T11:05:53","modified_gmt":"2026-03-20T15:05:53","slug":"research","status":"publish","type":"page","link":"https:\/\/people.clas.ufl.edu\/dlaroc10\/research\/","title":{"rendered":"Research"},"content":{"rendered":"<nav class=\"is-responsive wp-block-navigation is-layout-flex wp-block-navigation-is-layout-flex\" \n\t\t data-wp-interactive=\"core\/navigation\" data-wp-context='{\"overlayOpenedBy\":{\"click\":false,\"hover\":false,\"focus\":false},\"type\":\"overlay\",\"roleAttribute\":\"\",\"ariaLabel\":\"Menu\"}'><button aria-haspopup=\"dialog\" aria-label=\"Open menu\" class=\"wp-block-navigation__responsive-container-open\" \n\t\t\t\tdata-wp-on--click=\"actions.openMenuOnClick\"\n\t\t\t\tdata-wp-on--keydown=\"actions.handleMenuKeydown\"\n\t\t\t><svg width=\"24\" height=\"24\" xmlns=\"http:\/\/www.w3.org\/2000\/svg\" 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data-wp-context=\"{ &quot;submenuOpenedBy&quot;: { &quot;click&quot;: false, &quot;hover&quot;: false, &quot;focus&quot;: false }, &quot;type&quot;: &quot;submenu&quot;, &quot;modal&quot;: null, &quot;previousFocus&quot;: null }\" data-wp-interactive=\"core\/navigation\" data-wp-on--focusout=\"actions.handleMenuFocusout\" data-wp-on--keydown=\"actions.handleMenuKeydown\" data-wp-on--mouseenter=\"actions.openMenuOnHover\" data-wp-on--mouseleave=\"actions.closeMenuOnHover\" data-wp-watch=\"callbacks.initMenu\" tabindex=\"-1\" class=\"wp-block-navigation-item has-child open-on-hover-click  menu-item menu-item-type-post_type menu-item-object-page wp-block-navigation-submenu\"><a class=\"wp-block-navigation-item__content\" href=\"https:\/\/people.clas.ufl.edu\/dlaroc10\/research\/\" title=\"\"><span class=\"wp-block-navigation-item__label\">Research<\/span><\/a><button data-wp-bind--aria-expanded=\"state.isMenuOpen\" data-wp-on--click=\"actions.toggleMenuOnClick\" aria-label=\"Research submenu\" class=\"wp-block-navigation__submenu-icon wp-block-navigation-submenu__toggle\" ><svg xmlns=\"http:\/\/www.w3.org\/2000\/svg\" width=\"12\" height=\"12\" viewBox=\"0 0 12 12\" fill=\"none\" aria-hidden=\"true\" focusable=\"false\"><path d=\"M1.50002 4L6.00002 8L10.5 4\" stroke-width=\"1.5\"><\/path><\/svg><\/button><ul data-wp-on--focus=\"actions.openMenuOnFocus\" class=\"wp-block-navigation__submenu-container  menu-item menu-item-type-post_type menu-item-object-page wp-block-navigation-submenu\"><li class=\" wp-block-navigation-item  menu-item menu-item-type-post_type menu-item-object-page wp-block-navigation-link\"><a class=\"wp-block-navigation-item__content\"  href=\"https:\/\/people.clas.ufl.edu\/dlaroc10\/research\/equipment-and-ressources\/\" title=\"\"><span class=\"wp-block-navigation-item__label\">Equipment and resources<\/span><\/a><\/li><\/ul><\/li><li class=\" wp-block-navigation-item  menu-item menu-item-type-post_type menu-item-object-page wp-block-navigation-link\"><a class=\"wp-block-navigation-item__content\"  href=\"https:\/\/people.clas.ufl.edu\/dlaroc10\/publications\/\" title=\"\"><span class=\"wp-block-navigation-item__label\">Publications<\/span><\/a><\/li><li class=\" wp-block-navigation-item  menu-item menu-item-type-post_type menu-item-object-page wp-block-navigation-link\"><a class=\"wp-block-navigation-item__content\"  href=\"https:\/\/people.clas.ufl.edu\/dlaroc10\/members\/\" title=\"\"><span class=\"wp-block-navigation-item__label\">Members<\/span><\/a><\/li><li class=\" wp-block-navigation-item  menu-item menu-item-type-post_type menu-item-object-page wp-block-navigation-link\"><a class=\"wp-block-navigation-item__content\"  href=\"https:\/\/people.clas.ufl.edu\/dlaroc10\/thesis\/\" title=\"\"><span class=\"wp-block-navigation-item__label\">Thesis<\/span><\/a><\/li><li class=\" wp-block-navigation-item  menu-item menu-item-type-post_type menu-item-object-page wp-block-navigation-link\"><a class=\"wp-block-navigation-item__content\"  href=\"https:\/\/people.clas.ufl.edu\/dlaroc10\/courses\/\" title=\"\"><span class=\"wp-block-navigation-item__label\">Courses taught<\/span><\/a><\/li><li class=\" wp-block-navigation-item  menu-item menu-item-type-post_type menu-item-object-page wp-block-navigation-link\"><a class=\"wp-block-navigation-item__content\"  href=\"https:\/\/people.clas.ufl.edu\/dlaroc10\/contact\/\" title=\"\"><span class=\"wp-block-navigation-item__label\">Contact<\/span><\/a><\/li><li class=\" wp-block-navigation-item  menu-item menu-item-type-post_type menu-item-object-page wp-block-navigation-link\"><a class=\"wp-block-navigation-item__content\"  href=\"https:\/\/people.clas.ufl.edu\/dlaroc10\/cv\/\" title=\"\"><span class=\"wp-block-navigation-item__label\">CV<\/span><\/a><\/li><\/ul>\n\t\t\t\t\t\t\t<\/div>\n\t\t\t\t\t\t<\/div>\n\t\t\t\t\t<\/div>\n\t\t\t\t<\/div><\/nav>\n\n\n<section class=\"fullwidth-text-block\"><div class=\"container px-0\"><div class=\"row align-items-start\"><div class=\"col-12\">\n<h1 class=\"wp-block-heading has-text-align-center\">Research<\/h1>\n\n\n\n<p style=\"font-size:23px\">In Laroche Lab, we specialize in designing and fabricating nano-structures to study the fascinating effects that arise when different materials and\/or devices are interacting at the nanoscale.&nbsp; Utilizing state-of-the-art material systems with low disorder such as GaAs\/AlGaAs heterostructures, InAs nanowires with an aluminium epilayer and InSb nanowires, we engineer coupled systems where novel phenomena occur, and attempt to harness their properties for future nano-electronics and quantum computing applications.&nbsp; The devices under study are characterized through electrical transport in a dilution refrigerator at ultra-low temperatures, in the range of a few tens of milikelvin, and in the presence of a magnetic field.<\/p>\n\n\n\n<h1 class=\"wp-block-heading\" style=\"font-size:40px\"><span style=\"text-decoration: underline\">Coulomb drag between coupled 1D systems<\/span><br><\/h1>\n\n\n\n<p style=\"font-size:23px\">Despite their conceptual simplicity, one-dimensional systems remain a challenge to understand owing to the enhanced correlations and interactions that occur due to&nbsp;their restricted phase-space.&nbsp; As such, the simple Fermi-liquid model describing the physics of solid-state electrons in 2D and 3D no longer holds in 1D, where electronic transport is instead described by the Luttinger-liquid model which accounts for these enhanced interactions.&nbsp; Experimentally studying the intrinsic properties of 1D systems is also a challenging task.&nbsp; Standard measurements generally probe processes occurring in the high dimensional system leads, thereby providing no information about the nature of electron-electron interactions inside the 1D system itself.&nbsp; In contrast, experiments in coupled 1D systems, such as Coulomb drag, effectively probe electron-electron interactions.&nbsp; By using dual side processing on GaAs\/AlGaAs bilayer systems, two independently contacted quantum wires can be fabricated such that they are less than 15 nm apart.<\/p>\n\n\n\n<h3 class=\"wp-block-heading\"><div id=\"metaslider-id-294\" style=\"width: 100%;\" class=\"ml-slider-3-106-0 metaslider metaslider-flex metaslider-294 ml-slider has-dots-nav ms-theme-simply-dark\" role=\"region\" aria-label=\"New Slideshow\" data-height=\"300\" data-width=\"700\">\n    <div id=\"metaslider_container_294\">\n        <div id=\"metaslider_294\">\n            <ul aria-live='off' class='slides'>\n                <li style=\"display: block; width: 100%;\" class=\"slide-298 ms-image \" aria-roledescription=\"slide\" data-date=\"2025-04-24 15:47:50\" data-filename=\"Ebase1-498x213.png\" data-slide-type=\"image\"><img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/people.clas.ufl.edu\/dlaroc10\/files\/Ebase1-498x213.png\" height=\"300\" width=\"700\" alt=\"First fabrication step: Ohmic contacts and top gates are defined on top of the device\" class=\"slider-294 slide-298 msDefaultImage\" title=\"First fabrication step\" \/><div class=\"caption-wrap\"><div class=\"caption\">First fabrication step<\/div><\/div><\/li>\n                <li style=\"display: none; width: 100%;\" class=\"slide-297 ms-image \" aria-roledescription=\"slide\" data-date=\"2025-04-24 15:47:49\" data-filename=\"Ebase2-501x214.png\" data-slide-type=\"image\"><img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/people.clas.ufl.edu\/dlaroc10\/files\/Ebase2-501x214.png\" height=\"300\" width=\"700\" alt=\"Second fabrication step: A host substrate is epoxied over the device\" class=\"slider-294 slide-297 msDefaultImage\" title=\"Second fabrication step\" \/><div class=\"caption-wrap\"><div class=\"caption\">Second fabrication step<\/div><\/div><\/li>\n                <li style=\"display: none; width: 100%;\" class=\"slide-296 ms-image \" aria-roledescription=\"slide\" data-date=\"2025-04-24 15:47:49\" data-filename=\"Ebase3-503x215.png\" data-slide-type=\"image\"><img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/people.clas.ufl.edu\/dlaroc10\/files\/Ebase3-503x215.png\" height=\"300\" width=\"700\" alt=\"Third fabrication step: The device is flipped and the original substrate is mechanically lapped and chemically etched up until the stop-etch layer\" class=\"slider-294 slide-296 msDefaultImage\" title=\"Third fabrication step\" \/><div class=\"caption-wrap\"><div class=\"caption\">Third fabrication step<\/div><\/div><\/li>\n                <li style=\"display: none; width: 100%;\" class=\"slide-295 ms-image \" aria-roledescription=\"slide\" data-date=\"2025-04-24 15:47:49\" data-filename=\"Ebase4-498x213.png\" data-slide-type=\"image\"><img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/people.clas.ufl.edu\/dlaroc10\/files\/Ebase4-498x213.png\" height=\"300\" width=\"700\" alt=\"Final fabrication step: New gates are deposited on top of the device and aligned with the bottom gates\" class=\"slider-294 slide-295 msDefaultImage\" title=\"Final fabrication step\" \/><div class=\"caption-wrap\"><div class=\"caption\">Final fabrication step<\/div><\/div><\/li>\n            <\/ul>\n        <\/div>\n        \n    <\/div>\n<\/div><\/h3>\n\n\n\n<p style=\"font-size:23px\">We will use this platform, to perform Coulomb drag measurements, where a current in a quantum wire induces a voltage drop in the adjacent wire solely through Coulomb interactions.&nbsp; By measuring the dependence of the drag signal as a function of temperature, 1D density, magnetic field, geometry and material parameters, we will extract crucial information about the nature of Luttinger-liquids and about the strength of electron-electron interactions in a 1D systems.<\/p>\n\n\n<div class=\"wp-block-image\">\n<figure class=\"alignleft size-medium is-resized\"><a href=\"http:\/\/people.clas.ufl.edu\/dlaroc10\/files\/C-drag-1.png\"><img loading=\"lazy\" decoding=\"async\" width=\"300\" height=\"151\" src=\"http:\/\/people.clas.ufl.edu\/dlaroc10\/files\/C-drag-1-300x151.png\" alt=\"Schematic of a reciprocal Coulomb drag measurement. A current in the bottom wire induces an electron accumulation in the drag wire, hereby generating a drag voltage\" class=\"wp-image-410\" style=\"aspect-ratio:1.9868583524431116;width:492px;height:auto\" srcset=\"https:\/\/people.clas.ufl.edu\/dlaroc10\/files\/C-drag-1-300x151.png 300w, https:\/\/people.clas.ufl.edu\/dlaroc10\/files\/C-drag-1-1024x516.png 1024w, https:\/\/people.clas.ufl.edu\/dlaroc10\/files\/C-drag-1-768x387.png 768w, https:\/\/people.clas.ufl.edu\/dlaroc10\/files\/C-drag-1-1536x775.png 1536w, https:\/\/people.clas.ufl.edu\/dlaroc10\/files\/C-drag-1.png 1733w\" sizes=\"auto, (max-width: 300px) 100vw, 300px\" \/><\/a><figcaption class=\"wp-element-caption\">Schematic of a reciprocal Coulomb drag measurement. A current in the bottom wire induces an electron accumulation in the drag wire, hereby generating a drag voltage<\/figcaption><\/figure>\n<\/div>\n\n<div class=\"wp-block-image\">\n<figure class=\"alignright size-medium is-resized\"><img loading=\"lazy\" decoding=\"async\" width=\"300\" height=\"232\" src=\"http:\/\/people.clas.ufl.edu\/dlaroc10\/files\/Tunable-drag-300x232.png\" alt=\"Relative strength of reciprocal and non-reciprocal Coulomb drag as a function of gate voltage (x-axis) and temperature (y-axis). The gate voltage ranges between -0.3V and -0.35V, while temperature ranges from 3 Kelvin to 10 mK. Below 500 mK, the non-reciprocal drag signal dominates (ratio larger than 2) over most of the gate voltages, with a few small regions in gate voltage where reciprocal signal dominates. Between 400 mK and 750 mk, the contribution from non-reciprocal drag decreases and, above 750 mK, the drag is predominantly dominated by a reciprocal signal (ration lower than 0.3). Above 2K, the drag signal becomes small, leading to a majoritarely noise-dominated signal (ratio of 1).\" class=\"wp-image-318\" style=\"aspect-ratio:1.2931905435441504;width:398px;height:auto\" srcset=\"https:\/\/people.clas.ufl.edu\/dlaroc10\/files\/Tunable-drag-300x232.png 300w, https:\/\/people.clas.ufl.edu\/dlaroc10\/files\/Tunable-drag-1024x793.png 1024w, https:\/\/people.clas.ufl.edu\/dlaroc10\/files\/Tunable-drag-768x595.png 768w, https:\/\/people.clas.ufl.edu\/dlaroc10\/files\/Tunable-drag-1536x1190.png 1536w, https:\/\/people.clas.ufl.edu\/dlaroc10\/files\/Tunable-drag-2048x1586.png 2048w, https:\/\/people.clas.ufl.edu\/dlaroc10\/files\/Tunable-drag-200x155.png 200w\" sizes=\"auto, (max-width: 300px) 100vw, 300px\" \/><figcaption class=\"wp-element-caption\">Tunable contribution from reciprocal (yellow) and non-reciprocal (blue) Coulomb drag [1]. At low temperatures, the non-reciprocal generally dominates while reciprocal signal dominates at high temperatures<\/figcaption><\/figure>\n<\/div>\n\n\n<div style=\"height:100px\" aria-hidden=\"true\" class=\"wp-block-spacer\"><\/div>\n\n\n\n<h2 class=\"wp-block-heading\" style=\"font-size:40px\"><span style=\"text-decoration: underline\">Current research efforts<\/span> :<\/h2>\n\n\n\n<p style=\"font-size:23px\">Recently, we have measured an unexpected non-reciprocal Coulomb drag signal, both in laterally-coupled and vertically-coupled quantum wires.&nbsp; This signal was identified by measuring Coulomb drag using two opposite current directions. Combining both measurements together, the reciprocal signal is identified with the anti-symmetric component while the non-reciprocal signal is identified with the symmetric component. Further studies showed that the relative strength of both contributions is tunable with both temperature and wire width. Currently, we are studying the evolution of both signal as a function of interwire separation, magnetic field and disorder. We are also trying to explain why both contributions vary differently as a function of temperature.<\/p>\n\n\n\n<h3 class=\"wp-block-heading\"><span style=\"text-decoration: underline\">Relevant publications<\/span> :<\/h3>\n\n\n\n<ol class=\"wp-block-list\">\n<li><a href=\"https:\/\/journals.aps.org\/prb\/accepted\/10.1103\/5yqq-cw73\">Quasi-one-dimensional Coulomb drag between spin-polarized quantum wires<\/a>,<br>M. Zheng, R. Makaju, R.Gazizulin, A. Levchenko, S. J. Addamane, D. Laroche, Phys. Rev. B [accepted]<\/li>\n\n\n\n<li><a href=\"https:\/\/www.nature.com\/articles\/s41467-025-62324-6\"><span style=\"text-decoration: underline\">Tunable reciprocal and nonreciprocal contributions to 1D Coulomb Drag.<\/span><\/a><br>M. Zheng, R. Makaju, R.Gazizulin, S. J. Addamane, D. Laroche, Nature Communications volume 16, 6963 (2025).<\/li>\n\n\n\n<li><a href=\"https:\/\/journals.aps.org\/prl\/abstract\/10.1103\/v3dn-bnrp\">Quasi-1D Coulomb Drag in the Nonlinear Regime<\/a><br>M. Zheng, R. Makaju, R.Gazizulin, A. Levchenko, S. J. Addamane, D. Laroche, Phys. Rev. Lett 134, 236301 (2025).<\/li>\n\n\n\n<li><a href=\"https:\/\/journals.aps.org\/prb\/abstract\/10.1103\/PhysRevB.109.085101\"><span style=\"text-decoration: underline\">Nonreciprocal Coulomb drag between quantum wires in the quasi-one-dimensional regime.<\/span><\/a><br>R. Makaju, H. Kassar, S. M. Daloglu, A. Huynh, D. Laroche, A. Levchenko, and S. J. Addamane , Phys. Rev. B 109, 085101 (2024).<\/li>\n\n\n\n<li><a href=\"https:\/\/www.science.org\/doi\/full\/10.1126\/science.1244152?explicitversion=true\"><span style=\"text-decoration: underline\">1D-1D Coulomb Drag Signature of a Luttinger Liquid<\/span>.<\/a><br>D. Laroche, G. Gervais, M. P. Lilly and J. L. Reno, <em>Science<\/em>,&nbsp;<strong>343<\/strong>, 631 (2014).<\/li>\n\n\n\n<li><a href=\"https:\/\/www.nature.com\/articles\/nnano.2011.182\"><span style=\"text-decoration: underline\">Positive and Negative Coulomb Drag in Vertically Integrated One-Dimensional Quantum Wires<\/span>.&nbsp;&nbsp;<\/a><br>D. Laroche, G. Gervais, M. P. Lilly and J. L. Reno,&nbsp;<em>Nature Nanotechnolgy<\/em>,&nbsp;<strong>6<\/strong>, 793 (2011).<br><\/li>\n<\/ol>\n\n\n\n<hr class=\"wp-block-separator has-alpha-channel-opacity\"\/>\n\n\n\n<h1 class=\"wp-block-heading\" style=\"font-size:40px\"><span style=\"text-decoration: underline\">Majorana zero modes in hybrid superconductor-semiconductor devices<\/span><br><\/h1>\n\n\n\n<p style=\"font-size:23px\">Topological quantum computations offer a promising approach to fault-tolerant quantum computing by encoding and manipulating the quantum information non-locally in a non-Abelian degenerate ground state that is intrinsically immune against disorder.&nbsp; Majorana-Zero-Modes (MZMs) in nanowires with induced superconductivity and strong spin-orbit coupling under a magnetic field are arguably the front-runner in establishing topological quantum bits, with numerous signatures of MZMs having been experimentally observed.&nbsp; In Laroche lab, we will use novel techniques to further measure the properties of these promising systems.<\/p>\n\n\n\n<p style=\"font-size:23px\">In addition, we will work towards developing a novel platform for the observation of MZMs, or their fractional counter-part the parafermions, in the absence of an applied magnetic field.&nbsp; The material of choice for this platform is hybrid superconductor-semiconductor nanowire pairs coupled to a common superconductor.&nbsp; By designing nanowire networks with sufficiently large electron-electron interactions, induced proximity can arise through crossed-Andreev reflections, which will naturally give rise to MZMs or parafermions, even without an applied magnetic field.<\/p>\n\n\n<div class=\"wp-block-image\">\n<figure class=\"aligncenter size-medium\"><img loading=\"lazy\" decoding=\"async\" width=\"300\" height=\"184\" src=\"http:\/\/people.clas.ufl.edu\/dlaroc10\/files\/Crossed-AR-300x184.jpg\" alt=\"Schematic of crossed-Andreev reflections. Two nano-wires are deposted on the same s-wave superconductor. When an electron is incident on one of the wire, it emits a hole in the opposite wire. A Cooper pair is thus formed across two wires rather than in a single one.\" class=\"wp-image-217\" srcset=\"https:\/\/people.clas.ufl.edu\/dlaroc10\/files\/Crossed-AR-300x184.jpg 300w, https:\/\/people.clas.ufl.edu\/dlaroc10\/files\/Crossed-AR-342x210.jpg 342w, https:\/\/people.clas.ufl.edu\/dlaroc10\/files\/Crossed-AR.jpg 650w\" sizes=\"auto, (max-width: 300px) 100vw, 300px\" \/><figcaption class=\"wp-element-caption\">Schematic of crossed-Andreev reflections: a Cooper pair is formed across two wires rather than in a single one.<\/figcaption><\/figure>\n<\/div>\n\n\n<h2 class=\"wp-block-heading\" style=\"font-size:40px\"><span style=\"text-decoration: underline\">Current research efforts<\/span> :<\/h2>\n\n\n\n<p style=\"font-size:23px\">Our current efforts have shifted towards the fabrication of laterally coupled quantum wires in InAs heterostructures to measure Coulomb drag in this novel material platform and determine the impact of spin-orbit coupling on the drag measurements. Measuring Coulomb drag once a parent superconductor has been deposited on the wires to determine the strength of electron-electron interactions is the following step.<\/p>\n\n\n\n<h3 class=\"wp-block-heading\"><span style=\"text-decoration: underline\">Relevant publications:<\/span><\/h3>\n\n\n\n<p><a href=\"https:\/\/www.nature.com\/articles\/s41467-018-08161-2\"><span style=\"text-decoration: underline\">Observation of the 4\u03c0-periodic Josephson effect in InAs nanowires.<\/span>&nbsp;<\/a><br> D. Laroche, D. Bouman, D. J. van Woerkom, A. Proutski, C. Murthy, D. I. Pikulin, C. Nayak, R. J. J. van Gulik, J., Nyg\u00e5rd, P. Krogstrup, L. P. Kouwenhoven, A. Geresdi.&nbsp;<em>Nature Communications<\/em>&nbsp;<strong>10<\/strong>, 245 (2019).<br><\/p>\n\n\n\n<hr class=\"wp-block-separator has-alpha-channel-opacity\"\/>\n\n\n\n<h1 class=\"wp-block-heading\" style=\"font-size:40px\"><span style=\"text-decoration: underline\">Exotic phenomena in coupled SiGe-based bilayers<\/span><br><\/h1>\n\n\n\n<p style=\"font-size:23px\">Si\/SiGe and Ge\/SiGe heterostructures have been showing great promises in the recent year.&nbsp; Their nearly defect free growth, significant spin-orbit interaction and the possibility to induce superconductivity make these structures a promising platform both for fundamental research and quantum computing applications.&nbsp; Utilizing the expertise developed in GaAs\/AlGaAs bilayer systems, we will engineer devices where the density and the electronic confinement of Ge\/SiGe bilayers can be controlled simultaneously from both side.&nbsp; This will open up exciting research opportunities in the field of vertically coupled wires and bilayer exciton condensation. Recent experiments showed a quantum state at \u03bd_total = 1 that is consistent with the onset of exciton condensation. <\/p>\n\n\n<div class=\"wp-block-image\">\n<figure class=\"alignleft size-medium is-resized\"><img loading=\"lazy\" decoding=\"async\" width=\"300\" height=\"221\" src=\"http:\/\/people.clas.ufl.edu\/dlaroc10\/files\/Exciton-300x221.png\" alt=\"Comparison between simulated tunnel-induced quantum Hall gap (blue) and the experimentally measured one (green). The x-axis is the electron density and the y-axis is the SAS gap. Simulations predict a monotonically decreasing activation gap with energy around 0.5 K. The observed data is inconsistent with a tunnel-induced quantum Hall energy gap as it increases between 10x10^10 and 15x10^15 electrons \/ cm^-2 from 1k to 2.2 K, before slightly decreasing at larger densities.\" class=\"wp-image-313\" style=\"aspect-ratio:1.35756204482783;width:481px;height:auto\" srcset=\"https:\/\/people.clas.ufl.edu\/dlaroc10\/files\/Exciton-300x221.png 300w, https:\/\/people.clas.ufl.edu\/dlaroc10\/files\/Exciton-1024x756.png 1024w, https:\/\/people.clas.ufl.edu\/dlaroc10\/files\/Exciton-768x567.png 768w, https:\/\/people.clas.ufl.edu\/dlaroc10\/files\/Exciton-1536x1134.png 1536w, https:\/\/people.clas.ufl.edu\/dlaroc10\/files\/Exciton-200x148.png 200w, https:\/\/people.clas.ufl.edu\/dlaroc10\/files\/Exciton.png 1689w\" sizes=\"auto, (max-width: 300px) 100vw, 300px\" \/><figcaption class=\"wp-element-caption\">Comparison between simulated tunnel-induced quantum Hall gap (blue) and the experimentally measured one (green). The observed data is inconsistent with a tunnel-induced quantum Hall energy gap.<\/figcaption><\/figure>\n<\/div>\n\n<div class=\"wp-block-image\">\n<figure class=\"alignright size-medium is-resized\"><img loading=\"lazy\" decoding=\"async\" width=\"300\" height=\"178\" src=\"http:\/\/people.clas.ufl.edu\/dlaroc10\/files\/SiGe_2well-300x178.png\" alt=\"TEM picture of a Si\/SiGe\/Si double quantum well heterostructure. Dark spacers are located at the top and bottom of the structure. A 19.7 nm wide bottom quantum well and a 5.7 nm wide top quantum well separated by a darker 2nm barrier are clearly visible.\" class=\"wp-image-232\" style=\"aspect-ratio:1.6855412167500659;width:522px;height:auto\" srcset=\"https:\/\/people.clas.ufl.edu\/dlaroc10\/files\/SiGe_2well-300x178.png 300w, https:\/\/people.clas.ufl.edu\/dlaroc10\/files\/SiGe_2well-354x210.png 354w, https:\/\/people.clas.ufl.edu\/dlaroc10\/files\/SiGe_2well.png 674w\" sizes=\"auto, (max-width: 300px) 100vw, 300px\" \/><figcaption class=\"wp-element-caption\">TEM picture of a Si\/SiGe\/Si double quantum well heterostructure.<\/figcaption><\/figure>\n<\/div>\n\n\n<div style=\"height:31px\" aria-hidden=\"true\" class=\"wp-block-spacer\"><\/div>\n\n\n\n<h2 class=\"wp-block-heading\" style=\"font-size:40px\"><span style=\"text-decoration: underline\">Current research efforts<\/span> :<\/h2>\n\n\n\n<p style=\"font-size:23px\">We recently successfully achieve a device compatible with independent contact to each layer. Current efforts involve characterizing valley splitting in Si\/SiGe bilayers, and in measuring signature of exciton condensation with the novel devices in Ge\/SiGe bilayers.<\/p>\n\n\n\n<h3 class=\"wp-block-heading\">Relevant publications :<\/h3>\n\n\n\n<ol class=\"wp-block-list\">\n<li><a href=\"https:\/\/pubs.aip.org\/aip\/apl\/article\/119\/22\/223103\/40958\/Density-dependence-of-the-excitation-gaps-in-an\"><span style=\"text-decoration: underline\">Density dependence of the excitation gaps in an undoped Si\/SiGe double-quantum-well heterostructure.<\/span><\/a><br>D. Chen, S. Cai, N.-W. Hsu, S.-H. Huang, Y. Chuang, E. Nielsen, J.-Y. Li, C. W. Liu, T. M. Lu and D. Laroche Appl. Phys. Lett. 119, 223103 (2021).<\/li>\n\n\n\n<li><a href=\"https:\/\/pubs.aip.org\/aip\/apl\/article\/106\/14\/143503\/27277\/Magneto-transport-of-an-electron-bilayer-system-in\"><span style=\"text-decoration: underline\">Magneto-transport of an electron bilayer system in an undoped Si\/SiGe double-quantum-well heterostructure.<\/span>&nbsp;<\/a><br>D. Laroche, S.-H. Huang, E. Nielsen, C. W. Liu, J.-Y. Li and T. M. Lu,&nbsp;<em>Applied Physics Letters<\/em>,&nbsp;<strong>106<\/strong>, 143503 (2015).<\/li>\n<\/ol>\n<\/div><\/div><\/div><\/section>\n","protected":false},"excerpt":{"rendered":"","protected":false},"author":1026,"featured_media":0,"parent":0,"menu_order":2,"comment_status":"closed","ping_status":"closed","template":"","meta":{"_acf_changed":false,"featured_post":"","footnotes":"","_links_to":"","_links_to_target":""},"class_list":["post-22","page","type-page","status-publish","hentry"],"acf":[],"_links":{"self":[{"href":"https:\/\/people.clas.ufl.edu\/dlaroc10\/wp-json\/wp\/v2\/pages\/22","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/people.clas.ufl.edu\/dlaroc10\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/people.clas.ufl.edu\/dlaroc10\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/people.clas.ufl.edu\/dlaroc10\/wp-json\/wp\/v2\/users\/1026"}],"replies":[{"embeddable":true,"href":"https:\/\/people.clas.ufl.edu\/dlaroc10\/wp-json\/wp\/v2\/comments?post=22"}],"version-history":[{"count":10,"href":"https:\/\/people.clas.ufl.edu\/dlaroc10\/wp-json\/wp\/v2\/pages\/22\/revisions"}],"predecessor-version":[{"id":431,"href":"https:\/\/people.clas.ufl.edu\/dlaroc10\/wp-json\/wp\/v2\/pages\/22\/revisions\/431"}],"wp:attachment":[{"href":"https:\/\/people.clas.ufl.edu\/dlaroc10\/wp-json\/wp\/v2\/media?parent=22"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}