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</div> <div class="control"> <button class="button is-small is-link">Go</button> </div> </div> </form> </div> </div> <ol class="breathe-horizontal" start="1"> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2401.09549">arXiv:2401.09549</a> <span> [<a href="https://arxiv.org/pdf/2401.09549">pdf</a>, <a href="https://arxiv.org/format/2401.09549">other</a>] </span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Mesoscale and Nanoscale Physics">cond-mat.mes-hall</span> </div> </div> <p class="title is-5 mathjax"> Interferometric Single-Shot Parity Measurement in an InAs-Al Hybrid Device </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/cond-mat?searchtype=author&query=Aghaee%2C+M">Morteza Aghaee</a>, <a href="/search/cond-mat?searchtype=author&query=Ramirez%2C+A+A">Alejandro Alcaraz Ramirez</a>, <a href="/search/cond-mat?searchtype=author&query=Alam%2C+Z">Zulfi Alam</a>, <a href="/search/cond-mat?searchtype=author&query=Ali%2C+R">Rizwan Ali</a>, <a href="/search/cond-mat?searchtype=author&query=Andrzejczuk%2C+M">Mariusz Andrzejczuk</a>, <a href="/search/cond-mat?searchtype=author&query=Antipov%2C+A">Andrey Antipov</a>, <a href="/search/cond-mat?searchtype=author&query=Astafev%2C+M">Mikhail Astafev</a>, <a href="/search/cond-mat?searchtype=author&query=Barzegar%2C+A">Amin Barzegar</a>, <a href="/search/cond-mat?searchtype=author&query=Bauer%2C+B">Bela Bauer</a>, <a href="/search/cond-mat?searchtype=author&query=Becker%2C+J">Jonathan Becker</a>, <a href="/search/cond-mat?searchtype=author&query=Bhaskar%2C+U+K">Umesh Kumar Bhaskar</a>, <a href="/search/cond-mat?searchtype=author&query=Bocharov%2C+A">Alex Bocharov</a>, <a href="/search/cond-mat?searchtype=author&query=Boddapati%2C+S">Srini Boddapati</a>, <a href="/search/cond-mat?searchtype=author&query=Bohn%2C+D">David Bohn</a>, <a href="/search/cond-mat?searchtype=author&query=Bommer%2C+J">Jouri Bommer</a>, <a href="/search/cond-mat?searchtype=author&query=Bourdet%2C+L">Leo Bourdet</a>, <a href="/search/cond-mat?searchtype=author&query=Bousquet%2C+A">Arnaud Bousquet</a>, <a href="/search/cond-mat?searchtype=author&query=Boutin%2C+S">Samuel Boutin</a>, <a href="/search/cond-mat?searchtype=author&query=Casparis%2C+L">Lucas Casparis</a>, <a href="/search/cond-mat?searchtype=author&query=Chapman%2C+B+J">Benjamin James Chapman</a>, <a href="/search/cond-mat?searchtype=author&query=Chatoor%2C+S">Sohail Chatoor</a>, <a href="/search/cond-mat?searchtype=author&query=Christensen%2C+A+W">Anna Wulff Christensen</a>, <a href="/search/cond-mat?searchtype=author&query=Chua%2C+C">Cassandra Chua</a>, <a href="/search/cond-mat?searchtype=author&query=Codd%2C+P">Patrick Codd</a>, <a href="/search/cond-mat?searchtype=author&query=Cole%2C+W">William Cole</a> , et al. (137 additional authors not shown) </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2401.09549v4-abstract-short" style="display: inline;"> The fusion of non-Abelian anyons or topological defects is a fundamental operation in measurement-only topological quantum computation. In topological superconductors, this operation amounts to a determination of the shared fermion parity of Majorana zero modes. As a step towards this, we implement a single-shot interferometric measurement of fermion parity in indium arsenide-aluminum heterostruct… <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2401.09549v4-abstract-full').style.display = 'inline'; document.getElementById('2401.09549v4-abstract-short').style.display = 'none';">▽ More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2401.09549v4-abstract-full" style="display: none;"> The fusion of non-Abelian anyons or topological defects is a fundamental operation in measurement-only topological quantum computation. In topological superconductors, this operation amounts to a determination of the shared fermion parity of Majorana zero modes. As a step towards this, we implement a single-shot interferometric measurement of fermion parity in indium arsenide-aluminum heterostructures with a gate-defined nanowire. The interferometer is formed by tunnel-coupling the proximitized nanowire to quantum dots. The nanowire causes a state-dependent shift of these quantum dots' quantum capacitance of up to 1 fF. Our quantum capacitance measurements show flux h/2e-periodic bimodality with a signal-to-noise ratio of 1 in 3.7 $渭$s at optimal flux values. From the time traces of the quantum capacitance measurements, we extract a dwell time in the two associated states that is longer than 1 ms at in-plane magnetic fields of approximately 2 T. These results are consistent with a measurement of the fermion parity encoded in a pair of Majorana zero modes that are separated by approximately 3 $渭$m and subjected to a low rate of poisoning by non-equilibrium quasiparticles. The large capacitance shift and long poisoning time enable a parity measurement error probability of 1%. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2401.09549v4-abstract-full').style.display = 'none'; document.getElementById('2401.09549v4-abstract-short').style.display = 'inline';">△ Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 2 April, 2024; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 17 January, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> January 2024. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Comments:</span> <span class="has-text-grey-dark mathjax">Added data on a second measurement of device A and a measurement of device B, expanded discussion of a trivial scenario. Refs added, author list updated</span> </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2001.05221">arXiv:2001.05221</a> <span> [<a href="https://arxiv.org/pdf/2001.05221">pdf</a>] </span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Applied Physics">physics.app-ph</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Materials Science">cond-mat.mtrl-sci</span> </div> <div class="is-inline-block" style="margin-left: 0.5rem"> <div class="tags has-addons"> <span class="tag is-dark is-size-7">doi</span> <span class="tag is-light is-size-7"><a class="" href="https://doi.org/10.1063/1.5125751">10.1063/1.5125751 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Backward volume vs Damon-Eshbach: a travelling spin wave spectroscopy comparison </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/cond-mat?searchtype=author&query=Bhaskar%2C+U+K">U. K. Bhaskar</a>, <a href="/search/cond-mat?searchtype=author&query=Talmelli%2C+G">G. Talmelli</a>, <a href="/search/cond-mat?searchtype=author&query=Ciubotaru%2C+F">F. Ciubotaru</a>, <a href="/search/cond-mat?searchtype=author&query=Adelmann%2C+C">C. Adelmann</a>, <a href="/search/cond-mat?searchtype=author&query=Devolder%2C+T">T. Devolder</a> </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="2001.05221v2-abstract-short" style="display: inline;"> We compare the characteristics of electrically transduced Damon-Eshbach (DESWs) and backward volume (BVSWs) configurations within the same, 30 nm thick, ferromagnetic, CoFeB waveguide. Sub-micron U-shaped antennas are used to deliver the necessary in-plane and out-of-plane RF fields. We measure the spin-wave transmission with respect to in-plane field orientation, frequency and propagation distanc… <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2001.05221v2-abstract-full').style.display = 'inline'; document.getElementById('2001.05221v2-abstract-short').style.display = 'none';">▽ More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2001.05221v2-abstract-full" style="display: none;"> We compare the characteristics of electrically transduced Damon-Eshbach (DESWs) and backward volume (BVSWs) configurations within the same, 30 nm thick, ferromagnetic, CoFeB waveguide. Sub-micron U-shaped antennas are used to deliver the necessary in-plane and out-of-plane RF fields. We measure the spin-wave transmission with respect to in-plane field orientation, frequency and propagation distance. Unlike DESW, BVSWs are reciprocally transduced and collected for either direction of propagation, but their ability to transport energy is lower than DESWs for two reasons. This arises first because BVSW are inductively transduced less efficiently than DESWs. Also, in the range of wavevectors (~5 rad. um-1) typically excited by our antennas, the group velocity of BVSWs stays lower than that of DESW, which leads to reduced propagation ability that impact transmission signals in an exponential manner. In contrast, the group velocity of DESWs is maximum at low fields and decreases continuously with the applied field. The essential features of the measured SW characteristics are well reciprocated by a simple, 1-D analytical model which can be used to assess the potential of each configuration. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2001.05221v2-abstract-full').style.display = 'none'; document.getElementById('2001.05221v2-abstract-short').style.display = 'inline';">△ Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 3 June, 2021; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 15 January, 2020; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> January 2020. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Comments:</span> <span class="has-text-grey-dark mathjax">This work was funded through the FETOPEN-01-2016-2017-FET-Open research and innovation actions (CHIRON project: Grant Agreement No. 801055) and was partly supported by the French RENATECH network</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> Journal of Applied Physics 127, 033902 (2020) </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/1909.03702">arXiv:1909.03702</a> <span> [<a href="https://arxiv.org/pdf/1909.03702">pdf</a>] </span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Applied Physics">physics.app-ph</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Materials Science">cond-mat.mtrl-sci</span> </div> <div class="is-inline-block" style="margin-left: 0.5rem"> <div class="tags has-addons"> <span class="tag is-dark is-size-7">doi</span> <span class="tag is-light is-size-7"><a class="" href="https://doi.org/10.1109/TUFFC.2020.2967902">10.1109/TUFFC.2020.2967902 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> BPZT HBARs for bias-tunable, stress generation at GHz frequencies </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/cond-mat?searchtype=author&query=Bhaskar%2C+U+K">U. K. Bhaskar</a>, <a href="/search/cond-mat?searchtype=author&query=Tierno%2C+D">D. Tierno</a>, <a href="/search/cond-mat?searchtype=author&query=Talmelli%2C+G">G. Talmelli</a>, <a href="/search/cond-mat?searchtype=author&query=Ciubotaru%2C+F">F. Ciubotaru</a>, <a href="/search/cond-mat?searchtype=author&query=Adelmann%2C+C">C. Adelmann</a>, <a href="/search/cond-mat?searchtype=author&query=Devolder%2C+T">T. Devolder</a> </p> <p class="abstract mathjax"> <span class="has-text-black-bis has-text-weight-semibold">Abstract</span>: <span class="abstract-short has-text-grey-dark mathjax" id="1909.03702v2-abstract-short" style="display: inline;"> The high frequency performance of strong piezoelectric materials like PZT remains relatively less explored due to the assumption of large dielectric/ferroelectric losses at GHz frequencies. Recently, the advent of magnetoelectric technology as an on-chip route to excite magnetization dynamics has provided the impetus to evaluate the electromechanical performance of PZT at microwave frequencies. In… <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1909.03702v2-abstract-full').style.display = 'inline'; document.getElementById('1909.03702v2-abstract-short').style.display = 'none';">▽ More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="1909.03702v2-abstract-full" style="display: none;"> The high frequency performance of strong piezoelectric materials like PZT remains relatively less explored due to the assumption of large dielectric/ferroelectric losses at GHz frequencies. Recently, the advent of magnetoelectric technology as an on-chip route to excite magnetization dynamics has provided the impetus to evaluate the electromechanical performance of PZT at microwave frequencies. In this work, we demonstrate that HBARs fabricated using Barium-doped PZT (BPZT) films can efficiently generate acoustic waves up to 15 GHz. The ferroelectricity of BPZT endows added functionality to the resonator in the form of voltage tunability of the electromechanical performance. We extract the piezoelectric coefficient by numerically comparing the performance of BPZT with the Mason model. The extracted piezoelectric coefficient ~60 pm/V agrees well with reported values on thin film PZT measured at low frequencies (<100 MHz). Our results suggest that with further improvement in device design and material processing, BPZT resonators could operate as large amplitude, tunable stress transducers at GHz frequencies. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1909.03702v2-abstract-full').style.display = 'none'; document.getElementById('1909.03702v2-abstract-short').style.display = 'inline';">△ Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 3 June, 2021; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 9 September, 2019; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> September 2019. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Comments:</span> <span class="has-text-grey-dark mathjax">This work was funded through the FETOPEN-01-2016-2017-FET-Open research and innovation actions (CHIRON project: Grant Agreement No. 801055) and was partly supported by the French RENATECH network</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> IEEE Transactions on Ultrasonics, Ferroelectrics, and Frequency Control ( Volume: 67, Issue: 6, June 2020), Page(s): 1284 - 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