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name="order"><option selected value="-announced_date_first">Announcement date (newest first)</option><option value="announced_date_first">Announcement date (oldest first)</option><option value="-submitted_date">Submission date (newest first)</option><option value="submitted_date">Submission date (oldest first)</option><option value="">Relevance</option></select> </span> </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/2402.04175">arXiv:2402.04175</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2402.04175">pdf</a>, <a href="https://arxiv.org/format/2402.04175">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="High Energy Physics - Lattice">hep-lat</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Disordered Systems and Neural Networks">cond-mat.dis-nn</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Statistical Mechanics">cond-mat.stat-mech</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Computational Physics">physics.comp-ph</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Data Analysis, Statistics and Probability">physics.data-an</span> </div> </div> <p class="title is-5 mathjax"> Constrained curve fitting for semi-parametric models with radial basis function networks </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/cond-mat?searchtype=author&amp;query=Peterson%2C+C+T">Curtis Taylor Peterson</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Hasenfratz%2C+A">Anna Hasenfratz</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="2402.04175v1-abstract-short" style="display: inline;"> Common to many analysis pipelines in lattice gauge theory and the broader scientific discipline is the need to fit a semi-parametric model to data. We propose a fit method that utilizes a radial basis function network to approximate the non-parametric component of such models. The approximate parametric model is fit to data using the basin hopping global optimization algorithm. Parameter constrain&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2402.04175v1-abstract-full').style.display = 'inline'; document.getElementById('2402.04175v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2402.04175v1-abstract-full" style="display: none;"> Common to many analysis pipelines in lattice gauge theory and the broader scientific discipline is the need to fit a semi-parametric model to data. We propose a fit method that utilizes a radial basis function network to approximate the non-parametric component of such models. The approximate parametric model is fit to data using the basin hopping global optimization algorithm. Parameter constraints are enforced through Gaussian priors. The viability of our method is tested by examining its use in a finite-size scaling analysis of the $q$-state Potts model and $p$-state clock model with $q=2,3$ and $p=4,\infty$. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2402.04175v1-abstract-full').style.display = 'none'; document.getElementById('2402.04175v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 6 February, 2024; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> February 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">11 pages, 8 figures, 3 tables</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Report number:</span> FERMILAB-PUB-24-0042-V </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2305.10720">arXiv:2305.10720</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2305.10720">pdf</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Materials Science">cond-mat.mtrl-sci</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Applied Physics">physics.app-ph</span> </div> </div> <p class="title is-5 mathjax"> Observation and enhancement of room temperature bilinear magnetoelectric resistance in sputtered topological semimetal Pt3Sn </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/cond-mat?searchtype=author&amp;query=Fan%2C+Y">Yihong Fan</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Cresswell%2C+Z">Zach Cresswell</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Yang%2C+Y">Yifei Yang</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Jiang%2C+W">Wei Jiang</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Lv%2C+Y">Yang Lv</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Peterson%2C+T">Thomas Peterson</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Zhang%2C+D">Delin Zhang</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Liu%2C+J">Jinming Liu</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Low%2C+T">Tony Low</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Wang%2C+J">Jian-ping Wang</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="2305.10720v2-abstract-short" style="display: inline;"> Topological semimetal materials have become a research hotspot due to their intrinsic strong spin-orbit coupling which leads to large charge-to-spin conversion efficiency and novel transport behaviors. In this work, we have observed a bilinear magnetoelectric resistance (BMER) of up to 0.1 nm2A-1Oe-1 in a singlelayer of sputtered semimetal Pt3Sn at room temperature. Different from previous observa&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2305.10720v2-abstract-full').style.display = 'inline'; document.getElementById('2305.10720v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2305.10720v2-abstract-full" style="display: none;"> Topological semimetal materials have become a research hotspot due to their intrinsic strong spin-orbit coupling which leads to large charge-to-spin conversion efficiency and novel transport behaviors. In this work, we have observed a bilinear magnetoelectric resistance (BMER) of up to 0.1 nm2A-1Oe-1 in a singlelayer of sputtered semimetal Pt3Sn at room temperature. Different from previous observations, the value of BMER in sputtered Pt3Sn does not change out-of-plane due to the polycrystalline nature of Pt3Sn. The observation of BMER provides strong evidence of the existence of spin-momentum locking in the sputtered polycrystalline Pt3Sn. By adding an adjacent CoFeB magnetic layer, the BMER value of this bilayer system is doubled compared to the single Pt3Sn layer. This work broadens the material system in BMER study, which paves the way for the characterization of topological states and applications for spin memory and logic devices. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2305.10720v2-abstract-full').style.display = 'none'; document.getElementById('2305.10720v2-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 24 May, 2023; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 18 May, 2023; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> May 2023. </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2305.05801">arXiv:2305.05801</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2305.05801">pdf</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link 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/10.1038/s41467-023-39408-2">10.1038/s41467-023-39408-2 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Robust negative longitudinal magnetoresistance and spin-orbit torque in sputtered Pt3Sn topological semimetal </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/cond-mat?searchtype=author&amp;query=Zhang%2C+D">Delin Zhang</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Jiang%2C+W">Wei Jiang</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Yun%2C+H">Hwanhui Yun</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Benally%2C+O+J">Onri Jay Benally</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Peterson%2C+T">Thomas Peterson</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Cresswell%2C+Z">Zach Cresswell</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Fan%2C+Y">Yihong Fan</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Lv%2C+Y">Yang Lv</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Yu%2C+G">Guichuan Yu</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Barriocanal%2C+J+G">Javier Garcia Barriocanal</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Swatek%2C+P">Przemyslaw Swatek</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Mkhoyan%2C+K+A">K. Andre Mkhoyan</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Low%2C+T">Tony Low</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Wang%2C+J">Jian-Ping Wang</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="2305.05801v1-abstract-short" style="display: inline;"> Contrary to topological insulators, topological semimetals possess a nontrivial chiral anomaly that leads to negative magnetoresistance and are hosts to both conductive bulk states and topological surface states with intriguing transport properties for spintronics. Here, we fabricate highly-ordered metallic Pt3Sn and Pt3SnxFe1-x thin films via sputtering technology. Systematic angular dependence (&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2305.05801v1-abstract-full').style.display = 'inline'; document.getElementById('2305.05801v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2305.05801v1-abstract-full" style="display: none;"> Contrary to topological insulators, topological semimetals possess a nontrivial chiral anomaly that leads to negative magnetoresistance and are hosts to both conductive bulk states and topological surface states with intriguing transport properties for spintronics. Here, we fabricate highly-ordered metallic Pt3Sn and Pt3SnxFe1-x thin films via sputtering technology. Systematic angular dependence (both in-plane and out-of-plane) study of magnetoresistance presents surprisingly robust quadratic and linear negative longitudinal magnetoresistance features for Pt3Sn and Pt3SnxFe1-x, respectively. We attribute the anomalous negative longitudinal magnetoresistance to the type-II Dirac semimetal phase (pristine Pt3Sn) and/or the formation of tunable Weyl semimetal phases through symmetry breaking processes, such as magnetic-atom doping, as confirmed by first-principles calculations. Furthermore, Pt3Sn and Pt3SnxFe1-x show the promising performance for facilitating the development of advanced spin-orbit torque devices. These results extend our understanding of chiral anomaly of topological semimetals and can pave the way for exploring novel topological materials for spintronic devices. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2305.05801v1-abstract-full').style.display = 'none'; document.getElementById('2305.05801v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 9 May, 2023; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> May 2023. </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">13 pages, 4 figures</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> Nature Communications volume 14, Article number: 4151 (2023) </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2207.08872">arXiv:2207.08872</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2207.08872">pdf</a>]&nbsp;</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 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/10.1103/PhysRevMaterials.6.074206">10.1103/PhysRevMaterials.6.074206 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Room temperature spin-orbit torque efficiency in sputtered low-temperature superconductor delta-TaN </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/cond-mat?searchtype=author&amp;query=Swatek%2C+P+W">Przemyslaw Wojciech Swatek</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Hang%2C+X">Xudong Hang</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Fan%2C+Y">Yihong Fan</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Jiang%2C+W">Wei Jiang</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Yun%2C+H">Hwanhui Yun</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Lyu%2C+D">Deyuan Lyu</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Zhang%2C+D">Delin Zhang</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Peterson%2C+T+J">Thomas J. Peterson</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Sahu%2C+P">Protyush Sahu</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Benally%2C+O+J">Onri Jay Benally</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Cresswell%2C+Z">Zach Cresswell</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Liu%2C+J">Jinming Liu</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Pahari%2C+R">Rabindra Pahari</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Kukla%2C+D">Daniel Kukla</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Low%2C+T">Tony Low</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Mkhoyan%2C+K+A">K. Andre Mkhoyan</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Wang%2C+J">Jian-Ping Wang</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="2207.08872v2-abstract-short" style="display: inline;"> In the course of searching for promising topological materials for applications in future topological electronics, we evaluated spin-orbit torques (SOTs) in high-quality sputtered $未-$TaN/Co20Fe60B20 devices through spin-torque ferromagnetic resonance ST-FMR and spin pumping measurements. From the ST-FMR characterization we observed a significant linewidth modulation in the magnetic Co20Fe60B20 la&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2207.08872v2-abstract-full').style.display = 'inline'; document.getElementById('2207.08872v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2207.08872v2-abstract-full" style="display: none;"> In the course of searching for promising topological materials for applications in future topological electronics, we evaluated spin-orbit torques (SOTs) in high-quality sputtered $未-$TaN/Co20Fe60B20 devices through spin-torque ferromagnetic resonance ST-FMR and spin pumping measurements. From the ST-FMR characterization we observed a significant linewidth modulation in the magnetic Co20Fe60B20 layer attributed to the charge-to-spin conversion generated from the $未-$TaN layer. Remarkably, the spin-torque efficiency determined from ST-FMR and spin pumping measurements is as large as $螛 =$ 0.034 and 0.031, respectively. These values are over two times larger than for $伪-$Ta, but almost five times lower than for $尾-$Ta, which can be attributed to the low room temperature electrical resistivity $\sim 74渭惟$ cm in $未-$TaN. A large spin diffusion length of at least $\sim8$ nm is estimated, which is comparable to the spin diffusion length in pure Ta. Comprehensive experimental analysis, together with density functional theory calculations, indicates that the origin of the pronounced SOT effect in $未-$TaN can be mostly related to a significant contribution from the Berry curvature associated with the presence of a topically nontrivial electronic band structure in the vicinity of the Fermi level (EF). Through additional detailed theoretical analysis, we also found that an isostructural allotrope of the superconducting $未-$TaN phase, the simple hexagonal structure, $胃-$TaN, has larger Berry curvature, and that, together with expected reasonable charge conductivity, it can also be a promising candidate for exploring a generation of spin-orbit torque magnetic random access memory as cheap, temperature stable, and highly efficient spin current sources. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2207.08872v2-abstract-full').style.display = 'none'; document.getElementById('2207.08872v2-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 29 July, 2022; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 18 July, 2022; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> July 2022. </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">28 pages, 7 figures</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> Phys. Rev. Materials 6, 074206 (2022) </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2202.01384">arXiv:2202.01384</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2202.01384">pdf</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Materials Science">cond-mat.mtrl-sci</span> </div> </div> <p class="title is-5 mathjax"> Element Doping Enhanced Charge-to-Spin Conversion Efficiency in Amorphous PtSn4 Dirac Semimetal </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/cond-mat?searchtype=author&amp;query=Liu%2C+J">Jinming Liu</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Fan%2C+Y">Yihong Fan</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Zhang%2C+D">Delin Zhang</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Benally%2C+O+J">Onri J. Benally</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Bainsla%2C+L">Lakhan Bainsla</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Peterson%2C+T">Thomas Peterson</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Wang%2C+J">Jian-Ping Wang</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="2202.01384v1-abstract-short" style="display: inline;"> Topological semimetals (TSs) are promising candidates for low-power spin-orbit torque (SOT) devices due to their large charge-to-spin conversion efficiency. Here, we investigated the charge-to-spin conversion efficiency of amorphous PtSn4 (5 nm)/CoFeB (2.5-12.5 nm) layered structures prepared by a magnetron sputtering method at room temperature. The charge-to-spin ratio of PtSn4/CoFeB bilayers was&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2202.01384v1-abstract-full').style.display = 'inline'; document.getElementById('2202.01384v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2202.01384v1-abstract-full" style="display: none;"> Topological semimetals (TSs) are promising candidates for low-power spin-orbit torque (SOT) devices due to their large charge-to-spin conversion efficiency. Here, we investigated the charge-to-spin conversion efficiency of amorphous PtSn4 (5 nm)/CoFeB (2.5-12.5 nm) layered structures prepared by a magnetron sputtering method at room temperature. The charge-to-spin ratio of PtSn4/CoFeB bilayers was 0.08, characterized by a spin torque ferromagnetic resonance (ST-FMR) technique. This ratio can further increase to 0.14 by inducing dopants, like Al and CoSi, into PtSn4. The dopants can also decrease (Al doping) or increase (CoSi doping) the resistivity of PtSn4. The work proposed a way to enhance the spin-orbit coupling (SOC) in amorphous TSs with dopants. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2202.01384v1-abstract-full').style.display = 'none'; document.getElementById('2202.01384v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 2 February, 2022; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> February 2022. </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">18 pages, 5 figures</span> </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2101.11044">arXiv:2101.11044</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2101.11044">pdf</a>]&nbsp;</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> <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/10.1103/PhysRevLett.124.187701">10.1103/PhysRevLett.124.187701 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Voltage-controlled antiferromagnetism in magnetic tunnel junctions </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/cond-mat?searchtype=author&amp;query=Xu%2C+M">Meng Xu</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Li%2C+M">Mingen Li</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Khanal%2C+P">Pravin Khanal</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Habiboglu%2C+A">Ali Habiboglu</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Insana%2C+B">Blake Insana</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Xiong%2C+Y">Yuzan Xiong</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Peterson%2C+T">Thomas Peterson</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Myers%2C+J+C">Jason C. Myers</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Ortega%2C+D">Deborah Ortega</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Qu%2C+H">Hongwei Qu</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Chien%2C+C+L">C. L. Chien</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Zhang%2C+W">Wei Zhang</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Wang%2C+J">Jian-Ping Wang</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Wang%2C+W+G">W. G. Wang</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="2101.11044v1-abstract-short" style="display: inline;"> We demonstrate a voltage-controlled exchange bias effect in CoFeB/MgO/CoFeB magnetic tunnel junctions that is related to the interfacial Fe(Co)Ox formed between the CoFeB electrodes and the MgO barrier. The unique combination of interfacial antiferromagnetism, giant tunneling magnetoresistance, and sharp switching of the perpendicularly-magnetized CoFeB allows sensitive detection of the exchange b&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2101.11044v1-abstract-full').style.display = 'inline'; document.getElementById('2101.11044v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2101.11044v1-abstract-full" style="display: none;"> We demonstrate a voltage-controlled exchange bias effect in CoFeB/MgO/CoFeB magnetic tunnel junctions that is related to the interfacial Fe(Co)Ox formed between the CoFeB electrodes and the MgO barrier. The unique combination of interfacial antiferromagnetism, giant tunneling magnetoresistance, and sharp switching of the perpendicularly-magnetized CoFeB allows sensitive detection of the exchange bias. It is found that the exchange bias field can be isothermally controlled by magnetic fields at low temperatures. More importantly, the exchange bias can also be effectively manipulated by the electric field applied to the MgO barrier due to the voltage-controlled antiferromagnetic anisotropy in this system. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2101.11044v1-abstract-full').style.display = 'none'; document.getElementById('2101.11044v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 26 January, 2021; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> January 2021. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> Phys. Rev. Lett. 124, 187701, 2020 </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/2009.06711">arXiv:2009.06711</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2009.06711">pdf</a>]&nbsp;</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> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Other Condensed Matter">cond-mat.other</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/10.1103/PhysRevMaterials.5.045003">10.1103/PhysRevMaterials.5.045003 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Large field-like torque in amorphous Ru2Sn3 originated from the intrinsic spin Hall effect </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/cond-mat?searchtype=author&amp;query=Peterson%2C+T+J">Thomas J. Peterson</a>, <a href="/search/cond-mat?searchtype=author&amp;query=DC%2C+M">Mahendra DC</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Fan%2C+Y">Yihong Fan</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Chen%2C+J">Junyang Chen</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Zhang%2C+D">Delin Zhang</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Li%2C+H">Hongshi Li</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Swatek%2C+P">Przemyslaw Swatek</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Garcia-Barriocanal%2C+J">Javier Garcia-Barriocanal</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Wang%2C+J">Jian-Ping Wang</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="2009.06711v2-abstract-short" style="display: inline;"> We investigated temperature dependent current driven spin-orbit torques in magnetron sputtered Ru2Sn3 (4 and 10 nm) /Co20Fe60B20 (5 nm) layered structures with in-plane magnetic anisotropy. The room temperature damping-like and field-like spin torque efficiencies of the amorphous Ru2Sn3 films were measured to be 0.14 +- 0.008 (0.07 +- 0.012) and -0.03 +- 0.006 (-0.20 +- 0.009), for the 4 (10 nm) f&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2009.06711v2-abstract-full').style.display = 'inline'; document.getElementById('2009.06711v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2009.06711v2-abstract-full" style="display: none;"> We investigated temperature dependent current driven spin-orbit torques in magnetron sputtered Ru2Sn3 (4 and 10 nm) /Co20Fe60B20 (5 nm) layered structures with in-plane magnetic anisotropy. The room temperature damping-like and field-like spin torque efficiencies of the amorphous Ru2Sn3 films were measured to be 0.14 +- 0.008 (0.07 +- 0.012) and -0.03 +- 0.006 (-0.20 +- 0.009), for the 4 (10 nm) films respectively, by utilizing the second harmonic Hall technique. The large field-like torque in the relatively thicker Ru2Sn3 (10 nm) thin film is unique compared to the traditional spin Hall materials interfaced with thick magnetic layers with in-plane magnetic anisotropy which typically have dominant damping-like and negligible field-like torques. Additionally, the observed room temperature field-like torque efficiency in Ru2Sn3 (10 nm)/CoFeB (5 nm) is up to three times larger than the damping-like torque (-0.20 +- 0.009 and 0.07 +- 0.012, respectively) and thirty times larger at 50 K (-0.29 +- 0.014 and 0.009 +- 0.017, respectively). The temperature dependence of the field-like torques show dominant contributions from the intrinsic spin Hall effect while the damping-like torques show dominate contributions from the extrinsic spin Hall effects, skew scattering and side jump. Through macro-spin calculations, we found that including field-like torques on the order or larger than the damping-like torque can reduce the switching critical current and decrease magnetization procession for a perpendicular ferromagnetic layer. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2009.06711v2-abstract-full').style.display = 'none'; document.getElementById('2009.06711v2-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 4 March, 2021; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 14 September, 2020; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> September 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">Submitted to Physical Review Materials</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> Phys. Rev. Materials 5, 045003 (2021) </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/1909.02738">arXiv:1909.02738</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/1909.02738">pdf</a>, <a href="https://arxiv.org/format/1909.02738">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link 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/10.1103/PhysRevB.101.134430">10.1103/PhysRevB.101.134430 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> The interplay of large two-magnon ferromagnetic resonance linewidths and low Gilbert damping in Heusler thin films </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/cond-mat?searchtype=author&amp;query=Peria%2C+W+K">William K. Peria</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Peterson%2C+T+A">Timothy A. Peterson</a>, <a href="/search/cond-mat?searchtype=author&amp;query=McFadden%2C+A+P">Anthony P. McFadden</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Qu%2C+T">Tao Qu</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Liu%2C+C">Changjiang Liu</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Palmstr%C3%B8m%2C+C+J">Chris J. Palmstr酶m</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Crowell%2C+P+A">Paul A. Crowell</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="1909.02738v2-abstract-short" style="display: inline;"> We report on broadband ferromagnetic resonance linewidth measurements performed on epitaxial Heusler thin films. A large and anisotropic two-magnon scattering linewidth broadening is observed for measurements with the magnetization lying in the film plane, while linewidth measurements with the magnetization saturated perpendicular to the sample plane reveal low Gilbert damping constants of&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1909.02738v2-abstract-full').style.display = 'inline'; document.getElementById('1909.02738v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="1909.02738v2-abstract-full" style="display: none;"> We report on broadband ferromagnetic resonance linewidth measurements performed on epitaxial Heusler thin films. A large and anisotropic two-magnon scattering linewidth broadening is observed for measurements with the magnetization lying in the film plane, while linewidth measurements with the magnetization saturated perpendicular to the sample plane reveal low Gilbert damping constants of $(1.5\pm0.1)\times 10^{-3}$, $(1.8\pm0.2)\times 10^{-3}$, and $&lt;8\times 10^{-4}$ for Co$_2$MnSi/MgO, Co$_2$MnAl/MgO, and Co$_2$FeAl/MgO, respectively. The in-plane measurements are fit to a model combining Gilbert and two-magnon scattering contributions to the linewidth, revealing a characteristic disorder lengthscale of 10-100 nm. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1909.02738v2-abstract-full').style.display = 'none'; document.getElementById('1909.02738v2-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 9 April, 2020; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 6 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">8 pages, 5 figures</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> Phys. Rev. B 101, 134430 (2020) </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/1711.07969">arXiv:1711.07969</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/1711.07969">pdf</a>, <a href="https://arxiv.org/format/1711.07969">other</a>]&nbsp;</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> <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/10.1103/PhysRevB.97.020403">10.1103/PhysRevB.97.020403 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Suppression of the fieldlike spin-orbit torque efficiency due to the magnetic proximity effect in ferromagnet/platinum bilayers </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/cond-mat?searchtype=author&amp;query=Peterson%2C+T+A">T. A. Peterson</a>, <a href="/search/cond-mat?searchtype=author&amp;query=McFadden%2C+A+P">A. P. McFadden</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Palmstr%C3%B8m%2C+C+J">C. J. Palmstr酶m</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Crowell%2C+P+A">P. A. Crowell</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="1711.07969v2-abstract-short" style="display: inline;"> Current-induced spin-orbit torques in Co$_2$FeAl/Pt ultrathin bilayers are studied using a magnetoresistive harmonic response technique, which distinguishes the dampinglike and fieldlike contributions. The presence of a temperature-dependent magnetic proximity effect is observed through the anomalous Hall and anisotropic magnetoresistances, which are enhanced at low temperatures for thin platinum&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1711.07969v2-abstract-full').style.display = 'inline'; document.getElementById('1711.07969v2-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="1711.07969v2-abstract-full" style="display: none;"> Current-induced spin-orbit torques in Co$_2$FeAl/Pt ultrathin bilayers are studied using a magnetoresistive harmonic response technique, which distinguishes the dampinglike and fieldlike contributions. The presence of a temperature-dependent magnetic proximity effect is observed through the anomalous Hall and anisotropic magnetoresistances, which are enhanced at low temperatures for thin platinum thicknesses. The fieldlike torque efficiency decreases steadily as the temperature is lowered for all Pt thicknesses studied, which we propose is related to the influence of the magnetic proximity effect on the fieldlike torque mechanism. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1711.07969v2-abstract-full').style.display = 'none'; document.getElementById('1711.07969v2-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 21 November, 2017; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 21 November, 2017; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> November 2017. </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> Phys. Rev. B 97, 020403 (2018) </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/1610.03797">arXiv:1610.03797</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/1610.03797">pdf</a>, <a href="https://arxiv.org/format/1610.03797">other</a>]&nbsp;</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 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/10.1103/PhysRevB.94.235309">10.1103/PhysRevB.94.235309 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Spin injection and detection up to room temperature in Heusler~alloy/$n$-GaAs spin valves </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/cond-mat?searchtype=author&amp;query=Peterson%2C+T+A">T. A. Peterson</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Patel%2C+S+J">S. J. Patel</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Geppert%2C+C+C">C. C. Geppert</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Christie%2C+K+D">K. D. Christie</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Rath%2C+A">A. Rath</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Pennachio%2C+D">D. Pennachio</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Flatt%C3%A9%2C+M+E">M. E. Flatt茅</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Voyles%2C+P+M">P. M. Voyles</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Palmstr%C3%B8m%2C+C+J">C. J. Palmstr酶m</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Crowell%2C+P+A">P. A. Crowell</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="1610.03797v1-abstract-short" style="display: inline;"> We have measured the spin injection efficiency and spin lifetime in Co$_2$FeSi/$n$-GaAs lateral nonlocal spin valves from 20 to 300 K. We observe large ($\sim$40 $渭$V) spin valve signals at room temperature and injector currents of $10^3~$A/cm$^2$, facilitated by fabricating spin valve separations smaller than the 1 $渭$m spin diffusion length and applying a forward bias to the detector contact. Th&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1610.03797v1-abstract-full').style.display = 'inline'; document.getElementById('1610.03797v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="1610.03797v1-abstract-full" style="display: none;"> We have measured the spin injection efficiency and spin lifetime in Co$_2$FeSi/$n$-GaAs lateral nonlocal spin valves from 20 to 300 K. We observe large ($\sim$40 $渭$V) spin valve signals at room temperature and injector currents of $10^3~$A/cm$^2$, facilitated by fabricating spin valve separations smaller than the 1 $渭$m spin diffusion length and applying a forward bias to the detector contact. The spin transport parameters are measured by comparing the injector-detector contact separation dependence of the spin valve signal with a numerical model accounting for spin drift and diffusion. The apparent suppression of the spin injection efficiency at the lowest temperatures reflects a breakdown of the ordinary drift-diffusion model in the regime of large spin accumulation. A theoretical calculation of the D&#39;yakonov-Perel spin lifetime agrees well with the measured $n$-GaAs spin lifetime over the entire temperature range. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1610.03797v1-abstract-full').style.display = 'none'; document.getElementById('1610.03797v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 12 October, 2016; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> October 2016. </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">8 figures</span> </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/1508.02423">arXiv:1508.02423</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/1508.02423">pdf</a>, <a href="https://arxiv.org/ps/1508.02423">ps</a>, <a href="https://arxiv.org/format/1508.02423">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Disordered Systems and Neural Networks">cond-mat.dis-nn</span> <span class="tag is-small is-grey tooltip is-tooltip-top" data-tooltip="Mesoscale and Nanoscale Physics">cond-mat.mes-hall</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/10.1103/PhysRevB.92.140201">10.1103/PhysRevB.92.140201 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Anisotropic spin relaxation in $n$-GaAs from strong inhomogeneous hyperfine fields produced by the dynamical polarization of nuclei </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/cond-mat?searchtype=author&amp;query=Harmon%2C+N+J">N. J. Harmon</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Peterson%2C+T+A">T. A. Peterson</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Geppert%2C+C+C">C. C. Geppert</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Patel%2C+S+J">S. J. Patel</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Palmstr%C3%B8m%2C+C+J">C. J. Palmstr酶m</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Crowell%2C+P+A">P. A. Crowell</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Flatt%C3%A9%2C+M+E">M. E. Flatt茅</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="1508.02423v1-abstract-short" style="display: inline;"> The hyperfine field from dynamically polarized nuclei in n-GaAs is very spatially inhomogeneous, as the nu- clear polarization process is most efficient near the randomly-distributed donors. Electrons with polarized spins traversing the bulk semiconductor will experience this inhomogeneous hyperfine field as an effective fluctuating spin precession rate, and thus the spin polarization of an electr&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1508.02423v1-abstract-full').style.display = 'inline'; document.getElementById('1508.02423v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="1508.02423v1-abstract-full" style="display: none;"> The hyperfine field from dynamically polarized nuclei in n-GaAs is very spatially inhomogeneous, as the nu- clear polarization process is most efficient near the randomly-distributed donors. Electrons with polarized spins traversing the bulk semiconductor will experience this inhomogeneous hyperfine field as an effective fluctuating spin precession rate, and thus the spin polarization of an electron ensemble will relax. A theory of spin relaxation based on the theory of random walks is applied to such an ensemble precessing in an oblique magnetic field, and the precise form of the (unequal) longitudinal and transverse spin relaxation analytically derived. To investigate this mechanism, electrical three-terminal Hanle measurements were performed on epitaxially grown Co$_2$MnSi/$n$-GaAs heterostructures fabricated into electrical spin injection devices. The proposed anisotropic spin relaxation mechanism is required to satisfactorily describe the Hanle lineshapes when the applied field is oriented at large oblique angles. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1508.02423v1-abstract-full').style.display = 'none'; document.getElementById('1508.02423v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 10 August, 2015; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> August 2015. </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">submitted to Physical Review B Rapid Communications, 5 pages, 3 figures</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> Phys. Rev. B 92, 140201 (2015) </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/1508.02093">arXiv:1508.02093</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/1508.02093">pdf</a>, <a href="https://arxiv.org/ps/1508.02093">ps</a>, <a href="https://arxiv.org/format/1508.02093">other</a>]&nbsp;</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 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/10.1038/ncomms10296">10.1038/ncomms10296 <i class="fa fa-external-link" aria-hidden="true"></i></a></span> </div> </div> </div> <p class="title is-5 mathjax"> Dynamic detection of electron spin accumulation in ferromagnet-semiconductor devices by ferromagnetic resonance </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/cond-mat?searchtype=author&amp;query=Liu%2C+C">Changjiang Liu</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Patel%2C+S+J">Sahil J. Patel</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Peterson%2C+T+A">Timothy A. Peterson</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Geppert%2C+C+C">Chad C. Geppert</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Christie%2C+K+D">Kevin D. Christie</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Palmstr%C3%B8m%2C+C+J">Chris J. Palmstr酶m</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Crowell%2C+P+A">Paul A. Crowell</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="1508.02093v1-abstract-short" style="display: inline;"> A distinguishing feature of spin accumulation in ferromagnet-semiconductor devices is precession of the non-equilibrium spin population of the semiconductor in a magnetic field. This is the basis for detection techniques such as the Hanle effect, but these approaches become less effective as the spin lifetime in the semiconductor decreases. For this reason, no electrical Hanle measurement has been&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1508.02093v1-abstract-full').style.display = 'inline'; document.getElementById('1508.02093v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="1508.02093v1-abstract-full" style="display: none;"> A distinguishing feature of spin accumulation in ferromagnet-semiconductor devices is precession of the non-equilibrium spin population of the semiconductor in a magnetic field. This is the basis for detection techniques such as the Hanle effect, but these approaches become less effective as the spin lifetime in the semiconductor decreases. For this reason, no electrical Hanle measurement has been demonstrated in GaAs at room temperature. We show here that by forcing the magnetization in the ferromagnet (the spin injector and detector) to precess at the ferromagnetic resonance frequency, an electrically generated spin accumulation can be detected from 30 to 300 K. At low temperatures, the distinct Larmor precession of the spin accumulation in the semiconductor can be detected by ferromagnetic resonance in an oblique field. We verify the effectiveness of this new spin detection technique by comparing the injection bias and temperature dependence of the measured spin signal to the results obtained using traditional methods. We further show that this new approach enables a measurement of short spin lifetimes (&lt; 100 psec), a regime that is not accessible in semiconductors using traditional Hanle techniques. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('1508.02093v1-abstract-full').style.display = 'none'; document.getElementById('1508.02093v1-abstract-short').style.display = 'inline';">&#9651; Less</a> </span> </p> <p class="is-size-7"><span class="has-text-black-bis has-text-weight-semibold">Submitted</span> 9 August, 2015; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> August 2015. </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">4 figures</span> </p> <p class="comments is-size-7"> <span class="has-text-black-bis has-text-weight-semibold">Journal ref:</span> Nat. Commun. 7, 10296 (2016) </p> </li> </ol> <div class="is-hidden-tablet"> <!-- feedback for mobile only --> <span class="help" style="display: inline-block;"><a href="https://github.com/arXiv/arxiv-search/releases">Search v0.5.6 released 2020-02-24</a>&nbsp;&nbsp;</span> </div> </div> </main> <footer> <div class="columns is-desktop" role="navigation" aria-label="Secondary"> <!-- MetaColumn 1 --> <div class="column"> <div class="columns"> <div class="column"> <ul class="nav-spaced"> <li><a href="https://info.arxiv.org/about">About</a></li> <li><a href="https://info.arxiv.org/help">Help</a></li> </ul> </div> <div class="column"> <ul class="nav-spaced"> <li> <svg xmlns="http://www.w3.org/2000/svg" viewBox="0 0 512 512" class="icon filter-black" role="presentation"><title>contact arXiv</title><desc>Click here to contact arXiv</desc><path d="M502.3 190.8c3.9-3.1 9.7-.2 9.7 4.7V400c0 26.5-21.5 48-48 48H48c-26.5 0-48-21.5-48-48V195.6c0-5 5.7-7.8 9.7-4.7 22.4 17.4 52.1 39.5 154.1 113.6 21.1 15.4 56.7 47.8 92.2 47.6 35.7.3 72-32.8 92.3-47.6 102-74.1 131.6-96.3 154-113.7zM256 320c23.2.4 56.6-29.2 73.4-41.4 132.7-96.3 142.8-104.7 173.4-128.7 5.8-4.5 9.2-11.5 9.2-18.9v-19c0-26.5-21.5-48-48-48H48C21.5 64 0 85.5 0 112v19c0 7.4 3.4 14.3 9.2 18.9 30.6 23.9 40.7 32.4 173.4 128.7 16.8 12.2 50.2 41.8 73.4 41.4z"/></svg> <a href="https://info.arxiv.org/help/contact.html"> Contact</a> </li> <li> <svg xmlns="http://www.w3.org/2000/svg" viewBox="0 0 512 512" class="icon filter-black" role="presentation"><title>subscribe to arXiv mailings</title><desc>Click here to subscribe</desc><path d="M476 3.2L12.5 270.6c-18.1 10.4-15.8 35.6 2.2 43.2L121 358.4l287.3-253.2c5.5-4.9 13.3 2.6 8.6 8.3L176 407v80.5c0 23.6 28.5 32.9 42.5 15.8L282 426l124.6 52.2c14.2 6 30.4-2.9 33-18.2l72-432C515 7.8 493.3-6.8 476 3.2z"/></svg> <a href="https://info.arxiv.org/help/subscribe"> Subscribe</a> </li> </ul> </div> </div> </div> <!-- end MetaColumn 1 --> <!-- MetaColumn 2 --> <div class="column"> <div class="columns"> <div class="column"> <ul class="nav-spaced"> <li><a href="https://info.arxiv.org/help/license/index.html">Copyright</a></li> <li><a href="https://info.arxiv.org/help/policies/privacy_policy.html">Privacy Policy</a></li> </ul> </div> <div class="column sorry-app-links"> <ul class="nav-spaced"> <li><a href="https://info.arxiv.org/help/web_accessibility.html">Web Accessibility Assistance</a></li> <li> <p class="help"> <a class="a11y-main-link" href="https://status.arxiv.org" target="_blank">arXiv Operational Status <svg xmlns="http://www.w3.org/2000/svg" viewBox="0 0 256 512" class="icon filter-dark_grey" role="presentation"><path d="M224.3 273l-136 136c-9.4 9.4-24.6 9.4-33.9 0l-22.6-22.6c-9.4-9.4-9.4-24.6 0-33.9l96.4-96.4-96.4-96.4c-9.4-9.4-9.4-24.6 0-33.9L54.3 103c9.4-9.4 24.6-9.4 33.9 0l136 136c9.5 9.4 9.5 24.6.1 34z"/></svg></a><br> Get status notifications via <a class="is-link" href="https://subscribe.sorryapp.com/24846f03/email/new" target="_blank"><svg xmlns="http://www.w3.org/2000/svg" viewBox="0 0 512 512" class="icon filter-black" role="presentation"><path d="M502.3 190.8c3.9-3.1 9.7-.2 9.7 4.7V400c0 26.5-21.5 48-48 48H48c-26.5 0-48-21.5-48-48V195.6c0-5 5.7-7.8 9.7-4.7 22.4 17.4 52.1 39.5 154.1 113.6 21.1 15.4 56.7 47.8 92.2 47.6 35.7.3 72-32.8 92.3-47.6 102-74.1 131.6-96.3 154-113.7zM256 320c23.2.4 56.6-29.2 73.4-41.4 132.7-96.3 142.8-104.7 173.4-128.7 5.8-4.5 9.2-11.5 9.2-18.9v-19c0-26.5-21.5-48-48-48H48C21.5 64 0 85.5 0 112v19c0 7.4 3.4 14.3 9.2 18.9 30.6 23.9 40.7 32.4 173.4 128.7 16.8 12.2 50.2 41.8 73.4 41.4z"/></svg>email</a> or <a class="is-link" href="https://subscribe.sorryapp.com/24846f03/slack/new" target="_blank"><svg xmlns="http://www.w3.org/2000/svg" viewBox="0 0 448 512" class="icon filter-black" role="presentation"><path d="M94.12 315.1c0 25.9-21.16 47.06-47.06 47.06S0 341 0 315.1c0-25.9 21.16-47.06 47.06-47.06h47.06v47.06zm23.72 0c0-25.9 21.16-47.06 47.06-47.06s47.06 21.16 47.06 47.06v117.84c0 25.9-21.16 47.06-47.06 47.06s-47.06-21.16-47.06-47.06V315.1zm47.06-188.98c-25.9 0-47.06-21.16-47.06-47.06S139 32 164.9 32s47.06 21.16 47.06 47.06v47.06H164.9zm0 23.72c25.9 0 47.06 21.16 47.06 47.06s-21.16 47.06-47.06 47.06H47.06C21.16 243.96 0 222.8 0 196.9s21.16-47.06 47.06-47.06H164.9zm188.98 47.06c0-25.9 21.16-47.06 47.06-47.06 25.9 0 47.06 21.16 47.06 47.06s-21.16 47.06-47.06 47.06h-47.06V196.9zm-23.72 0c0 25.9-21.16 47.06-47.06 47.06-25.9 0-47.06-21.16-47.06-47.06V79.06c0-25.9 21.16-47.06 47.06-47.06 25.9 0 47.06 21.16 47.06 47.06V196.9zM283.1 385.88c25.9 0 47.06 21.16 47.06 47.06 0 25.9-21.16 47.06-47.06 47.06-25.9 0-47.06-21.16-47.06-47.06v-47.06h47.06zm0-23.72c-25.9 0-47.06-21.16-47.06-47.06 0-25.9 21.16-47.06 47.06-47.06h117.84c25.9 0 47.06 21.16 47.06 47.06 0 25.9-21.16 47.06-47.06 47.06H283.1z"/></svg>slack</a> </p> </li> </ul> </div> </div> </div> <!-- end MetaColumn 2 --> </div> </footer> <script src="https://static.arxiv.org/static/base/1.0.0a5/js/member_acknowledgement.js"></script> </body> </html>

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