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href="/search/advanced?terms-0-term=Putz%2C+R&amp;terms-0-field=author&amp;size=50&amp;order=-announced_date_first">Advanced Search</a> </div> </div> <input type="hidden" name="order" value="-announced_date_first"> <input type="hidden" name="size" value="50"> </form> <div class="level breathe-horizontal"> <div class="level-left"> <form method="GET" action="/search/"> <div style="display: none;"> <select id="searchtype" name="searchtype"><option value="all">All fields</option><option value="title">Title</option><option selected value="author">Author(s)</option><option value="abstract">Abstract</option><option value="comments">Comments</option><option value="journal_ref">Journal reference</option><option value="acm_class">ACM classification</option><option value="msc_class">MSC classification</option><option value="report_num">Report number</option><option value="paper_id">arXiv identifier</option><option value="doi">DOI</option><option value="orcid">ORCID</option><option 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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/2110.09205">arXiv:2110.09205</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/2110.09205">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"> Control of Electrochemical Corrosion Properties by Influencing Mn Partitioning through Intercritically Annealing of Medium-Mn Steel </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/cond-mat?searchtype=author&amp;query=P%C3%BCtz%2C+R+D">Ren茅 Daniel P眉tz</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Allam%2C+T">Tarek Allam</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Wang%2C+J">Junmiao Wang</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Nowak%2C+J">Jakub Nowak</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Haase%2C+C">Christian Haase</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Sandl%C3%B6bes-Haut%2C+S">Stefanie Sandl枚bes-Haut</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Krupp%2C+U">Ulrich Krupp</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Zander%2C+D">Daniela Zander</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="2110.09205v1-abstract-short" style="display: inline;"> Medium-Mn steels exhibit excellent mechanical properties and lower production costs compared to high-Mn steels, which makes them a potential material for future application in the automotive industry. Intercritical annealing (ICA) after cold rolling allows to control the stacking fault energy (SFE) of austenite, the fraction of ferrite and reverted austenite, and the element partitioning (especial&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2110.09205v1-abstract-full').style.display = 'inline'; document.getElementById('2110.09205v1-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="2110.09205v1-abstract-full" style="display: none;"> Medium-Mn steels exhibit excellent mechanical properties and lower production costs compared to high-Mn steels, which makes them a potential material for future application in the automotive industry. Intercritical annealing (ICA) after cold rolling allows to control the stacking fault energy (SFE) of austenite, the fraction of ferrite and reverted austenite, and the element partitioning (especially Mn). Although Mn deteriorates the corrosion behavior of Fe-Mn-Al alloys, the influence of austenite fraction and element partitioning of Mn on the electrochemical corrosion behavior has not been investigated yet. Therefore, the electrochemical corrosion behavior in 0.1 M H2SO4 of X6MnAl12-3, which was intercritically annealed for 2 h at 550 掳C, 600 掳C and 700 掳C, was investigated by potentiodynamic polarization (PDP), electrochemical impedance spectroscopy (EIS) and mass spectroscopy with inductively coupled plasma (ICP-MS). Additionally, specimens after 1 h and 24 h of immersion were examined via SEM to visualize the corrosion damage. The ICA specimens showed a selective dissolution of reverted austenite due to its micro-galvanic coupling with the adjacent ferrite. The severity of the micro-galvanic coupling can be reduced by decreasing the interface area as well as the chemical gradient of mainly Mn between ferrite and reverted austenite by ICA. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('2110.09205v1-abstract-full').style.display = 'none'; document.getElementById('2110.09205v1-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> 18 October, 2021; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> October 2021. </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">23 pages, 14 Figures, 4 Tables</span> </p> </li> <li class="arxiv-result"> <div class="is-marginless"> <p class="list-title is-inline-block"><a href="https://arxiv.org/abs/cond-mat/9410039">arXiv:cond-mat/9410039</a> <span>&nbsp;[<a href="https://arxiv.org/pdf/cond-mat/9410039">pdf</a>, <a href="https://arxiv.org/ps/cond-mat/9410039">ps</a>, <a href="https://arxiv.org/format/cond-mat/9410039">other</a>]&nbsp;</span> </p> <div class="tags is-inline-block"> <span class="tag is-small is-link tooltip is-tooltip-top" data-tooltip="Condensed Matter">cond-mat</span> </div> </div> <p class="title is-5 mathjax"> Conserving approximation for the three-band Hubbard model: flat quasiparticle dispersion </p> <p class="authors"> <span class="search-hit">Authors:</span> <a href="/search/cond-mat?searchtype=author&amp;query=Putz%2C+R">R. Putz</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Preuss%2C+R">R. Preuss</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Muramatsu%2C+A">A. Muramatsu</a>, <a href="/search/cond-mat?searchtype=author&amp;query=Hanke%2C+W">W. Hanke</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="cond-mat/9410039v3-abstract-short" style="display: inline;"> It is shown that the low-energy single-particle excitation-spectrum of the three-band Hubbard model at hole-dopings away from half-filling agrees remarkably well with Quantum Monte Carlo data and spectroscopic experiments within the framework of a conserving approximation that includes self-consistently the interaction with charge, spin, and two-particle fluctuations. The dispersion of the quasi&hellip; <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('cond-mat/9410039v3-abstract-full').style.display = 'inline'; document.getElementById('cond-mat/9410039v3-abstract-short').style.display = 'none';">&#9661; More</a> </span> <span class="abstract-full has-text-grey-dark mathjax" id="cond-mat/9410039v3-abstract-full" style="display: none;"> It is shown that the low-energy single-particle excitation-spectrum of the three-band Hubbard model at hole-dopings away from half-filling agrees remarkably well with Quantum Monte Carlo data and spectroscopic experiments within the framework of a conserving approximation that includes self-consistently the interaction with charge, spin, and two-particle fluctuations. The dispersion of the quasiparticle-peak obtained from the spectral-weight function is flat around the $(蟺,0)$ and $(0,蟺)$ points as has been observed in recent angle-resolved photoemission measurement. The significant reduction of the quasiparticle-dispersion near the Fermi-energy is due to spin-fluctuations, rather than being induced by band effects. <a class="is-size-7" style="white-space: nowrap;" onclick="document.getElementById('cond-mat/9410039v3-abstract-full').style.display = 'none'; document.getElementById('cond-mat/9410039v3-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 October, 1994; <span class="has-text-black-bis has-text-weight-semibold">v1</span> submitted 12 October, 1994; <span class="has-text-black-bis has-text-weight-semibold">originally announced</span> October 1994. </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">REVtex, 10 pages, 4 figures (in uuencoded postscript format) appended at the end of the file</span> </p> </li> </ol> <div 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