{"status":"ok","message-type":"work","message-version":"1.0.0","message":{"indexed":{"date-parts":[[2025,12,13]],"date-time":"2025-12-13T15:30:59Z","timestamp":1765639859535,"version":"3.48.0"},"reference-count":64,"publisher":"IOP Publishing","issue":"26","license":[{"start":{"date-parts":[[2020,3,31]],"date-time":"2020-03-31T00:00:00Z","timestamp":1585612800000},"content-version":"vor","delay-in-days":0,"URL":"https:\/\/publishingsupport.iopscience.iop.org\/iop-standard\/v1"},{"start":{"date-parts":[[2020,3,31]],"date-time":"2020-03-31T00:00:00Z","timestamp":1585612800000},"content-version":"tdm","delay-in-days":0,"URL":"https:\/\/iopscience.iop.org\/info\/page\/text-and-data-mining"}],"content-domain":{"domain":["iopscience.iop.org"],"crossmark-restriction":false},"short-container-title":["J. Phys.: Condens. Matter"],"published-print":{"date-parts":[[2020,6,17]]},"abstract":"<jats:title>Abstract<\/jats:title>\n                  <jats:p>\n                    A multi-functional Gd\n                    <jats:sub>5<\/jats:sub>\n                    Si\n                    <jats:sub>1.3<\/jats:sub>\n                    Ge\n                    <jats:sub>2.7<\/jats:sub>\n                    thin film deposited by pulsed laser ablation in the form of an ensemble of nanoparticles was studied for 18 thermal cycles via electron transport measurements together with structural and magnetic characterization. A general negative thermal dependency of the resistivity (\n                    <jats:italic>\u03c1<\/jats:italic>\n                    ) is observed, which contrasts with the metallic-like behavior observed in bulk Gd\n                    <jats:sub>5<\/jats:sub>\n                    Si\n                    <jats:sub>\n                      <jats:italic>x<\/jats:italic>\n                    <\/jats:sub>\n                    Ge\n                    <jats:sub>\n                      4\u2212\n                      <jats:italic>x<\/jats:italic>\n                    <\/jats:sub>\n                    compounds. This general trend is interrupted by a two-step, positive-slope transition in\n                    <jats:italic>\u03c1<\/jats:italic>\n                    (\n                    <jats:italic>T<\/jats:italic>\n                    ) throughout the [150, 250] K interval, corresponding to two consecutive magnetic transitions: a fully coupled magnetostructural followed by a magnetic order on heating. An avalanche-like behavior is unveiled by the \u2202\n                    <jats:italic>\u03c1<\/jats:italic>\n                    \/\u2202\n                    <jats:italic>T<\/jats:italic>\n                    (\n                    <jats:italic>T<\/jats:italic>\n                    ) curves and is explained based on the severe strains induced cyclically by the magnetostructural transition, leading to a cycling evolution of the transition onset temperature (\n                    <jats:inline-formula>\n                      <jats:tex-math>\n                        \n                      <\/jats:tex-math>\n                      <mml:math xmlns:mml=\"http:\/\/www.w3.org\/1998\/Math\/MathML\" display=\"inline\" overflow=\"scroll\">\n                        <mml:mi>\u2202<\/mml:mi>\n                        <mml:msubsup>\n                          <mml:mrow>\n                            <mml:mi>T<\/mml:mi>\n                          <\/mml:mrow>\n                          <mml:mrow>\n                            <mml:mi mathvariant=\"normal\">h<\/mml:mi>\n                          <\/mml:mrow>\n                          <mml:mrow>\n                            <mml:mo>\u2033<\/mml:mo>\n                          <\/mml:mrow>\n                        <\/mml:msubsup>\n                      <\/mml:math>\n                    <\/jats:inline-formula>\n                    \/\u2202\n                    <jats:italic>n<\/jats:italic>\n                    \u223c 1.6 K\/cycle,\n                    <jats:italic>n<\/jats:italic>\n                    being the number of cycles). Such behavior is equivalent to the action of a pressure of 0.56 kBar being formed and building up at every thermal cycle due to the large volume induced change across the magnetostructural transition. Moreover the thermal hysteresis, detected in both\n                    <jats:italic>\u03c1<\/jats:italic>\n                    and magnetization versus temperature curves, evolves significantly along the cycles, decreasing as\n                    <jats:italic>n<\/jats:italic>\n                    increases. This picture corroborates the thermal activation energy enhancement\u2014estimated via an exponential fitting of the \u2202\n                    <jats:italic>\u03c1<\/jats:italic>\n                    \/\u2202\n                    <jats:italic>T<\/jats:italic>\n                    (\n                    <jats:italic>T<\/jats:italic>\n                    ) in the avalanche regime. This work demonstrates the importance of using a short-range order technique, to probe both magnetic and magnetostructural transitions and their evolution with thermal cycles.\n                  <\/jats:p>","DOI":"10.1088\/1361-648x\/ab79f9","type":"journal-article","created":{"date-parts":[[2020,2,25]],"date-time":"2020-02-25T17:30:42Z","timestamp":1582651842000},"page":"265401","update-policy":"https:\/\/doi.org\/10.1088\/crossmark-policy","source":"Crossref","is-referenced-by-count":1,"title":["Evolution of two-step magnetic transition on nanogranular Gd\n                    <sub>5<\/sub>\n                    Si\n                    <sub>1.3<\/sub>\n                    Ge\n                    <sub>2.7<\/sub>\n                    thin film"],"prefix":"10.1088","volume":"32","author":[{"ORCID":"https:\/\/orcid.org\/0000-0003-0010-1568","authenticated-orcid":false,"given":"J H","family":"Belo","sequence":"first","affiliation":[]},{"given":"A L","family":"Pires","sequence":"additional","affiliation":[]},{"given":"I T","family":"Gomes","sequence":"additional","affiliation":[]},{"given":"J B","family":"Sousa","sequence":"additional","affiliation":[]},{"given":"R L","family":"Hadimani","sequence":"additional","affiliation":[]},{"given":"D C","family":"Jiles","sequence":"additional","affiliation":[]},{"given":"A M","family":"Pereira","sequence":"additional","affiliation":[]},{"given":"J P","family":"Ara\u00fajo","sequence":"additional","affiliation":[]}],"member":"266","published-online":{"date-parts":[[2020,3,31]]},"reference":[{"key":"cmab79f9bib1","doi-asserted-by":"publisher","DOI":"10.1116\/1.4882858","type":"journal-article","article-title":"Magnetocaloric effect in nanoscale thin films and heterostructures","volume":"32","author":"Miller","year":"2014","journal-title":"J. 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