{"status":"ok","message-type":"work","message-version":"1.0.0","message":{"indexed":{"date-parts":[[2026,9,26]],"date-time":"2026-09-26T16:52:52Z","timestamp":1790441572603,"version":"4.1.0"},"reference-count":45,"publisher":"Springer Science and Business Media LLC","issue":"1","license":[{"start":{"date-parts":[[2020,1,17]],"date-time":"2020-01-17T00:00:00Z","timestamp":1579219200000},"content-version":"tdm","delay-in-days":0,"URL":"https:\/\/creativecommons.org\/licenses\/by\/4.0"},{"start":{"date-parts":[[2020,1,17]],"date-time":"2020-01-17T00:00:00Z","timestamp":1579219200000},"content-version":"vor","delay-in-days":0,"URL":"https:\/\/creativecommons.org\/licenses\/by\/4.0"}],"content-domain":{"domain":["link.springer.com"],"crossmark-restriction":false},"short-container-title":["NPG Asia Mater"],"published-print":{"date-parts":[[2020,12]]},"abstract":"Abstract<\/jats:title>Pure spin current transport has become the central point of the state-of-the-art spintronics. While most spin current phenomena have been extensively explored, aspects of the pure spin current injected into ferromagnetic metals are far from completely understood. The reports on a fundamental problem, i.e. the spin relaxation asymmetry with spin current polarization collinear or transverse to the magnetization of ferromagnetic metals, are quite controversial. By employing a Y3<\/jats:sub>Fe5<\/jats:sub>O12<\/jats:sub> (YIG)\/Cu\/Ni80<\/jats:sub>Fe20<\/jats:sub> (Py)\/Ir25<\/jats:sub>Mn75<\/jats:sub> (IrMn) spin valve heterostructure with the thermal inverse spin Hall effect (ISHE) of a Py well separated from other thermoelectric transport and thermal Hall effects, we find that the ISHE signal amplitude in 10\u2009nm Py increases by 80% when changing the relative orientation of the YIG and Py magnetization from orthogonal (\u22a5) to collinear (||). Moreover, the spin-diffusion length \u03bb<\/jats:italic>sf<\/jats:sub> and effective spin Hall angle $$\\theta _{{\\mathrm{SH}}}^{{\\mathrm{eff}}}$$<\/jats:tex-math>\n \n \n \u03b8<\/mml:mi>\n <\/mml:mrow>\n \n SH<\/mml:mi>\n <\/mml:mrow>\n \n eff<\/mml:mi>\n <\/mml:mrow>\n <\/mml:msubsup>\n <\/mml:math><\/jats:alternatives><\/jats:inline-formula> of Py are also spin orientation dependent and vary from $$\\lambda _{{\\mathrm{sf}}}^ \\bot$$<\/jats:tex-math>\n \n \n \u03bb<\/mml:mi>\n <\/mml:mrow>\n \n sf<\/mml:mi>\n <\/mml:mrow>\n \n \u22a5<\/mml:mo>\n <\/mml:mrow>\n <\/mml:msubsup>\n <\/mml:math><\/jats:alternatives><\/jats:inline-formula>\u2009=\u20091.0\u2009\u00b1\u20090.1\u2009nm to $$\\lambda _{{\\mathrm{sf}}}^\\parallel$$<\/jats:tex-math>\n \n \n \u03bb<\/mml:mi>\n <\/mml:mrow>\n \n sf<\/mml:mi>\n <\/mml:mrow>\n \n \u2225<\/mml:mo>\n <\/mml:mrow>\n <\/mml:msubsup>\n <\/mml:math><\/jats:alternatives><\/jats:inline-formula>\u2009=\u20092.8\u2009\u00b1\u20090.5\u2009nm with $$\\theta _{{\\mathrm{SH}}}^{{\\mathrm{eff}}}\\left( \\bot \\right)\/\\theta _{{\\mathrm{SH}}}^{{\\mathrm{eff}}}\\left( \\parallel \\right)$$<\/jats:tex-math>\n \n \n \n \u03b8<\/mml:mi>\n <\/mml:mrow>\n \n SH<\/mml:mi>\n <\/mml:mrow>\n \n eff<\/mml:mi>\n <\/mml:mrow>\n <\/mml:msubsup>\n \n \n \u22a5<\/mml:mo>\n <\/mml:mrow>\n <\/mml:mfenced>\n \u2215<\/mml:mo>\n \n \n \u03b8<\/mml:mi>\n <\/mml:mrow>\n \n SH<\/mml:mi>\n <\/mml:mrow>\n \n eff<\/mml:mi>\n <\/mml:mrow>\n <\/mml:msubsup>\n \n \n \u2225<\/mml:mo>\n <\/mml:mrow>\n <\/mml:mfenced>\n <\/mml:mrow>\n <\/mml:math><\/jats:alternatives><\/jats:inline-formula>\u2009=\u20091.5, respectively. Our results demonstrate magnetization orientation-dependent spin relaxation and spin injection efficiency of a pure spin current, revealing that exchange interactions in ferromagnetic metals strongly affect the transport of the pure spin current.<\/jats:p>","DOI":"10.1038\/s41427-019-0191-1","type":"journal-article","created":{"date-parts":[[2020,1,17]],"date-time":"2020-01-17T00:03:03Z","timestamp":1579219383000},"update-policy":"https:\/\/doi.org\/10.1007\/springer_crossmark_policy","source":"Crossref","is-referenced-by-count":16,"title":["Strong spin orientation-dependent spin current diffusion and inverse spin Hall effect in a ferromagnetic metal"],"prefix":"10.1038","volume":"12","author":[{"given":"Zhaozhao","family":"Zhu","sequence":"first","affiliation":[],"role":[{"vocabulary":"crossref","role":"author"}]},{"given":"Xiaoli","family":"Zheng","sequence":"additional","affiliation":[],"role":[{"vocabulary":"crossref","role":"author"}]},{"given":"Gang","family":"Li","sequence":"additional","affiliation":[],"role":[{"vocabulary":"crossref","role":"author"}]},{"given":"He","family":"Bai","sequence":"additional","affiliation":[],"role":[{"vocabulary":"crossref","role":"author"}]},{"given":"Jian","family":"Su","sequence":"additional","affiliation":[],"role":[{"vocabulary":"crossref","role":"author"}]},{"given":"Ying","family":"Zhang","sequence":"additional","affiliation":[],"role":[{"vocabulary":"crossref","role":"author"}]},{"given":"Jian-Wang","family":"Cai","sequence":"additional","affiliation":[],"role":[{"vocabulary":"crossref","role":"author"}]}],"member":"297","published-online":{"date-parts":[[2020,1,17]]},"reference":[{"key":"191_CR1","doi-asserted-by":"crossref","first-page":"262","DOI":"10.1038\/nature08876","volume":"464","author":"Y Kajiwara","year":"2010","unstructured":"Kajiwara, Y. et al. 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