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10.1038/srep15302 http://scihub22266oqcxt.onion/10.1038/srep15302 C4609968!4609968 !26477669     free     free     free Deprecated: Implicit conversion from float 211.6 to int loses precision in C:\Inetpub\vhosts\kidney.de\httpdocs\pget.php on line 534 Deprecated: Implicit conversion from float 211.6 to int loses precision in C:\Inetpub\vhosts\kidney.de\httpdocs\pget.php on line 534 Deprecated: Implicit conversion from float 211.6 to int loses precision in C:\Inetpub\vhosts\kidney.de\httpdocs\pget.php on line 534 Warning: imagejpeg(C:\Inetpub\vhosts\kidney.de\httpdocs\phplern\26477669 .jpg): Failed to open stream: No such file or directory in C:\Inetpub\vhosts\kidney.de\httpdocs\pget.php on line 117       Sci+Rep 2015 ; 5 (ä): 15302 Nephropedia Template TP {{tp|p=26477669 |t=2015. Route to Topological Superconductivity via Magnetic Field Rotation |pdf=|usr=}}{{26477669 }} gab.com Text Route to Topological Superconductivity via Magnetic Field Rotation JO: Sci Rep http://www.kidney.de/pget.php?&tw=1&pmid=26477669 #FOAvip The verification of topological superconductivity has become a major experimental challenge. Apart from the very few spin-triplet superconductors with p-wave pairing symmetry, another candidate system is a conventional, two-dimensional (2D) s-wave superconductor in a magnetic field with a sufficiently strong Rashba spin-orbit coupling. Typically, the required magnetic field to convert the superconductor into a topologically non-trivial state is however by far larger than the upper critical field H(c2), which excludes its realization. In this article, we argue that this problem can be overcome by rotating the magnetic field into the superconducting plane. We explore the character of the superconducting state upon changing the strength and the orientation of the magnetic field and show that a topological state, established for a sufficiently strong out-of-plane magnetic field, indeed extends to an in-plane field orientation. We present a three-band model applicable to the superconducting interface between LaAlO3 and SrTiO3, which should fulfil the necessary conditions to realize a topological superconductor. Twit Text FOAVip Route to Topological Superconductivity via Magnetic Field Rotation ????Sci Rep http://www.kidney.de/pget.php?&tw=1&pmid=26477669 #FOAvip Twit Text # Free Paper on # # # # # LINK http://www.kidney.de/pget.php?&tw=1&pmid=26477669 #FOAvip English Wikipedia <ref>{{Cite pmid|26477669 }}</ref> Route to Topological Superconductivity via Magnetic Field Rotation #MMPMID26477669 Loder F ; Kampf AP ; Kopp T Sci Rep 2015[Oct]; 5 (ä): 15302 PMID26477669 show ga The verification of topological superconductivity has become a major experimental challenge. Apart from the very few spin-triplet superconductors with p-wave pairing symmetry, another candidate system is a conventional, two-dimensional (2D) s-wave superconductor in a magnetic field with a sufficiently strong Rashba spin-orbit coupling. Typically, the required magnetic field to convert the superconductor into a topologically non-trivial state is however by far larger than the upper critical field H(c2), which excludes its realization. In this article, we argue that this problem can be overcome by rotating the magnetic field into the superconducting plane. We explore the character of the superconducting state upon changing the strength and the orientation of the magnetic field and show that a topological state, established for a sufficiently strong out-of-plane magnetic field, indeed extends to an in-plane field orientation. We present a three-band model applicable to the superconducting interface between LaAlO3 and SrTiO3, which should fulfil the necessary conditions to realize a topological superconductor. äRoute to Topological Superconductivity via Magnetic Field Rotation (epmc).pdf DeepDyve Pubget Overpricing