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10.1038/ncomms12576 http://scihub22266oqcxt.onion/10.1038/ncomms12576 C5013552!5013552 !27573209     free     free     free Deprecated: Implicit conversion from float 229.6 to int loses precision in C:\Inetpub\vhosts\kidney.de\httpdocs\pget.php on line 534 Deprecated: Implicit conversion from float 229.6 to int loses precision in C:\Inetpub\vhosts\kidney.de\httpdocs\pget.php on line 534 Deprecated: Implicit conversion from float 229.6 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\27573209 .jpg): Failed to open stream: No such file or directory in C:\Inetpub\vhosts\kidney.de\httpdocs\pget.php on line 117       Nat+Commun 2016 ; 7 (ä): 12576 Nephropedia Template TP {{tp|p=27573209 |t=2016. Temperature-driven massless Kane fermions in HgCdTe crystals |pdf=|usr=}}{{27573209 }} gab.com Text Temperature-driven massless Kane fermions in HgCdTe crystals JO: Nat Commun http://www.kidney.de/pget.php?&tw=1&pmid=27573209 #FOAvip It has recently been shown that electronic states in bulk gapless HgCdTe offer another realization of pseudo-relativistic three-dimensional particles in condensed matter systems. These single valley relativistic states, massless Kane fermions, cannot be described by any other relativistic particles. Furthermore, the HgCdTe band structure can be continuously tailored by modifying cadmium content or temperature. At critical concentration or temperature, the bandgap collapses as the system undergoes a semimetal-to-semiconductor topological phase transition between the inverted and normal alignments. Here, using far-infrared magneto-spectroscopy we explore the continuous evolution of band structure of bulk HgCdTe as temperature is tuned across the topological phase transition. We demonstrate that the rest mass of Kane fermions changes sign at critical temperature, whereas their velocity remains constant. The velocity universal value of (1.07±0.05) × 10(6)?m?s(-1) remains valid in a broad range of temperatures and Cd concentrations, indicating a striking universality of the pseudo-relativistic description of the Kane fermions in HgCdTe. Twit Text FOAVip Temperature-driven massless Kane fermions in HgCdTe crystals ????Nat Commun http://www.kidney.de/pget.php?&tw=1&pmid=27573209 #FOAvip Twit Text # Free Paper on # # # # # LINK http://www.kidney.de/pget.php?&tw=1&pmid=27573209 #FOAvip English Wikipedia <ref>{{Cite pmid|27573209 }}</ref> Temperature-driven massless Kane fermions in HgCdTe crystals #MMPMID27573209 Teppe F ; Marcinkiewicz M ; Krishtopenko SS ; Ruffenach S ; Consejo C ; Kadykov AM ; Desrat W ; But D ; Knap W ; Ludwig J ; Moon S ; Smirnov D ; Orlita M ; Jiang Z ; Morozov SV ; Gavrilenko VI ; Mikhailov NN ; Dvoretskii SA Nat Commun 2016[Aug]; 7 (ä): 12576 PMID27573209 show ga It has recently been shown that electronic states in bulk gapless HgCdTe offer another realization of pseudo-relativistic three-dimensional particles in condensed matter systems. These single valley relativistic states, massless Kane fermions, cannot be described by any other relativistic particles. Furthermore, the HgCdTe band structure can be continuously tailored by modifying cadmium content or temperature. At critical concentration or temperature, the bandgap collapses as the system undergoes a semimetal-to-semiconductor topological phase transition between the inverted and normal alignments. Here, using far-infrared magneto-spectroscopy we explore the continuous evolution of band structure of bulk HgCdTe as temperature is tuned across the topological phase transition. We demonstrate that the rest mass of Kane fermions changes sign at critical temperature, whereas their velocity remains constant. The velocity universal value of (1.07±0.05) × 10(6)?m?s(-1) remains valid in a broad range of temperatures and Cd concentrations, indicating a striking universality of the pseudo-relativistic description of the Kane fermions in HgCdTe. äTemperature-driven massless Kane fermions in HgCdTe crystals (epmc).pdf DeepDyve Pubget Overpricing