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10.1088/1468-6996/10/2/024303 http://scihub22266oqcxt.onion/10.1088/1468-6996/10/2/024303 C5090433!5090433 !27877276     free     free     free Warning: file_get_contents(https://eutils.ncbi.nlm.nih.gov/entrez/eutils/elink.fcgi?dbfrom=pubmed&id=27877276 &cmd=llinks): Failed to open stream: HTTP request failed! 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Organic superconductors with an incommensurate anion structure |pdf=|usr=}}{{27877276 }} gab.com Text Organic superconductors with an incommensurate anion structure JO: Sci Technol Adv Mater http://www.kidney.de/pget.php?&tw=1&pmid=27877276 #FOAvip Superconducting incommensurate organic composite crystals based on the methylenedithio-tetraselenafulvalene (MDT-TSF) series donors, where the energy band filling deviates from the usual 3/4-filled, are reviewed. The incommensurate anion potential reconstructs the Fermi surface for both (MDT-TSF)(AuI(2))(0.436) and (MDT-ST)(I(3))(0.417) neither by the fundamental anion periodicity q nor by 2 q , but by 3 q , where MDT-ST is 5H-2-(1,3-dithiol-2-ylidene)-1,3-diselena-4,6-dithiapentalene, and q is the reciprocal lattice vector of the anion lattice. The selection rule of the reconstructing vectors is associated with the magnitude of the incommensurate potential. The considerably large interlayer transfer integral and three-dimensional superconducting properties are due to the direct donor-donor interactions coming from the characteristic corrugated conducting sheet structure. The materials with high superconducting transition temperature, T(c), have large ratios of the observed cyclotron masses to the bare ones, which indicates that the strength of the many-body effect is the major determinant of T(c). (MDT-TS)(AuI(2))(0.441) shows a metal-insulator transition at T(MI)=50 K, where MDT-TS is 5H-2-(1,3-diselenol-2-ylidene)-1,3,4,6-tetrathiapentalene, and the insulating phase is an antiferromagnet with a high Néel temperature (T(N)=50 K) and a high spin-flop field (B(sf)=6.9 T). There is a possibility that this material is an incommensurate Mott insulator. Hydrostatic pressure suppresses the insulating state and induces superconductivity at T(c)=3.2 K above 1.05 GPa, where T(c) rises to the maximum, T(c)(max)=4.9 K at 1.27 GPa. This compound shows a usual temperature-pressure phase diagram, in which the superconducting phase borders on the antiferromagnetic insulating phase, despite the unusual band filling. Twit Text FOAVip Organic superconductors with an incommensurate anion structure ????Sci Technol Adv Mater http://www.kidney.de/pget.php?&tw=1&pmid=27877276 #FOAvip Twit Text # Free Paper on # # # # # LINK http://www.kidney.de/pget.php?&tw=1&pmid=27877276 #FOAvip English Wikipedia <ref>{{Cite pmid|27877276 }}</ref> Organic superconductors with an incommensurate anion structure #MMPMID27877276 Kawamoto T ; Takimiya K Sci Technol Adv Mater 2009[Apr]; 10 (2 ): 024303 PMID27877276 show ga Superconducting incommensurate organic composite crystals based on the methylenedithio-tetraselenafulvalene (MDT-TSF) series donors, where the energy band filling deviates from the usual 3/4-filled, are reviewed. The incommensurate anion potential reconstructs the Fermi surface for both (MDT-TSF)(AuI(2))(0.436) and (MDT-ST)(I(3))(0.417) neither by the fundamental anion periodicity q nor by 2 q , but by 3 q , where MDT-ST is 5H-2-(1,3-dithiol-2-ylidene)-1,3-diselena-4,6-dithiapentalene, and q is the reciprocal lattice vector of the anion lattice. The selection rule of the reconstructing vectors is associated with the magnitude of the incommensurate potential. The considerably large interlayer transfer integral and three-dimensional superconducting properties are due to the direct donor-donor interactions coming from the characteristic corrugated conducting sheet structure. The materials with high superconducting transition temperature, T(c), have large ratios of the observed cyclotron masses to the bare ones, which indicates that the strength of the many-body effect is the major determinant of T(c). (MDT-TS)(AuI(2))(0.441) shows a metal-insulator transition at T(MI)=50 K, where MDT-TS is 5H-2-(1,3-diselenol-2-ylidene)-1,3,4,6-tetrathiapentalene, and the insulating phase is an antiferromagnet with a high Néel temperature (T(N)=50 K) and a high spin-flop field (B(sf)=6.9 T). There is a possibility that this material is an incommensurate Mott insulator. Hydrostatic pressure suppresses the insulating state and induces superconductivity at T(c)=3.2 K above 1.05 GPa, where T(c) rises to the maximum, T(c)(max)=4.9 K at 1.27 GPa. This compound shows a usual temperature-pressure phase diagram, in which the superconducting phase borders on the antiferromagnetic insulating phase, despite the unusual band filling. äOrganic superconductors with an incommensurate anion structure (epmc).pdf DeepDyve Pubget Overpricing