Possible Fano resonance for high-Tc multi-gap superconductivity in p-Terphenyl doped by K at the Lifshitz transition

被引:42
作者
Mazziotti, Maria Vittoria [1 ]
Valletta, Antonio [2 ]
Campi, Gaetano [3 ]
Innocenti, Davide [4 ]
Perali, Andrea [5 ]
Bianconi, Antonio [1 ,3 ,6 ,7 ]
机构
[1] Rome Int Ctr Mat Sci Superstripes, RICMASS, Via Sabelli 119A, I-00185 Rome, Italy
[2] CNR, Inst Microelect & Microsyst, Via Fosso Cavaliere 100, I-00133 Rome, Italy
[3] CNR, Inst Crystallog, Via Salaria,Km 29-300, I-00015 Monterotondo Roma, Italy
[4] Univ Liverpool, Dept Chem, Liverpool L69 7ZD, Merseyside, England
[5] Univ Camerino, Phys Unit, Sch Pharm, Camerino, Italy
[6] Natl Res Nucl Univ, MEPhI Moscow Engn Phys Inst, Kashirskoe Shosse 31, Moscow 115409, Russia
[7] Latvian Acad Sci, Akad Laukums 1, LV-1050 Riga, Latvia
关键词
SHAPE RESONANCE; QUANTUM STRIPES; PHASE; SUPERLATTICE; DISORDER; ORDER;
D O I
10.1209/0295-5075/118/37003
中图分类号
O4 [物理学];
学科分类号
0702 ;
摘要
Recent experiments have reported the emergence of high-temperature superconductivity with critical temperature T-c between 43K and 123K in a potassium-doped aromatic hydrocarbon para-Terphenyl or p-Terphenyl. This achievement provides the record for the highest T-c in an organic superconductor overcoming the previous record of T-c = 38K in Cs3C60 fulleride. Here we propose that the driving mechanism is the quantum resonance between superconducting gaps near a Lifshitz transition which belongs to the class of Fano resonances called shape resonances. For the case of p-Terphenyl our numerical solutions of the multigap equation shows that high T-c is driven by tuning the chemical potential by K doping and it appears only in a narrow energy range near a Lifshitz transition. At the maximum critical temperature, T-c = 123 K, the condensate in the appearing new small Fermi surface pocket is in the BCS-BEC crossover while the T-c drops below 0.3K where it is in the BEC regime. Finally, we predict the experimental results which can support or falsify our proposed mechanism: a) the variation of the isotope coefficient as a function of the critical temperature and b) the variation of the gaps and their ratios 2 Delta/T-c as a function of T-c. Copyright (C) EPLA, 2017
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页数:7
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