scholarly journals Universal description of granular metals at low temperatures: Granular Fermi liquid

2004 ◽  
Vol 70 (20) ◽  
Author(s):  
I. S. Beloborodov ◽  
A. V. Lopatin ◽  
V. M. Vinokur
1999 ◽  
Vol 112 (12) ◽  
pp. 707-711 ◽  
Author(s):  
M.O. Dzero ◽  
L.P. Gor'kov ◽  
V.Z. Kresin

2006 ◽  
Vol 7 (5) ◽  
pp. 809-898 ◽  
Author(s):  
G. Benfatto ◽  
A. Giuliani ◽  
V. Mastropietro

Physica ◽  
1971 ◽  
Vol 52 (2) ◽  
pp. 193-204 ◽  
Author(s):  
L.E. Reichl ◽  
E.R. Tuttle

2016 ◽  
Vol 113 (48) ◽  
pp. 13654-13659 ◽  
Author(s):  
Cyril Proust ◽  
Baptiste Vignolle ◽  
Julien Levallois ◽  
S. Adachi ◽  
Nigel E. Hussey

Our knowledge of the ground state of underdoped hole-doped cuprates has evolved considerably over the last few years. There is now compelling evidence that, inside the pseudogap phase, charge order breaks translational symmetry leading to a reconstructed Fermi surface made of small pockets. Quantum oscillations [Doiron-Leyraud N, et al. (2007)Nature447(7144):565–568], optical conductivity [Mirzaei SI, et al. (2013)Proc Natl Acad Sci USA110(15):5774–5778], and the validity of Wiedemann–Franz law [Grissonnache G, et al. (2016)Phys Rev B93:064513] point to a Fermi liquid regime at low temperature in the underdoped regime. However, the observation of a quadratic temperature dependence in the electrical resistivity at low temperatures, the hallmark of a Fermi liquid regime, is still missing. Here, we report magnetoresistance measurements in the magnetic-field–induced normal state of underdoped YBa2Cu4O8that are consistent with aT2resistivity extending down to 1.5 K. The magnitude of theT2coefficient, however, is much smaller than expected for a single pocket of the mass and size observed in quantum oscillations, implying that the reconstructed Fermi surface must consist of at least one additional pocket.


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