Kanigel A, Chatterjee U, Randeria M, Norman M R, Koren G, Kadowaki K, Campuzano J C
Department of Physics, University of Illinois at Chicago, Chicago, Illinois 60607, USA.
Phys Rev Lett. 2008 Sep 26;101(13):137002. doi: 10.1103/PhysRevLett.101.137002.
In the underdoped high temperature superconductors, instead of a complete Fermi surface above Tc, only disconnected Fermi arcs appear, separated by regions that still exhibit an energy gap. We show that in this pseudogap phase, the energy-momentum relation of electronic excitations near EF behaves like the dispersion of a normal metal on the Fermi arcs, but like that of a superconductor in the gapped regions. We argue that this dichotomy in the dispersion is difficult to reconcile with a competing order parameter, but is consistent with pairing without condensation.
在欠掺杂高温超导体中,高于临界温度(Tc)时并非出现完整的费米面,而是仅出现断开的费米弧,被仍存在能隙的区域隔开。我们表明,在这个赝能隙相中,费米能级(EF)附近电子激发的能量 - 动量关系在费米弧上表现得像正常金属的色散,但在能隙区域表现得像超导体的色散。我们认为这种色散的二分法难以与竞争序参量相协调,但与无凝聚的配对是一致的。