Nonlinear c-axis transport in Bi_2Sr_2CaCu_2O_(8+d) from two-barrier tunneling

Abstract

Motivated by the peculiar features observed through intrinsic tunneling spectroscopy of Bi${}_2$Sr${}_2$CaCu${}_2$O${}_{8+\delta }$ mesas in the normal state, we have extended the normal state two-barrier model for the c-axis transport [M. Giura et al., Phys. Rev. B {\bf 68}, 134505 (2003)] to the analysis of $dI/dV$ curves. We have found that the purely normal-state model reproduces all the following experimental features: (a) the parabolic $V$-dependence of $dI/dV$ in the high-$T$ region (above the conventional pseudogap temperature), (b) the emergence and the nearly voltage-independent position of the "humps" from this parabolic behavior lowering the temperature, and (c) the crossing of the absolute $dI/dV$ curves at a characteristic voltage $V^{\times }$. Our findings indicate that conventional tunneling can be at the origin of most of the uncommon features of the c axis transport in Bi${}_2$Sr${}_2$CaCu${}_2$O${}_{8+\delta }$. We have compared our calculations to experimental data taken in severely underdoped and slightly underdoped Bi${}_2$Sr${}_2$CaCu${}_2$O${}_{8+\delta }$ small mesas. We have found good agreement between the data and the calculations, without any shift of the calculated dI/dV on the vertical scale. In particular, in the normal state (above $T^{\ast }$) simple tunneling reproduces the experimental dI/dV quantitatively. Below $T^{\ast }$ quantitative discrepancies are limited to a simple rescaling of the voltage in the theoretical curves by a factor $\sim$2. The need for such modifications remains an open question, that might be connected to a change of the charge of a fraction of the carriers across the pseudogap opening.

arXiv comment7 pages, 5 figures

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