Probing the relationship between superexchange and superconductivity in cuprates

One of the most basic ideas in science is the controlled experiment. A single "independent" variable is changed while all others are held fixed. One then observes how the properties of the system change. Unfortunately, reality is more complicated and there are rarely any truly independent variables, particularly in materials science.

Since the discovery of cuprate superconductors one-quarter of a century ago there has been a constant struggle to tease out systematic trends that can provide insight into the underlying physics causing the superconductivity. This is a challenge because it is difficult to change only one variable. For example, a key property is how the superconductivity changes with the chemical composition of the material, particularly with regard to the doping level, i.e., the density of charge carriers. The problem is that with changes in doping, many other things change as well: the amount of disorder, the periodicity and strength of magnetic interactions, crystal structure, ... 

There is a beautiful experimental paper that recently overcomes these problems. 

On the electron pairing mechanism of copper-oxide high temperature superconductivity

Shane M. O’Mahony, Wangping Ren, Weijiong Chen,  Yi Xue Chong, Xiaolong Liu, H. Eisaki, S. Uchida, M. H. Hamidian, and J. C. Séamus Davis 

In a very clever way they can do all their measurements on a single material of fixed chemical composition, and yet vary a key parameter, the size of the energy difference between the relevant oxygen and copper electronic states, Epsilon.

In the material under study,  Bi2Sr2CaCu2O8+x, there are CuO5 units, as pictured below. In the crystal there is a modulation of delta, the distance at which the fifth oxygen sits above the CuO4 squares that form the square lattices that comprise the layers responsible for the superconductivity.

Due to electrostatics, the distance delta has an effect on the energy Epsilon. This in turn changes the size of the magnetic superexchange between neighbouring copper spins, as pictured below.

In the experiment, a STM is used to measure how Epsilon varies as delta varies (see the red dots in the Figure below). We then expect this to vary the superexchange.

An electron-pair (Josephson) STM is used to measure the magnitude of the superfluid density (electron-pair density) and how it changes with delta (see the blue dots in the figure below).

These two sets of measurement are combined in the second figure below. 

The yellow band in the figure above is the range of values expected from theory, including the recent paper.

Oxygen hole content, charge-transfer gap, covalency, and cuprate superconductivity

Nicolas Kowalski, Sidhartha Shankar Dash, Patrick Sémon, David Sénéchal, and André-Marie Tremblay

The theory is based on DMFT calculations for a three-band Hubbard model, following earlier work including by Weber, Haule, Kotliar, and independently by Maier.

Quanta magazine has a popular report on the experiment. The headline, "High-Temperature Superconductivity Understood at Last", overstates the significance of the experiment.

There are still issues of correlation versus causality. I would also like to see what other theories predict for the relationship between Epsilon and the pairing density. Nevertheless, it is a beautiful experiment and marks a significant advance.