Solution to two long-standing mysteries of cuprate superconductivity found

May 08, 2014
Scientists find solution to 2 long-standing mysteries of cuprate superconductivity
Disappearing stripes linked with free electron movement: Scientists used a precision microscope to simultaneously explore electrons' arrangements and movements as charge carriers called holes were added to transform a copper-oxide material from an insulator to a superconductor. With increasing hole density, the material first takes on a mysterious Credit: Brookhaven National Laboratory

Scientists seeking to understand the intricacies of high-temperature superconductivity—the ability of certain materials to carry electrical current with no energy loss—have been particularly puzzled by a mysterious phase that emerges as charge carriers are added that appears to compete with superconductivity. It's also been a mystery why, within this "pseudogap" phase, the movement of superconducting electrons appears to be restricted to certain directions. So exploring the pseudogap and whether and how it affects the movement of electrons has been a pivotal challenge.

Now, a team lead by scientists at the U.S. Department of Energy's (DOE) Brookhaven National Laboratory and Cornell University have used unique capabilities to reveal detailed characteristics of the electrons in one of these materials as it transforms from an insulator through the mysterious pseudogap phase and eventually into a full-blown superconductor. The results, described in the May 9, 2014, issue of Science, link two distinct personality changes in the material's electrons: the disappearance of a rather exotic periodic static arrangement of certain electrons within the pseudogap phase, and the sudden ability of all the material's electrons to move freely in any direction. The finding strengthens support for the idea that the periodic arrangement—variously referred to as "stripes" or "density waves"—restricts the flow of electrons and impairs maximal in the pseudogap phase.

"This is the first time an experiment has directly linked the disappearance of the density waves and their associated nanoscale crystal distortions with the emergence of universally free-flowing electrons needed for unrestricted superconductivity," said lead author J.C. Séamus Davis, a senior physicist and Director of DOE's Center for Emergent Superconductivity at Brookhaven Lab and also a professor at both Cornell University and the St. Andrews University in Scotland. "These new measurements finally show us why, in the mysterious pseudogap state of this material, the electrons are less free to move."

That information, in turn, may help scientists engineer ways to get superconductivity flowing under more favorable conditions. Right now, even these "high-temperature" copper-oxide materials operate as superconductors only when cooled to below -100 degrees Celsius. "That's room temperature during a particularly bad winter in Antarctica," Davis said. The hope is to find ways to raise the operating temperature for real-world energy-saving applications—things like highly efficient power generation and transmission and computers that work at speeds thousands of times faster than today's.

Unique tool tracks electronic states

In their native state, even at super chilly temperatures, the copper-oxide materials are actually strong insulators. To induce them to superconduct, the scientists chemically inject additional electronic carriers, a process called doping. But tracking how this process alters the electronic structure and associated nanoscale distortions as the material transforms from insulator to pseudogap phase and eventually full-blown superconductivity is no easy task.

"The crystal distortions appear in our experiments like the ghostly, smeary shadows that a moving person makes in a long photographic exposure, making it difficult to really recognize their features and their character, or even see them at all in many cases," said Simon Billinge, a Brookhaven physicist who heads a team exploring the role of such nanoscale fluctuations in superconductors and other complex materials. "We are only now developing tools and methods to see and track these subtle effects."

To capture the elusive electronic behavior, Chung-Koo Kim, a postdoctoral fellow in Billinge's group, and Kazuhiro Fujita, a Research Associate in Davis' Group, worked with Davis using a spectroscopic imaging scanning tunneling microscope invented by the latter. This tool allows the scientists to simultaneously visualize the spatial arrangements of individual static electrons and the direction of travel of those that are free to move. They systematically scanned the copper-oxide material under various levels of doping to see how the arrangements and behavior of the electrons changed as the material evolved.

Davis likens the technique to flying over a frozen river where you can see static patterns formed by the ice while also detecting flowing liquid water—and doing it over and over through the spring as the frozen waterway gradually melts. In the copper-oxide material, instead of raising the temperature, the scientists raise the level of doping to "melt" the density waves at a particular "critical point."

"This was a massive effort, taking many person-years, making long and difficult measurements on multiple samples to track the evolution of these two effects," Davis said.

Evidence of electron personality change

At low charge carrier density, the microscopic flyovers revealed somewhat static, ordered electrons—the "frozen" stripe patterns—and the flow of superconducting electrons limited to only certain directions. But subsequent scans taken as more charge carriers were added revealed that the static pattern disappeared and electrons began to flow freely in all directions at exactly the same level of doping—close to the point at which the most robust superconductivity sets in.

"This is the first direct observation that these two phenomena are linked: The with their associated nanoscale distortions disappear and the electrons in the material change their personality suddenly at a well-defined material composition," Billinge said.

This direct observation confirms a long-held suspicion that the static electron arrangement and associated nanoscale fluctuations impair the free flow of electrons—like ice on a river impairs the flow of liquid water, Davis said. By analogy, adding charge carriers breaks up the static pattern, like melting the ice.

"We are demonstrating that when the electrons are no longer hampered by the 'frozen' density wave state, they become universally free to flow unimpeded," Davis said.

Another way to look at it, Billinge said, is by thinking of a chess game with kings, bishops, and knights filling the board so none can move. As you gradually remove some of the pieces—analogous to doping with called "holes," which is what the scientists did—some of the pieces would be free to move according to their usual rules. More holes would allow more movement. But what the scientists observed instead is that at low "hole" concentration, certain kinds of movement (say, the kings' forward and sideways movements) were prohibited and that the chessboard itself appeared to have a different kind of pattern—stripes instead of alternating squares. But at the critical hole concentration—precisely 20 percent—the researchers found that both the quantum rules-of-the-game and the board itself changed, allowing the free movement of all pieces.

Of course, freeing in a copper-oxide insulator to get superconducting current flowing for useful applications won't be quite as easy as melting ice to get liquid water or removing pieces from a chessboard. But it does offer clues.

"What this discovery implies is that if you prevented the static stripes from ever occurring, you might end up with a material that could act as a superconductor at a lower density of doping—and a much higher temperature," Davis said.

Explore further: Scientists gain new insight into mysterious electronic phenomenon

More information: "Simultaneous Transitions in Cuprate Momentum-Space Topology and Electronic Symmetry Breaking" Science, 2014.

add to favorites email to friend print save as pdf

Related Stories

A grand unified theory of exotic superconductivity?

Oct 17, 2013

(Phys.org) —Years of experiments on various types of high-temperature (high-Tc) superconductors—materials that offer hope for energy-saving applications such as zero-loss electrical power lines—have ...

Recommended for you

New terahertz device could strengthen security

Nov 21, 2014

We are all familiar with the hassles that accompany air travel. We shuffle through long lines, remove our shoes, and carry liquids in regulation-sized tubes. And even after all the effort, we still wonder if these procedures ...

CERN makes public first data of LHC experiments

Nov 21, 2014

CERN today launched its Open Data Portal where data from real collision events, produced by experiments at the Large Hadron Collider (LHC) will for the first time be made openly available to all. It is expected ...

User comments : 1

Adjust slider to filter visible comments by rank

Display comments: newest first

Pejico
May 08, 2014
This comment has been removed by a moderator.
Pejico
May 08, 2014
This comment has been removed by a moderator.
johanfprins
not rated yet May 09, 2014
A superconducting phase consists of stationary Mott-orbitals. When injecting charge-carriers, they replace those charge-carriers near the injecting contact, while the replaced charge-carriers move on to replace the next ones, etc. In order to break loose and move to the next site, a charge-carrier requires an energy E=E(B)+1/2*m*v^2 where E(B) is the binding energy of the stationary charge carrier and 1/2*m*v^2 the KE required to move through a distance R to the next trapping site. This energy is obtained from a quantum fluctuation which provides the energ E for an allowed time interval (delta)t.

When R is too large, SC motion cannot occur since not enough energy E is available for a long enough time interval (delta)t. The pseudo-phase is the formation of Mott-orbitals. The critical distances R appears initially along rows of these orbitals: Stripes. At a high enough density, motion is not only restricted along certain directions. The SC- and pseudo-phases are simple to model.

Please sign in to add a comment. Registration is free, and takes less than a minute. Read more

Click here to reset your password.
Sign in to get notified via email when new comments are made.