Historical research guide · 0916 · 2011
Light-Induced Superconductivity in a Stripe-Ordered Cuprate
D. Fausti · R. I. Tobey · N. Dean · S. Kaiser · A. Dienst · M. C. Hoffmann · S. Pyon · T. Takayama · H. Takagi · A. Cavalleri
In one minute
Some copper-oxide compounds refuse to superconduct because their electrons lock into stripes — alternating one-dimensional lanes of spin and charge that hold the material rigid. Fausti, Tobey, Dean and colleagues in Andrea Cavalleri’s group hit one of those compounds, a lanthanum-europium-strontium copper oxide that does not superconduct at all, with a femtosecond pulse of mid-infrared light. For a moment afterwards it is a superconductor, and not a single-layer one: current moves coherently between the copper-oxide planes as well as within them, which makes it three-dimensional. They know because a Josephson plasma resonance appears promptly in the material’s optical response along the stacking axis, the fingerprint of coherent tunnelling from layer to layer. The striking number is the clock. The superconducting phase assembles within one to two picoseconds at most, far faster than anyone expected it could. That speed is the result’s teeth: it puts hard new limits on what stripe order can be and on how it is related to superconductivity.
Connection
Chapter 11 treats superconductors as the material where the most interesting effects are looked for, and this is the demonstration that superconductivity itself can be switched on by light in a compound that does not have it — a property of matter driven into existence rather than doped in. Chapter 2 keeps the ledger of what a driven electromagnetic field can be made to do to a medium, and a single infrared pulse turning a striped, non-superconducting crystal into a three-dimensional superconductor belongs on that ledger.
From the source
One of the most intriguing features of some high-temperature cuprate superconductors is the interplay between one-dimensional striped spin order and charge order on the one hand, and superconductivity on the other.Abstract, first sentence
The starting material is chosen precisely because it does not superconduct: La1.675Eu0.2Sr0.125CuO4, a stripe-ordered cuprate in its nonsuperconducting state.Abstract, second sentence
Mid-infrared femtosecond pulses transform that compound into a transient three-dimensional superconductor — the superconductivity is induced by the light, not present beforehand.Abstract, second sentence
The evidence for the claim is a specific optical signature: the emergence of coherent interlayer transport is evidenced by the prompt appearance of a Josephson plasma resonance in the c-axis optical properties, which is the response of coherent tunnelling between the copper-oxide planes.Abstract, third sentence
An upper limit for the time scale needed to form the superconducting phase is estimated at 1 to 2 picoseconds, which the authors state is significantly faster than expected.Abstract, fourth sentence
The consequence the authors draw is theoretical rather than technological: the speed of formation places stringent new constraints on our understanding of stripe order and its relation to superconductivity, which is the question the follow-up experiments are aimed at.Abstract, closing sentence
The way in
https://doi.org/10.1126/science.1197294How to cite it
D. Fausti, R. I. Tobey, N. Dean, S. Kaiser, A. Dienst, M. C. Hoffmann, S. Pyon, T. Takayama, H. Takagi, A. Cavalleri (2011) Light-Induced Superconductivity in a Stripe-Ordered Cuprate doi:10.1126/science.1197294