Showing posts with label University of Bath. Show all posts
Showing posts with label University of Bath. Show all posts

Friday, July 8, 2016

Controlling matter with light




For a recent colloquium at the University of Bath, Professor Andrea Cavalleri was invited to talk about his work on ‘controlling solid phases with light’. A team led by Andrea at the Max Planck Institute for the Structure and Dynamics of Matter have been studying the response of materials using intense laser pulses of low frequency. I asked Andrea about the motivation for the work in their most recent paper, and the future of controlling matter with light.
Mostly, scientists have probed matter non-resonantly using lasers operating at frequencies near the visible part of the spectrum. More recently however, radiation in the mid infra-red to THz region of the spectrum has provided direct access to the low energy excitations in solids, such as phonons, excitons, and many others. Due to advances in high power sources, this type of radiation can be used not only to probe matter, but to drive it into a new transient state.
Andrea’s team have been ultimately seeking to control matter with light by driving solids into a non-equilibrium state, and this includes the optical enhancement of superconductivity.
“Our goal in particular is to use light to generate phases that do not occur spontaneously at equilibrium, like for example superconductivity at higher temperatures. Traditionally, quantum-phase discovery has been achieved by materials synthesis or by using pressure or strong magnetic fields, but the ability to generate sculpted, coherent light fields opens new possibilities which are only starting to be explored.”
 Schematic LTT crystal structure for LESCOx. © 2016 IOP Publishing Ltd. All rights reserved.
Schematic LTT crystal structure for LESCOx. ©2016 IOP Publishing Ltd. All rights reserved.
In 2011, the team were able to measure superconducting-like optical properties in the cuprate, LESCO at temperatures far greater than the equilibrium transition temperature using these methods. Later, the same was found for YBCO and x-ray diffraction experiments hinted at intense light pulses forcing a structural change to the crystal as the driving mechanism for enhanced superconductivity.
Now, the team have focused on potassium doped buckyballs to see if the same effects can be seen. Buckyballs (Buckminsterfullerene) are large carbon cages made up of 60 atoms. When doped with potassium to form K3C60, the material becomes superconducting with an equilibrium transition temperature of 20 K.
In their experiments, a mid-infrared laser pulse (the ‘pump’) was firstly used to excite K3C60 powder in the range of 80 – 200 meV photon energy. Shortly after (about 1 ps), the excited state was measured using a second pulse (the ‘probe’) of THz frequency, which is used to detect changes in the reflectivity. It was found that the mid-infrared pulses had induced a large increase in carrier mobility and the opening of a gap in the optical conductivity which then disappears around a picosecond later.
These superconducting-like optical properties mimic the same signatures seen when cooling K3C60 below its equilibrium transition temperature. And so for a fleeting second (…or picosecond), light had driven the material into a superconducting state! What’s even more interesting is that the state seemingly survives up to around 100 K, which is around 5 times greater than the equilibrium transition temperature.
Similar to the team’s work on YBCO, they explain their results by light pulses distorting the crystal lattice which may increase the electron-phonon coupling, favouring stronger superconductivity. However, the results for K3C60 are even more convincing than their previous work on the cuprates since the interpretation of these experiments was difficult as their highly unconventional superconduting state is still not fully understood. In addition, the cuprates are two dimensional materials with peculiar transport properties.
“The novelty of our result on K3C60 resides in the fact that it demonstrates that light-induced superconductivity is a far more general phenomenon than previously envisaged. Unlike cuprates, K3C60 is a fully three-dimensional molecular solid, where the equilibrium superconducting state is quite conventional and fairly well understood.”
The optical signatures seen in the team’s experiments are extremely short lived and the superconducting-like state only exists on the order of picoseconds. Currently, this is too short for the traditional superconducting tests of zero electrical resistance and expulsion of magnetic fields (Meissner effect) to be performed. However, the optical signatures are clear and the work of Cavalleri et al. paves the way for controlling phenomena in solids with light.
“The possibilities offered by intense, sculpted light fields at THz frequencies for controlling and switching complex matter is enormous.”
An application using current methods of short light pulses could be to create a highly efficient switchable superconductor device. Conversely, if the light-induced state can be maintained for any significant time, the idea of creating optically pumped room temperature superconductors could become a reality.
“Great efforts are being aimed at developing new THz sources, which can produce picosecond-to-nanosecond narrow band, high field pulses, tunable in the broadest possible spectral range. These may be used to drive transient superconductors in a quasi-persistent mode, thus extending their lifetime.”
It is clear to see that we have only scratched the surface of this relatively new phenomenon, but the future is truly exciting.

Monday, May 23, 2016

SpectroscopyNOW- Laser challenge: Infrared pulse


http://www.spectroscopynow.com/ir/details/highlight/14de329bf14/Last-Months-Most-Accessed-Feature-Laser-challenge-Infrared-pulse.html

Bubbly laser

The fiber's long and thin bubbles of glass reflect light into the fiber's core much in the same way that light reflects off the surface of the soap bubble in the foreground, making it appear iridescent. Credit: University of Bath
Researchers in the UK have designed and constructed a new type of laser that can generate pulsed or continuous mid-infrared (IR) emission in the challenging 3.1 to 3.2 micrometre wavelength range. Writing in The Optical Society's journal Optica, William Wadsworth and colleagues at the University of Bath, explain how they have achieved a spectral range that has been an obstacle for laser developers for a long time. The new system could be useful in mid-infrared spectroscopy, environmental sensing and detection and even consumer devices.
The new laser combines aspects of stable, high-quality, high-power hollow-fibre lasers with an appropriate gas in the hollow optical fibre to create a fibre gas laser. "Beyond about 2.8 micrometres, conventional fibre lasers start to fall off in terms of power, and the other main technology for the mid IR, quantum cascade lasers, doesn't pick up until beyond 3.5 micrometres," says Wadsworth explain the difficult gap. He led the research team alongside Bath's Jonathan Knight.

Gas and fibres

Key to the new laser's success is the team's development of silica hollow-core fibres that perform exceptionally well in the mid-IR. Hollow-core fibres are a new class of fibres that use internal glass structures to confine light within, whereas conventional optical fibres confine light in a solid core of glass. "You can think of the structures in our fibres as very long and thin bubbles of glass," muses Wadsworth. "By surrounding the region of space in the middle of the fibre with the bubbles, light that is reflected by the bubbles will be trapped inside of the hollow core." The light travelling within the hollow fibre remains mostly in the empty core and so wavelengths beyond 2.8 micrometres are not lost. Silica is the preferred material for optical fibres because it is relatively inexpensive, easy to manufacture and extremely strong.
The team points out that lasers require an electric current or a pumping laser to excite a material's electrons, which then emit photons as they drop back to their unexcited state. The researchers used acetylene gas, which emits in the mid-IR and can be excited, or pumped, using laser technology adapted from the telecommunications industry. The research shows that the hollow-core fibres can hold gas and trap light in the same place so that they might interact over lengths of 10 or 11 metres in the team's experiments. Such coupling has been done before, but the novelty of this work lies in the addition of a feedback fibre. This last component was essential to building a true laser.
The feedback fibre takes a small amount of light produced in the fibre containing the acetylene gas and uses that light to seed another cycle of light amplification; this reduces the pump power required to produce a laser beam. Critically for future applications is the use of practical, inexpensive diode lasers from the already mature telecommunications sector.

Wavelength extension

"We developed a way to use light to pump molecules and generate light that is not that common to see in a laser system," explains team member Fei Yu. "This new way to construct a gas laser could be expanded to make more and more laser types that would have been impossible without our hollow-core fibre." The same approach should work with other gases allowing emission up to 5 micrometres. "This laser is just one use of our hollow-core fibre," adds team member Muhammad Rosdi Abu Hassan. "We see it stimulating other applications of the hollow fibre and new ways of interacting different types of laser beams with gases at various wavelengths, including wavelengths that you wouldn't expect to work."
The next phase in the resarch will involve improvements to the laser output, Hassan told SpectroscopyNOW. "At the moment, the maximum laser output is 4 milliwatts with 8.8% laser efficiency for synchronous pumping and 2.5 milliwatts with 6.7% laser efficiency for Continuous Wave (CW) laser," he explained. "Mid-infrared fibre lasers when compared to fibre lasers that emit at 1 or 2 micrometres are seen to produce significantly lower output power. However, our system is extremely low threshold running stably around 3 micrometres and scalable through the use of existing 1.5 micrometre laser technology using an oscillator/amplifier configuration."