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Tuesday, 11 Dec 2018

Researchers develop organic-perovskite laser diode

An organic laser can be made to produce any wavelength, this tunability would be very useful in applications ranging from medical diagnostics to environmental sensing


20 Nov 2017 | Editor

A team of researchers from Penn State and Princeton University have taken a big step toward creating a diode laser from a hybrid organic-inorganic material that can be deposited from solution on a laboratory benchtop.

In a paper published online in the journal Nature Photonics, the researchers report the first "Continuous-wave lasing in an organic-inorganic lead halide perovskite semiconductor."

An organic laser diode could have advantages. First, because organic semiconductors are relatively soft and flexible, organic lasers could be incorporated into new form factors not possible for their inorganic counterparts. While inorganic semiconductor lasers are relatively limited in the wavelengths, or colours, of light they emit, an organic laser can produce any wavelength a chemist cares to synthesise in the lab by tailoring the structure of the organic molecules. This tunability could be very useful in applications ranging from medical diagnostics to environmental sensing.

According to the researchers nobody has yet succeeded in making an organic laser diode, but the key may well involve related materials — organic/inorganic perovskites — that have gotten a lot of attention in the research community over the last few years. This hybrid material has already been responsible for a meteoric rise in the efficiency of photovoltaics.

Perovskites are fairly common minerals that share a similar cubic crystal structure. Somewhat paradoxically, one of the reasons these hybrid perovskite materials work so well in solar cells is that they are good light emitters. For that reason, they are also of interest for use in LEDs and lasers. The material Giebink and his colleagues are studying is composed of an inorganic perovskite sublattice with relatively big organic molecules confined in the middle.

In some inorganic lasers there are narrow regions called quantum wells where charge carriers can be trapped as the electrons and holes fall into the wells. The intensity of the lasing depends on how many charge carriers can be packed into the quantum wells. In the perovskite material, the arrangement of the high-temperature-phase inclusions inside the low temperature bulk seems to mimic these quantum wells and may play a role in enabling the continuous lasing.

Nevertheless, these results do point toward an opportunity to engineer a material that has the built-in qualities of this mixed phase arrangement, but without having to actually cool the material to low temperature. The current paper points to a couple of ideas for how those materials could be designed. The next big step then is to switch from optical pumping with an external laser to a perovskite laser diode that can be powered directly with electrical current.

In addition to Giebink and Jia, other contributors include Alex Grede, a graduate student in Giebink's lab, and Princeton assistant professor Barry Rand and his graduate student Ross Kerner.

The Air Force Office of Scientific Research, the National Science Foundation, DARPA and the Office of Naval Research supported this work.

"It's usually not a big leap to turn a light emitting diode into a laser." "You essentially just add mirrors and drive it harder. Once organic light-emitting diodes were invented 30 years ago, everybody thought that as soon as we had relatively efficient OLEDs, that an organic laser diode would soon follow."


"The ultimate goal is to make an electrically driven perovskite laser diode."


"That would be a game changer. It is fairly easy to make the perovskite material lase by optical pumping, that is, by shining another laser on it. However, this has only worked for very short pulses due to a poorly understood phenomenon we call lasing death. Getting it to go continuously is a key step toward an eventual electrically driven device. What we found in this recent study is a curious quirk. We can avoid lasing death entirely just by lowering the temperature of the material a little bit to induce a partial phase transition."


Chris Giebink, assistant professor of electrical engineering, Penn State

"When we lowered the temperature below the phase transition, we were surprised to find that the material initially emitted light from the low temperature phase, but then changed over within 100 nanoseconds and began lasing from the high-temperature phase — for over an hour."


"It turned out that as the material heated up, although most of the material remained in the low-temperature phase, small pockets of the high-temperature phase formed, and that was where the lasing was coming from."


Yufei Jia, a graduate student in Giebink's lab and lead author

Continuous-wave lasing in an organic–inorganic lead halide perovskite semiconductor

Yufei Jia | Ross A. Kerner | Alex J. Grede | Barry P. Rand | Noel C. Giebink

Nature Photonics 11, 784–788 (2017) | doi:10.1038/s41566-017-0047-6

Received: 15 August 2017 | Accepted: 11 October 2017 | Published online: 20 November 2017

Abstract

Hybrid organic–inorganic perovskites have emerged as promising gain media for tunable, solution-processed semiconductor lasers. However, continuous-wave operation has not been achieved so far1,2,3. Here, we demonstrate that optically pumped continuous-wave lasing can be sustained above threshold excitation intensities of ~17 kW cm–2 for over an hour in methylammonium lead iodide (MAPbI3) distributed feedback lasers that are maintained below the MAPbI3 tetragonal-to-orthorhombic phase transition temperature of T ≈ 160 K. In contrast with the lasing death phenomenon that occurs for pure tetragonal-phase MAPbI3 at T > 160 K (ref. 4), we find that continuous-wave gain becomes possible at T ≈ 100 K from tetragonal-phase inclusions that are photogenerated by the pump within the normally existing, larger-bandgap orthorhombic host matrix. In this mixed-phase system, the tetragonal inclusions function as carrier recombination sinks that reduce the transparency threshold, in loose analogy to inorganic semiconductor quantum wells, and may serve as a model for engineering improved perovskite gain media.