No jargon

Research highlights in plain language

What we found and why it matters, written for curious readers.

Artist's rendering of an exciton, drawn as a bright particle, sitting in a lattice of green electrons and lit by a laser beam.
Light creates mobile particles that become ‘dressed’ by a surrounding crystal of electrons, turning each one into a tiny sensor of the crystal’s motion.

Zhou Lab, Maryland

Taking the pulse of an electron crystal

Light-created particles let us measure how an otherwise invisible crystal of electrons vibrates, stiffens, and melts.

In earlier work, we showed that electrons can freeze into an orderly pattern known as a Wigner crystal (see Electrons crystallize!). A natural next question is how such a crystal actually behaves: how stiff it is, how much it trembles from quantum and thermal motion, and how it eventually melts. This has been hard to answer, because a crystal made entirely of electrons leaves almost no fingerprint that ordinary instruments can pick up.

In this work, we use light to create excitons (pairs of an electron and a ‘hole’) inside a semiconductor sheet only a few atoms thick. Surrounded by the electron crystal, each exciton slightly distorts the arrangement of electrons around it. As the exciton moves through the material, this distortion travels along with it, and the two together form a composite particle that we call a ‘Wigner polaron’. Wigner polarons act as tiny built-in probes: using them, we can measure the electron crystal’s stiffness and watch how it vibrates and melts, opening a new optical window into a state of matter made entirely of electrons.

The paper was published in Nature Physics, with an accompanying News & Views, and was carried out in collaboration with ETH Zurich, Brookhaven National Laboratory, and Heidelberg University. Coverage by Phys.org and Maryland Today.

Illustration of twisted WSe₂: two honeycomb atomic lattices forming a moiré pattern over a colored energy landscape, magenta arrows for the holes' spins all pointing up, black arrows running around the edge of the sample, and a red laser beam focused on one site.
One hole sits in each well of the moiré landscape (purple), all spins aligned (magenta arrows), with current flowing along the edges (black arrows). A laser (red) reads the state out.

Zhou Lab, Maryland

Seeing a topological magnet with light

Light shows that charges in a twisted semiconductor line up their spins on their own and form a quantum anomalous Hall state.

In an ordinary conductor, electrons bump into defects and lose energy as heat. In a ‘quantum Hall’ state, current instead flows without loss along the edges of a sample, protected by topology, but only in a very strong magnetic field. A ‘quantum anomalous Hall’ state does the same with no magnet, because the material supplies its own magnetism. Two slightly twisted sheets of the semiconductor WSe2 were thought to host one, but the magnetism had never been seen directly.

We use light to see it. Light creates excitons that bind to the holes (missing electrons) sitting on the moiré pattern of the twisted layers, and these ‘attractive polarons’ reveal which way the holes’ spins point. When exactly one hole sits on each moiré site, we find that the spins line up spontaneously, the hallmark of a magnet. By following how this state shifts in a magnetic field, we confirm that it is topological. A voltage across the two layers switches the system between this magnet and an ‘antiferromagnet’, in which neighboring spins point in opposite directions.

The paper was published in Physical Review X and was carried out in collaboration with the Hafezi group at UMD.

Piezoresponse force microscopy image of triangular domains and bright domain walls in twisted hexagonal boron nitride, with a 1 micrometer scale bar.
Domains and domain walls in twisted hexagonal boron nitride, imaged by piezoresponse force microscopy. The walls generate strong in-plane electric fields that can confine excitons in an adjacent layer.

Zhou Lab, Maryland

Squeezing excitons into nanoscale channels

Naturally occurring electric fields can trap excitons in channels only a few nanometers wide.

When particles such as electrons are confined in a very small space, remarkable quantum effects emerge. This is, for example, how quantum dots (the tiny light emitters in QLED televisions) get their brilliant colors. Electrons are relatively easy to confine: they carry electric charge, so electric fields can trap and steer them. Excitons are much harder. An exciton is an electron bound to a ‘hole’ (the empty spot left behind by a missing electron), and the pair as a whole carries no net charge, so electric fields have almost nothing to grab onto. Trapping excitons in spaces just a few nanometers wide is a long-standing goal, because tightly confined excitons interact strongly with one another and could serve as sources of quantum light, where light is emitted one photon at a time.

In this work, we show that excitons can be trapped by electric fields that arise naturally in a ‘moiré’ superlattice. When two layers of an insulating crystal called hexagonal boron nitride are stacked with a small twist, they form a repeating pattern of patches whose built-in electric fields point up or down, out of the layers. While this out-of-plane field is well known, it is naturally accompanied by strong electric fields lying within the plane, concentrated right at the boundaries between patches, the so-called domain walls. By placing a semiconductor sheet just a few atoms thick right above this surface, we find that excitons become trapped in narrow one-dimensional channels running along these walls. These results establish an electrical route to trapping and arranging excitons at the nanometer scale.

The paper was published in Physical Review Letters.

Scanning electron micrograph of a silver metasurface: parallel grooves roughly 150 nanometers apart, with a 250-nanometer scale bar.
A silver thin film is patterned with nanoscale grooves (imaged by scanning electron microscopy) to create an optical lattice.

Zhou Lab, Maryland

An optical lattice for excitons

A patterned metal surface squeezes light into a nanoscale lattice that can shape how excitons behave.

When two light beams cross, they interfere and create a standing wave, a regular pattern of bright and dark stripes. These standing waves are routinely used to trap atoms (known as an optical lattice), but can they also trap other particles, such as excitons (electron–hole pairs) in a semiconductor? To trap excitons in a useful way, the stripes would need to be only tens of nanometers apart. But the spacing of a conventional optical lattice, created by interference, cannot be much smaller than the wavelength of light, hundreds of nanometers, which is too coarse to strongly modify exciton behavior.

In this work, we create an optical lattice far below this so-called ‘diffraction limit’. A metal surface carved with a fine pattern (a metasurface) converts laser light into plasmon polaritons, light waves that sit on the metal surface but are squeezed to much shorter length scales. These squeezed waves allow us to imprint a fine, repeating energy landscape onto excitons in a single-layer semiconductor placed nearby. Interestingly, this scheme uses about 100 times less laser power than shining light directly on the material, offering a power-efficient route to artificial crystals for excitons and light-driven quantum matter.

The paper was published in Science Advances and was carried out in collaboration with the Hafezi group at UMD.

Illustration of light trapped between two atomically thin mirrors, each drawn as a single layer of atoms.
Two monolayer ‘excitonic mirrors’ trap light between them, forming an optical cavity only a few atoms thick.

Zhou Lab, Maryland

Trapping light with atomically thin mirrors

Two semiconductor sheets only a few atoms thick can form a complete and highly unusual optical cavity.

An optical cavity traps light by bouncing it back and forth between mirrors, so that light and matter interact far more strongly than they otherwise would. This trick is at the heart of lasers, sensors, and quantum optics. In earlier work, we showed that a single semiconductor monolayer, just a few atoms thick, can act as a near-perfect mirror (see An atomically thin mirror).

In this work, we use these atomically thin mirrors to build a complete optical cavity. Besides being extraordinarily compact, the cavity behaves in unusual ways: the trapped light forms a ‘flat band,’ meaning the photons act as though they are very heavy. With a magnetic field, the cavity can also be made ‘chiral,’ where it responds differently to light that corkscrews to the left versus to the right (circularly polarized light). Together, these features offer new ways to control light and its interaction with matter, useful for future photonic and quantum-optical devices.

The paper was published in Science Advances and was carried out in collaboration with the Hafezi group at UMD.

Illustration of a laser beam striking a stack of atomically thin layers, with charges drawn as small spheres among the atoms.
A laser creates pairs of positive and negative charges bound together in an atomically thin material. The charge pairs change how the material interacts with the laser beam.

Zhou Lab, Maryland

Strong optical nonlinearity

A little light or voltage can sharply switch how an atom-thin device absorbs and transmits light.

When light shines on a semiconductor, it kicks electrons into higher energy states, leaving behind positively charged ‘holes’ that pair up with electrons to form excitons. While these excitons ‘live’ inside the material, they can alter its optical response, allowing a light beam’s shape, direction, or color to change in a ‘nonlinear’ way, meaning the response is not simply proportional to how much light you put in.

In this work, we demonstrate a strong and tunable nonlinear response in a device made of three atom-thin layers of the semiconductor tungsten diselenide. Remarkably, even a small amount of laser light can dramatically change the material’s behavior, switching it from absorbing light to letting light through. The effect can also be turned on and off with a voltage. This discovery opens a powerful new platform for advanced optical and quantum technologies.

The study was published in Nature Photonics and carried out in collaboration with the Hafezi group at UMD and the QPress facility at Brookhaven National Laboratory.

Two photoluminescence maps of interlayer excitons at low and high laser power; at high power the emission spreads across the outlined device. Scale bar 2 micrometers.
Map of the light emitted by interlayer excitons in a MoSe2/hBN/MoSe2 device; the dashed line marks the sample boundary. Created by a focused laser, the long-lived excitons spread over micrometers before recombining.

Zhou Lab, Maryland

Controlling bright, long-lived excitons

A three-layer structure makes excitons bright, long-lived, and electrically movable—ingredients needed for collective quantum states.

When certain quantum particles (so-called bosons) are cooled and crowded together, they can lock into a single collective state, a Bose–Einstein condensate. This has been achieved with atoms, and theory predicts that excitons, bound electron–hole pairs in a semiconductor, could condense at far higher temperatures. The catch is that an exciton usually vanishes quickly, as its electron and hole recombine and emit light, before enough of them can gather to condense.

‘Interlayer’ excitons, with the electron in one atom-thin layer and the hole in a neighboring one, live much longer, but they are usually also much dimmer. Here we sandwich a single sheet of insulating hexagonal boron nitride between two layers of the semiconductor MoSe2: thick enough to keep the charges apart, yet thin enough that they remain tightly bound and bright, even at higher temperatures and densities. A voltage across the stack tunes the excitons’ energy over a wide range and can push them across the device, giving us an electrical handle on a dense cloud of interlayer excitons and a promising platform for an exciton condensate.

The paper was published in Physical Review Letters and was carried out in collaboration with the QPress facility at Brookhaven National Laboratory.

Illustration of two interlocking triangular lattices of electrons, one violet and one gold, stacked as a bilayer crystal.
Wigner crystals made of two layers of electrons.

Postdoctoral work, Harvard

Electrons crystallize!

Electrons in two atom-thin layers can lock together into a stable, ordered crystal.

Crystals are made of atoms arranged in a regular pattern. In the 1930s, the physicist Eugene Wigner predicted that electrons themselves could also form such patterns, now called Wigner crystals. These crystals are very difficult to create because electrons are extremely light, and without chemical bonds to hold them in place, they tend to move around a lot, both from quantum effects (the uncertainty principle) and from heat.

In our work, we show that stacking two atomically thin semiconductor layers close together creates electric forces strong enough to hold Wigner crystals in place. Electrons in the two layers interlock to form a ‘bilayer’ Wigner crystal that is remarkably stable and has an intriguing stacking pattern. This system is an excellent playground for exploring how these electron crystals change, or ‘melt,’ when shaken by heat and by quantum fluctuations.

The study was published in Nature and carried out in collaboration with the Park, Kim, Lukin, and Demler groups at Harvard. Coverage by Quanta Magazine.

Schematic of a van der Waals heterostructure suspended over a gold mirror under a gate voltage, with photoluminescence maps at 0 and minus 150 volts.
The light emitted by monolayer MoSe2 is modulated as we reversibly change the distance between the semiconductor and a mirror.

Postdoctoral work, Harvard

Mechanical tuning of light–matter interactions

Moving an atom-thin semiconductor closer to or farther from a mirror controls how strongly it emits light.

An atom, molecule, or other ‘emitter’ holding extra energy can release it as light, a process called spontaneous emission that makes LEDs and fluorescent lamps glow. It is tempting to think that how fast an emitter gives off its light is fixed by the emitter itself. In fact it also depends on the emitter’s surroundings, and shaping those surroundings with carefully designed optical structures, such as cavities and photonic crystals, has become a cornerstone of modern optics.

In this work, we control the light emission of excitons (bound electron–hole pairs) in an atomically thin semiconductor using nothing more than a simple mirror. By moving the semiconductor toward or away from the mirror, we change the excitons’ surroundings and substantially modify how much light they emit. We show that this control can even happen in real time, which could lead to new applications in both classical and quantum optical information processing.

The paper was published in Physical Review Letters and was done in collaboration with the Kim and Lukin groups at Harvard.

Thermal camera images of sapphire, fused silica, and samarium nickelate from 100 to 140 degrees Celsius; only the nickelate's apparent temperature stays nearly constant.
Unlike normal materials, thermal radiation from samarium nickelate does not change significantly as its temperature rises.

Doctoral work, Harvard

Unusual thermal radiation

A material can heat up without appearing much hotter to an infrared camera.

All matter emits thermal radiation above absolute zero temperature (also known as ‘blackbody radiation’). Normally the hotter an object gets, the more thermal power it radiates, which is the principle behind infrared thermal imaging.

In this work, we show that an oxide called SmNiO3 breaks this basic rule: its thermal radiation barely changes as it heats up. The trick is a metal–insulator transition, a switch between conducting and non-conducting states. As the temperature rises, the material becomes more metal-like in just the right way to make it look cooler than it actually is, canceling out the usual increase in glow. This effect could enable new technologies for thermal camouflage (hiding from infrared cameras) and heat management.

The paper was published in Proceedings of the National Academy of Sciences with the Kats group at Wisconsin, and was highlighted by the Department of Energy.

Schematic of light reflecting from a MoSe2 monolayer between hBN layers, with optical and reflection images of the sample.
A monolayer of MoSe2, containing merely three layers of atoms, can act as a highly reflecting mirror thanks to the excellent coherence of its excitons.

Postdoctoral work, Harvard

An atomically thin mirror

A semiconductor just three atoms thick can reflect nearly all light of the right color.

Metals reflect light but become transparent if thinned down to less than tens of atoms thick. So ultimately, how thin can a mirror be? Can we make mirrors made of just a few layers of atoms?

One way to do this is to use a ‘resonance’ effect. Light of just the right color can make a material buzz with optical excitations. If those excitations release all their stored energy back as light, then all the incoming light is reflected, because the re-emitted light and the incoming light add up to send the beam straight back. In practice, though, some of that energy usually leaks away as heat, so the light ends up absorbed instead of reflected.

In this work, we show that in high-quality sheets of the semiconductor MoSe2, the excitons get rid of their energy almost entirely by emitting light (rather than losing it as heat) when the material is very cold. As a result, these sheets, though only three atoms thick, can act almost as a perfect mirror, and their reflection can be switched on and off with a voltage. This is about as thin as a mirror can get, and it opens up unique applications, from nonlinear quantum optics to metasurfaces (flat, patterned surfaces that steer light).

This paper was published in Physical Review Letters and was done in collaboration with the Kim and Lukin groups at Harvard. Coverage by Physics, Nature, and Chemistry World.

Schematic of a two-dimensional semiconductor on a silver surface, with a dark exciton coupling to a surface plasmon polariton.
By bringing a two-dimensional semiconductor, WSe2, close to an ultra-flat metal surface, we enhance and directly probe the emission of the nominally spin-forbidden dark excitons.

Postdoctoral work, Harvard

Seeing the dark states

An ultra-flat metal surface makes normally hidden, long-lived excitons bright enough to measure.

Excitons, bound electron and hole pairs, are an elementary optical excitation of semiconductors. Inside an exciton, the spins of the electron and hole can be either parallel or antiparallel. Excitons with antiparallel spins (bright excitons) can quickly decay by emitting light, while those with parallel spins do not usually emit light. These so-called ‘dark excitons’ are attractive for information processing because they live longer than bright excitons, but they are also harder to study experimentally.

In this work, we introduce a way to detect dark excitons in an atom-thin sheet of the semiconductor WSe2 by placing it right next to a metal surface. Near the metal, the dark excitons couple strongly to ripples of electrons and light that ride along the metal’s surface (called surface plasmon polaritons). This coupling boosts the dark excitons’ light emission enough that we can finally measure it. The method gives scientists a much better handle on studying and controlling excitons, opening new possibilities for metasurfaces and optoelectronics (electronics that work with light).

This work appeared in Nature Nanotechnology and was done in collaboration with the Kim and Lukin groups at Harvard, with a News & Views in Nature Nanotechnology.

Schematic of a fuel cell with a nickelate electrolyte that conducts protons but blocks electrons, beside photographs of microfabricated cells.
In the new electrolyte, ionic conduction is sustained by protons while electronic conduction is blocked by a fuel-induced metal–insulator transition, enabling high-performance low-temperature solid oxide fuel cells.

Doctoral work, Harvard

New design rules for fuel cells

A fuel-cell material can carry useful ions while automatically blocking wasteful electron flow.

Fuel cells can generate electricity by oxidizing fuels in an environmentally friendly fashion. The electrolyte, the component of a fuel cell that separates the fuel from the oxidizer, needs high ionic conductivity but low electronic conductivity. Typically ionic conduction in a solid electrolyte is created by vacancies (missing atoms) in the lattice. These missing atoms, however, also often create electronic conduction, leading to efficiency loss or even catastrophic failure of fuel cells.

In this work, we report a completely new way to design the electrolyte, using a quantum material called SmNiO3. Unlike most materials, SmNiO3 becomes far better at blocking electrons once it soaks up hydrogen from the fuel, thanks to a metal–insulator transition (a switch from conducting to non-conducting). At the same time, it stays very good at carrying ions, on par with the best electrolytes at similar temperatures. That combination, blocking electrons while passing ions, is exactly what a fuel cell needs, so this result points to better low-temperature fuel cells and new rules for designing energy materials.

The paper appeared in Nature, with coverage by Nature Energy, Harvard, Argonne National Laboratory, IEEE Spectrum, and National Science Review. This work was done in collaboration with the groups of H. Zhou and D. Fong at Argonne.

Artist's rendering of a brain, one half drawn as circuitry and the other as coloured neurons.
Strongly correlated materials show promise for future memory and neuromorphic devices.

Doctoral work, Harvard

Brain-inspired computing devices

Materials that switch between states could help computers process information more like the brain, using far less energy.

‘Brain-inspired’ computing, using artificial neural networks, has driven huge progress in artificial intelligence, including image and speech recognition. Run on ordinary digital computers, though, these programs use far more power than a real brain, which is a big problem for battery-powered devices like phones. Building computer chips that imitate the brain directly in the hardware could make this kind of computing much more energy-efficient.

Here we review progress towards building such hardware, neuromorphic devices and circuits, using correlated materials and their phase transitions, with particular emphasis on materials synthesis and device physics, and critically evaluate their prospects.

The paper was published in Proceedings of the IEEE.

Crystal structure of samarium nickelate beside photographs of a film switching from an opaque metal to a transparent insulator when electrons are added.
Electron doping turns SmNiO3 from a reflective metal to a transparent insulator at room temperature, opening new directions for electronics and optics.

Doctoral work, Harvard

New metal–insulator phase transitions

Adding electrons can turn a shiny conducting oxide into a transparent insulator at room temperature.

Being able to dramatically change a material’s properties by switching its ‘electronic phase’ (see the post below) could open the door to many new electronic and optical devices.

Here we report the discovery of a new type of metal-to-insulator transition in an oxide material, SmNiO3, driven by electron doping. The oxide turns from a shiny metal to a transparent insulator when doped with lithium ions or protons. Its electronic conductivity changes by more than eight orders of magnitude, among the highest ratios achieved in phase-change materials at room temperature. We attribute the transition to a Mott transition driven by a quantum mechanical effect called electron correlation. Such a drastic phase transition forms an emerging platform for studying many-body physics and for realizing oxide-based reconfigurable electronic and optical devices.

The paper was published in Nature Communications with coverage from Harvard and Phys.org.

Schematic of a device switching from insulator to metal under a nanosecond voltage pulse.
Using an electrical pulse, we can switch an insulating material into a metal within nanoseconds.

Doctoral work, Harvard

Ultrafast metal–insulator transitions

A short electrical pulse can switch vanadium dioxide from an insulator to a metal within billionths of a second.

Electrons can move freely in a metal but not so in an insulator. Intriguingly, certain materials can switch between being a metal and an insulator depending on external conditions, just as water can change its phase between solid, liquid, and gas. Perhaps the most famous material hosting such metal–insulator transitions is vanadium dioxide, whose electrical and optical properties change dramatically when heated above 68 °C. This phase change, if triggered electrically, may enable a range of new electronic and optical devices.

Here, by optimizing materials growth and device structures, we are able to trigger the phase change in VO2 with a voltage within a few billionths of a second, the fastest achieved electrically at the time. Such a study of the dynamics of the phase transition not only forms the foundation for new electronics and optics, but can also help to resolve the long debate over the mechanism of the VO2 transition initiated by J. B. Goodenough and N. F. Mott.

The paper appeared in IEEE Electron Device Letters and was done in collaboration with Micron Technology. See the related discussion in Nature.