My research interests are broad, and nearly any topic related to stars or planets is fascinating to me. Although I'm a theorist, I tend to work on problems related to observational puzzles. Much of my work focuses on fluid dynamics within stars and planets, and my methods include a variety of analytical and numerical techniques coupled with sophisticated stellar evolution codes. You can learn more about my research at the links provided below.

Saturn Ring Seismology

Seismology is our most powerful tool for understanding the interiors of stars and planets. Indeed, our knowledge of the interior structures of the Earth and Sun owes its existence primarily to seismic measurements. Unfortunately, remotely detecting seismic disturbances on planets other than the Earth is very difficult, and until recently such a feat had never been achieved. Intriguingly, Saturn offers an unprecedented opportunity to observe seismic oscillations through their gravitational interactions with Saturn's rings. Recent observations of Saturn's ring system have revealed the presence of density waves within the rings excited by global oscillation modes of Saturn. Hedman & Nicholson (2013) used observations of Saturn's rings with the Cassini satellite to measure the frequencies of the waves in the rings, thereby precisely measuring a small set of the planet's mode frequencies. These observations reveal the presence of unexpected planetary oscillation modes, finely split in frequency from those expected, and whose presence may shed new light on Saturn's interior structure.

Above: Animation of an oscillation mode of Saturn creating waves in the rings. Credit: Robert Hurt

Below: Cartoon of the interior structure of Saturn inferred from my seismic analysis.

My group's work has focused on the origin of the unexpected oscillation modes of Saturn, and to understand their implications for its structure. Along with postdocs Chris Mankovich and Janosz Dewberry, we have constructed planetary models and computed the corresponding mode frequencies, comparing them with the observed mode frequencies. The frequencies of the modeled fundamental modes match the observed frequencies to an accuracy of roughly 1%. The additional unexpected modes only exist in models containing a large stably stratified (non-convective) planetary core. The stable stratification allows for the presence of gravity modes which can mix with the fundamental modes to obtain a detectable influence on the rings. Saturn's core must be diffuse or "fuzzy", containing a gradual transition from a gaseous envelope to a icy/rocky core.

Here are our articles on the subject:

  • Saturn IV
  • Saturn III
  • Saturn II
  • Saturn I
  • Pre-Supernova Outbursts

    Massive stars explode as supernovae when they die, but historically they were not predicted to give any warning signs that they are about to explode. However, observations of many types supernovae now show evidence for mass loss or eruptions from the star in its final years of life. In a few cases, these outbursts have been observed directly. These eruptions may be linked to evolution in the core of the star, where the nuclear energy generation rate increases by a factor of roughly one million over the last decades of the star's life. However, most of this nuclear energy escapes in neutrinos, and photons in the core of the star cannot diffuse to the surface before the star explodes, so another form of energy transport would be needed to link nuclear energy generation in the core with an outburst at the surface of the star.

    My group has examined the role of energy transport by hydrodynamic waves that are excited as a byproduct of the core convection associated with energetic nuclear burning. Our work shows these waves can carry a small fraction of the nuclear energy toward the surface of the star, and that waves can become the dominant form of energy transport in the last years of a star's life. The waves damp and deposit heat in the envelope of the star, which can cause the star to become much brighter at its surface and generate a pre-supernova outburst. The density structure of the star may also be affected, which will alter the appearance of the subsequent supernova.

    Above: Cartoon picture showing how waves excited in the core of a star can travel into the envelope of a star, where they deposit enough energy to power an eruption from the surface of the star.

    Below: Movie showing how the structure of a red supergiant might evolve in its final years of life before it goes supernova. The color shows the density of the star: its core contains nearly half its mass but is too small to see at this scale.

    Here are our recent articles on the subject:

  • The appearance of Supernovae with Pre-Supernova Outbursts
  • Simulations of Pre-Supernova Outbursts
  • The Energy Budget of Pre-Supernova Outbursts
  • Pre-Supernova Outbursts in Helium Stars
  • Pre-Supernova Outbursts in Red Supergiants
  • Tidal Migration of Moons and Exoplanets

    Just as our own moon is slowly moving away from the Earth, the moons of Jupiter and Saturn have slowly migrated outward over the history of the solar system. Recent measurements from have revealed that Saturn's moons are currently migrating much faster than astronomers had guessed, including its largest moon Titan. The rapid migration leads to tidal heating of the moons and helps explain why Saturn's moon Enceladus is volcanically active.

    Here is the discovery of the outward migration of Titan:

  • Titan's Migration
  • My research has attempted to explain the rapid migration (and predicted it for Titan) through a process called resonance locking. In this scenario, moons get trapped in resonances with oscillation modes of their host planets. As the planets evolve, the resonant semi-major axes associated with the oscillation modes can move away from the planet, carrying moons with them. The migration of the moons is therefore determined by the thermal evolution of the planet, which proceeds on a timescale shorter than conventional ("constant Q") tidal migration, and hence the moons migrate faster than expected.

    Above: Animation showing how a moon can "surf" a resonance lock outward.

    Below: The difference in migration histories of the moons according to standard (constant Q) tidal theories and the resonance locking theory. Unlike standard tidal theories, resonance locking is compatible with the contemporaneous formation of Saturn and its moons.

    Here is the paper predicting outward migration of Titan:

  • Resonance Locking
  • Click below for a cool movie describing some related work:

  • Encelade Team
  • Just as planetary moons can migrate via resonance locking, so can exoplanets that are close to their host stars. In this case, the exoplanets usually orbit faster than the star rotates, causing the planet's orbit to decay at about the same rate that the star evolves. This can cause the orbital evolution to be much faster (or slower) than predicted by other theories, and has a unique imprint on the distribution of exoplanet orbital periods.

    Above: As a star evolves, its oscillation mode frequencies increase with time, sweeping up nearby planets and causing them to migrate inwards, toward their impending doom.

    Here is our recent article on the subject:

  • Exoplanet Migration
  • Uncovering Stellar Mergers with Asteroseismology

    About one out of every ten stars merges with another star during its lifetime. However, identifying stars that have already merged with a companion can be difficult if you don't know what to look for. My group has bee predicting the affect on the structure of the star, and how this imprints the fingerprint of a prior merger in the asteroseismic pulsation spectrum of a red giant star. By looking for this fingerprint amongst asteroseismic catalogs, we have identified a couple dozen red giant stars that likely underwent a merger in their recent past.

    Above: Stars that merge on the red giant branch have dense, degenerate, undermassive cores compared to single stars or stars that merge on the main sequence. This means their asteroseismic period spacing is smaller than expected for their mass, allowing them to be identified.

    Here is our recent article on the subject:

  • Asteroseismic Fingerprints
  • Tidally Trapped Pulsations

    For a star in a close binary system, the tidally distorted shape acts like a lens that focuses pulsations in the star. Unlike single stars, the pulsations of these stars can be localized to one side of the star and aligned with the tidal axis, such that the amplitude of the pulsation is modulated over the orbital period. Several such systems have now been found, and I have been working to understand the physics of these tidally trapped pulsations.

    Below: A model of the binary system TIC63328020, which contains a tidally trapped pulsation aligned with the axis connecting the two stars. The colors represent flux perturbations produced by the pulsation as it propagates around the pulsation axis.

    Merging White Dwarfs

    White dwarfs with short orbital periods emit gravitational waves, which causes the orbit to decay until the white dwarfs merge or begin mass transfer. Much of my graduate work focused on the tidal interactions in the white dwarfs before they merge, which effect the outcome of the merger or mass transfer process. Along with Kevin Burdge and Tom Prince, we are now finding these binary white dwarfs with ZTF, allowing for a new understanding of the population of merging white dwarfs. The movie above depicts the recently discovered system J1539+5027, the shortest period eclipsing binary star known, with an orbital period just under seven minutes.

    Movie made by Robert Hurt.

    Here are a couple recently discovered white dwarf binary systems:

  • 7-minute binary
  • 20-minute binary
  • The image below shows my inner artist's conception of the J0651 binary white dwarf system, which has an orbital period of just 12.75 minutes. The sizes/separations of all objects below are shown to scale! These systems are placing new constraints on tidal spin-up and heating of the white dwarfs, in addition to the physics of binary stars that gives rise to these systems.

    Compact Object Rotation

    Above: Animation of a differentially rotating star, where inner layers rotate faster than the outer layers. This shear creates instabilities that act like friction and bring the star closer to a rigidly rotating configuration.

    The rotation rates of compact objects (such as white dwarfs, neutron stars, and black holes) are determined by the angular momentum inherited from the progenitor star. It is the rotation rates of the cores of these stars (which are difficult to measure) that are most important, but these rotation rates are determined by uncertain processes that redistribute angular momentum within stars as they evolve. Fortunately, asteroseismic observations have recently directly measured the core rotation rates of many stars, allowing us to develop a better theoretical understanding of the physical mechanisms at work.

    Along with collaborators Tony Piro, Adam Jermyn, and Linhao Ma, we have investigated angular momentum transport due to magnetic torques caused by the Tayler instability. We have found that these torques predict internal rotation rates roughly consistent with those measured by asteroseismology. We are now making predictions for the spins of neutron stars and black holes, finding that these compact objects may be born spinning much slower than prior expectations.

    Here are my group's recent articles on the subject:

  • Slowing Stellar Spins
  • Black Hole Spins
  • Neutron Star Spins
  • Magneto-asteroseismology

    Magnetic fields are an important but poorly understood aspect of stellar evolution. In the past, our inability to measure magnetic fields within stars has hampered the development of a coherent picture of stellar magnetism. Now, asteroseismology is offering the first glimpses of magnetic fields within stars. In red giant stars, pulsations at the surface of the star are created by waves that travel from the surface of the star, into its core, and back to the surface.

    Above: Animation showing the ray path of a wave propagating in a red giant.

    Below: Cartoon illustrating the trapping of a wave within a red giant with a magnetized core, referred to as the magnetic greenhouse effect.

    If a strong magnetic field lurks within the star's core, the picture changes. When the wave encounters the strong magnetic field, it is redirected by magnetic tension forces. This changes the nature of the wave, such that it can no longer escape from the star's core and propagate back to the surface. The loss of the wave energy at the surface of the star results in a decreased stellar pulsation amplitude, signaling the presence of a strong magnetic field in the star's core. This effect is observed in roughly one out of five red giants, whose cores contain magnetic fields thousands to millions of times stronger than typical refrigerator magnets!

    An open access link to the published article can be found at the

  • Authorea portal
  • See also
  • Red Giant Magnets
  • Neutron Star Spin

    Pulsars are rotating neutron stars whose spin periods can be very accurately measured via radio pulses emitted when the star's magnetic field points toward the Earth. Most pulsars rotate with periods of roughly one second, but we have a poor understanding of what determines the rotation rate of a pulsar as it is first born during a supernova explosion. My work has focused on the final days and hours of a stars life, during which nuclear burning proceeds so rapidly that the star's core is irradiated by waves launched by extremely vigorous convection. These waves are powerful enough to change the spin direction and spin rate of the core, such that its spin undergoes a random walk. The spin period of the core at the end of the random walk (when the supernova occurs) is tantalizingly similar to that needed to match the observed spin periods of young pulsars!

    Above: Animation of the spin-up of a massive stellar core (here made to look like the Earth). The direction of the rotation axis varies randomly, although on average the spin frequency slowly increases in time.

    Below: The distribution of expected spin periods of a massive stellar core just before core-collapse (bottom axis) and soon after neutron star formation (top axis).

    My article on the subject:

  • NSspin
  • Heartbeat Stars

    Click Here for Interactive Model of KIC 8164262!!!

    Heartbeat stars are an emerging class of eccentric short-period binary stars. The characteristic "heartbeat'' signal evident in their light curves is produced by a combination of tidal distortion, reflection, and Doppler boosting near orbital periastron. Many heartbeat stars continue to oscillate after periastron, indicative of the tidal excitation of oscillation modes within one or both stars. These systems are among the most eccentric short period binaries known, and they constitute an exciting opportunity to observe and understand tidal effects in action.

    The video above shows an animation of the orbit of the heartbeat star KOI-54. The bottom panel shows the light curve, which contains a spike near periastron (due to the effects listed above) and oscillations away from periastron due to tidally excited stellar oscillations modes. The stellar oscillations cuase the stars to dissipate orbital energy, causing their orbit to slowly circularize. My research seeks to understand the tidally excited oscillations and their effect on the orbital evolution of eccentric binary stars.

    What would a heartbeat star sound like? Click below to find out! To generate this "sound curve", I have converted the light curve (measured by Kepler) into a sound byte, and sped it up by a factor of 5 million. The "heartbeat" sound you'll hear is produced by the tidal distortion, reflection, and Doppler boosting at periastron. The steady tone is produced by the tidally excited oscillations.

    Hear the Heartbeat!

    Here is an article on the subject:

  • KOI-54
  • Stay tuned, more work on heartbeat stars is underway!

    Tides in Triples

    In addition to finding planets, the Kepler satellite uncovered a bunch of very interesting stellar systems. One such system is HD 181068, aka, "Trinity", which is composed of a red giant primary star orbited by a pair of K dwarf stars. The dwarf stars orbit each other every 0.9 days, and their center of mass orbits the red giant every 45 days. The animation below depicts the system, with all sizes and orbital periods shown to scale.

    HD 181068 also shows a type of stellar pulsation never observed before. The motion of the K dwarfs around each other causes the red giant to feel a changing gravitational field. The force from this gravitational field excites oscillations within the red giant, which can be detected by the Kepler satellite. Because the K dwarfs orbit each other very fast, their motion excites sound waves, or p-modes, within the red giant. This is the first star system in which p-modes have been observed to be excited by companion stars.

    Here is my article on the system:

  • HD 181068
  • Supernova Seismology

    If the core of a massive star is rapidly rotating just before the star dies, its collapse into a neutron star will occur faster along the poles than it will along the equator. This asymmetry causes the neutron star to be born rapidly oscillating. These oscillations create gravitational waves whose frequencies depend on the properties of the neutron star. The detection of these gravitational waves is possible for a supernova within the local group of galaxies, and could be used to learn about the extreme conditions within newborn neutron stars. My work presents semi-anlaytic calcultions to explain the amplitudes and frequencies of the gravitational waves generated during the supernova, in addition to their lifetime. I find that the amplitude of the gravitational waves decays on timescales of about 10 ms as fluid motions generated by the oscillating neutron star carry energy outwards into the surrounding supernova material.

    Above: Rapidly rotating core-collapse simulation (created by collaborators Hannah Klion, Ernazar Abdikamalov, and Christian Ott) showing the oscillating proto-neutron star. The associated gravitational wave signal is shown by the lower curve.

    Below: The timescale on which the energy contained in the proto-neutron star oscillations leaks into the surrounding supernova. The peak at 770 Hz is created by the fundamental oscillation mode of the neutron star, which is responsible for the bulk of the gravitational wave emission.

    My article on the subject:

  • Supernova