Highlights of Recent Research

Little Red Dots (2026)

JWST has uncovered an abundant population of compact red sources in the early Universe whose nature remains uncertain. Could these little red dots be hydrogen-burning stars with masses hundreds of thousands of times that of the Sun? We explore how metal-enriched supermassive stars develop inflated, cool envelopes and eventually collapse into seeds of supermassive black holes.

Inflated Supermassive Stars as Little Red Dots and Progenitors of Supermassive Black Holes
Wenbin Lu · 2026 · Preprint

Hertzsprung–Russell diagram showing stellar luminosity versus effective temperature for five metallicities. At high masses, the more metal-rich sequences extend toward cooler temperatures; the Z = 0.01 sequence reaches the shaded region labeled LRDs.
Stellar models in the luminosity–temperature plane. At sufficiently high masses, luminosities approach the Eddington limit, making the outer envelope structure highly sensitive to metallicity-dependent opacity. More metal-rich stars develop much more extended envelopes. For near-solar metallicity (metal mass fraction Z ≈ 0.01), the envelope expands until the photosphere reaches hydrogen recombination temperatures, forming a cool branch qualitatively similar to the observed little red dots (shaded region). Models for low-mass stars (M ≤ 100 solar masses) are taken from the MIST zero-age main-sequence (ZAMS) models.

What’s found

We construct models of supermassive stars in hydrostatic and thermal equilibrium. Their interiors contain a hot, nuclear-burning core surrounded by an envelope whose structure depends strongly on metallicity. Enhanced opacity can inflate the envelope, allowing metal-rich models to reach surface temperatures near 7,000 K.

The maximum stable mass is of the order $10^6 M_\odot$ (depending on core rotation). As the stars exhaust hydrogen on a timescale of the order 1 Myr, they can become unstable under general relativity and collapse into massive black holes.

Why it matters

This interpretation could connect little red dots to the formation of supermassive black holes. Cool stellar photospheres naturally produce observed rest-frame optical emission, while the predicted maximum luminosity is comparable to the observed bright-end luminosity function cutoff.

The strongest support for this model comes from the abundance of little red dots. Combined with a supermassive star’s nuclear lifetime of ~1 Myr, their observed number density predicts the number density of present-day supermassive black holes to within a factor of order unity, assuming that each little red dot leaves a black hole retaining most of the stellar mass.

Testing this picture requires more detailed calculations of the emergent spectra, especially the Balmer features and effects of departures from local thermodynamic equilibrium.

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Luminous Fast Blue Optical Transients (2026)

What powers AT2018cow’s UV/optical emission many years after the explosion, and can it reveal the central compact object’s mass? We show that a super-Eddington disk wind allows a broad range of accretor masses, distinguishable through infrared observations.

Implications of the UV/optical Plateau of AT2018cow
Wenbin Lu and Anthony L. Piro · 2026 · Preprint

Two-panel spectral comparison. Models spanning different accretor masses overlap at the Hubble ultraviolet and optical measurements but separate in the infrared. The right panel compares hydrogen-rich and hydrogen-poor winds for 1.4- and 10-solar-mass accretors. Magenta triangles mark JWST sensitivities.
Model spectra compared with AT2018cow’s late-time data by Hubble and XMM-Newton (upper limit). Different accretor masses can produce similar UV/optical emission but diverge in the infrared. The right panel highlights the dependence on mass and wind composition. Magenta triangles indicate JWST 5σ sensitivities for 10 ks exposures.

What’s found

We model a super-Eddington disk wind together with irradiation of the outer disk. Fits to Hubble photometry allow accretors from a $1.4M_\odot$ neutron star to a $\sim100M_\odot$ black hole. The wind’s color temperature depends weakly on mass, making these models difficult to distinguish in the UV/optical.

Why it matters

The plateau alone does not establish an unusually massive black hole. Infrared free-free emission and recombination lines offer tests of accretor mass and wind composition. The inferred disk properties are consistent with disruption of or merger with a companion star.

Earlier in Tsuna & Lu (2025), we propose a micro-tidal disruption event following a stripped-envelope supernova: a natal kick sends the newborn neutron star or black hole into its companion, disrupting it. Accretion of the stellar debris drives a powerful wind that collides with the supernova ejecta, providing a possible engine for LFBOTs.

For a broader introduction, our review Ho & Lu (2026) summarizes LFBOT observations, proposed origins, and promising ways to distinguish the models.

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Binaries in galactic nuclei and chaotic tides (2026)

A massive black hole can tear a stellar binary apart, ejecting one star at high speed and capturing the other. What happens during the many passages before breakup? We show how repeated perturbations excite chaotic stellar oscillations, tightening binaries and creating a channel for exceptionally fast escaping stars.

Formation of Close Binaries through Massive Black Hole Perturbations and Chaotic Tides
Howard Hao-Tse Huang and Wenbin Lu · 2026 · The Open Journal of Astrophysics

Schematic of a stellar binary orbiting a massive black hole. Outer-orbit relaxation and precession accompany black-hole perturbations of the binary eccentricity. Red arrows connect chaotic tidal growth at close stellar encounters to rapid circularization and formation of a close binary.
A stellar binary repeatedly passes near a massive black hole while its outer orbit evolves through relaxation and precession. Black-hole perturbations can increase the binary’s eccentricity until the stars pass within a few stellar radii of each other. Chaotic tidal excitation then removes orbital energy, rapidly shrinking and circularizing the binary.

What’s found

We model repeated black-hole perturbations together with tidal interactions between the two stars. The perturbations can drive the binary to highly eccentric orbits, bringing the stars within a few stellar radii of each other. Their oscillations then grow chaotically, draining energy from the orbit and rapidly shrinking the binary.

In the modeled regime where binaries approach the tidal breakup boundary gradually (so-called “empty loss-cone”), up to half of initially wide binaries become close binaries instead of being disrupted while still wide. Their separations can shrink to less than ~10 stellar radii.

Why it matters

This mechanism creates close binaries in galactic nuclei and provides a channel for producing the fastest hypervelocity stars when the tightened binaries eventually break apart. It also connects binary evolution near massive black holes to repeating partial tidal disruptions and quasi-periodic eruptions. The fraction that undergoes this process depends on the initial binary properties and orbital environment.

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Fast X-ray Transients (2026)

Can we identify neutron star mergers promptly when their narrow gamma-ray burst jets point away from us? We show that cooling of the jet-driven cocoon can produce a brief soft X-ray flash for off-axis observers, even when the gamma-ray burst is missed.

First Light of Neutron Star Mergers: Off-axis Cocoon Cooling X-ray Emission from Short Gamma-Ray Burst Jets
Jian-He Zheng and Wenbin Lu · 2026 · Accepted; arXiv preprint

Six simulation snapshots showing the energy density of a jet and its surrounding cocoon from 0 to about 1,000 seconds in the lab frame. Black solid and green dashed curves mark the photospheric and diffusion radii in the last three panels.
A jet propagating through neutron star merger ejecta creates a hot cocoon that expands beyond the ejecta. Colors show logarithmic energy density; black solid and green dashed curves mark the photospheric and diffusion radii. The six snapshots follow the lab-frame evolution to roughly 1,000 seconds, when cooling radiation can escape.

What’s found

We simulate a short gamma-ray burst jet propagating through merger ejecta and follow the surrounding cocoon to the radius where photons diffuse out. Its cooling produces soft X-ray flashes lasting a few to ten seconds for off-axis observers. In our canonical model, Einstein Probe could detect a GW170817-like event at viewing angles up to 45 degrees, and events with smaller viewing angles of 10 degrees can be detected up to a distance of 1 Gpc.

Why it matters

These flashes could trigger rapid follow-up even without a detectable gamma-ray burst. Subsequent kilonova and jet-afterglow observations would test the merger interpretation. This is a predicted counterpart whose detectability depends on the jet power, ejecta density profile, and viewing angle.

This work extends our studies of jet-driven cocoons in stellar explosions. In Zheng & Lu (2026), we show that cooling cocoons from long gamma-ray burst jets viewed off axis can produce fast X-ray transients without detectable gamma-ray counterparts. In Zheng et al. (2025), we model EP240414a as an off-axis jet–cocoon system, connecting its X-ray flash, optical emission, and radio afterglow to a stellar explosion.

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Ultra-long-period Pulsars (2026)

Some radio sources pulse only once every few minutes or hours. If they are neutron stars, how did they reach such long spin periods? We propose that gas captured from a supernova-shocked companion forms a disk that rapidly brakes the newborn neutron star.

Accretion from a Shock-inflated Companion: Spinning Down Neutron Stars to Hour-long Periods
Savannah Cary, Wenbin Lu, Calvin Leung, and Tin Long Sunny Wong · 2026 · The Astrophysical Journal, 996, 141

Six period–period-derivative diagrams show modeled neutron stars evolving from birth to one million years. Colored points indicate initial magnetic field strength, while gray points and symbols show observed pulsars and magnetars. Strong-field models evolve toward very long spin periods.
Evolution in spin period P and period derivative P-dot. Colored points show model neutron stars at six ages, with color indicating initial magnetic field strength; gray symbols show observed sources. Interaction with an accretion disk rapidly spins down strongly magnetized neutron stars, producing a long-period population.

What’s found

We simulate a supernova in a close binary and show that the newborn neutron star can capture gas from its shock-inflated companion. The captured gas forms a disk. During a brief “propeller” phase, the rotating magnetosphere expels disk material and loses angular momentum, rapidly slowing the neutron star.

Our models produce both ordinary pulsars and ultra-long-period neutron stars. The longest periods require strong initial magnetic fields, typically above $10^{14}$ G.

Why it matters

This channel links binary stellar evolution to ultra-long-period pulsars. It offers a formation mechanism for slowly rotating neutron stars, while the origin of their radio emission remains a separate question.

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