I'm a computational biophysicist working at the intersection of protein physics, soft matter, and tissue mechanics. I received my Ph.D. in computational biology and bioinformatics from Yale University in 2024, advised by Corey O'Hern. My doctoral work was in equal parts protein structural informatics and soft matter physics. Since 2024, I have been a postdoctoral researcher in the Syracuse Physics Department, working with M. Lisa Manning. In collaboration with Alessandro Mongera, we have developed new discrete element models for dynamic and sparse tissues under tension. See below for highlights of my work and my CV.
Protein cores all pack to the same density (φ ≈ 0.55), but there has been no physical explanation for why. We show this value marks the onset of a jamming transition: as hydrophobic interactions drive collapse, the core undergoes a floppy-to-rigid transition with the same power-law scaling hallmarks seen in jammed particulate systems. To demonstrate this, I built a new all-atom protein model from scratch — using only hard-core repulsion, bond geometry, and weak hydrophobic attraction — that achieves near-zero Ramachandran and side-chain dihedral outliers without explicit dihedral restraints, staying within ~1 Å RMSD of crystal structures at jamming onset and refolding from partially unfolded states. The model shows that the stereochemical constraints of real amino acids shift jamming onset from φ ≈ 0.63 (simple polymers) down to exactly the φ ≈ 0.55 observed in nature.
Embryonic mesenchymal tissues are porous, under tension, and flow like a fluid — a combination that naively should be unstable. We developed a new particle-based interaction model with hysteretic sticking and stochastic bond kinetics to show that contact inhibition of locomotion (CIL) resolves this paradox, directing cell activity away from neighbors to prevent clustering. Mean-field continuum equations connect cell-scale parameters directly to emergent diffusivity, tension, and structural texture, collapsing simulation data across eight orders of magnitude and matching quantitative measurements in the avian presomitic mesoderm.
Protein cores pack to the same density as jammed repulsive amino acids — but proteins collapse via attraction, not compression. Is the correspondence deep or coincidental? I developed simulations of attractive and repulsive bead-spring polymers and disconnected disks under open boundary conditions, including a novel radial compression protocol for generating jammed packings without periodic boundaries. Collapsed attractive polymers quenched below the glass transition reach the same interior packing fraction as jammed repulsive systems across all system sizes, damping rates, and initial conditions. By decomposing the dynamical matrix into stiffness and stress components, I showed that repulsive polymer packings are hypostatic but effectively isostatic when accounting for quartic modes, and that attractive packings are also effectively isostatic under a contact definition set by the change in interaction stiffness. All four systems — repulsive and attractive, connected and disconnected — share the same power-law scaling for the vibrational density of states and excess contact number, establishing a universal connection between polymer collapse and jamming.