Research

I work on the analysis of numerical methods for partial differential equations, particularly those that are built to respect the structure of the equations they approximate. Many PDEs, such as Maxwell’s equations and Fluids equations are written in terms of the gradient, curl, and divergence. The way these operators fit together is understood via the de Rham complex. Finite element exterior calculus (FEEC) and discrete exterior calculus (DEC) are frameworks for numerical methods which respect the de Rham complex structure. Much of my work is about analyzing these methods, and in this process, I frequently get to use tools in a broad spectrum of mathematical subjects including topology, geometry, analysis, and combinatorics. Understanding these connections is another key motivation for my research interest.

The de Rham complex in three dimensions and a finite element subcomplex made of Lagrange, Nédélec, Raviart–Thomas, and discontinuous piecewise polynomials. A commuting projection maps each space onto its discrete counterpart so that every square in the diagram commutes; for example, curl Π1h u = Π2h curl u.

Commuting projections

Commuting projections are a fundamental tool in FEEC. They map scalar and vector-valued functions onto finite element spaces in a way that commutes with the differential operators. They are the standard route to proving stability and error estimates for mixed and structure-preserving finite element methods. The most useful projections are local, bounded in L2, and commuting all at once. Having these three properties in combination is hard to arrange. The “canonical” interpolants commute but need extra smoothness, while earlier bounded projections were either global or bounded only in a stronger norm.

With Alexandre Ern, Johnny Guzmán, and Martin Vohralík, we constructed projections with all three properties onto the Lagrange, Nédélec, Raviart–Thomas, and discontinuous spaces of lowest and higher order on tetrahedral meshes. The projections are assembled from local weight functions which are piecewise polynomials on the Alfeld split of a patch of elements, computed by solving small discrete problems whose stability comes from discrete Poincaré inequalities (for the divergence and curl as well as the gradient).

The needed discrete Poincaré inequalities are often cited as known, but the results are spread across the literature under different hypotheses. Of interest for us, was having these inequalities with uniformly bounded constants over patches of elements. With Alexandre Ern, Johnny Guzmán, and Martin Vohralík, we wrote a review on these inequalities, providing three routes to proving the inequalities with ideas for tracking how the constants depend on the shape regularity of the mesh, the number of elements, and the polynomial degree, with particular attention to local patches of elements.

Furthermore, with Alexandre Ern and Johnny Guzmán, we developed commuting projections that also preserve piecewise polynomial boundary traces, which are useful for problems with nonhomogeneous boundary data.

A triangulation with one vertex star shaded and each of its six triangles split into three at its barycenter
A vertex star (shaded) in a triangulation, with each of its triangles split at its barycenter. This is the two-dimensional Alfeld split. In three dimensions each tetrahedron is split into four. The weight functions behind our projections are piecewise polynomials on split patches like this one.

Discrete exterior calculus

DEC represents discrete differential forms as cochains. These are essentially numbers attached to the vertices, edges, faces, and cells of a simplicial mesh and of its dual mesh. Then one has a discrete exterior derivative as the incidence matrix (coboundary operator) of the simplicial mesh and discrete Hodge stars are built from the geometry of the two meshes. DEC has wide applications in computer-aided geometric design as well as numerical methods for PDEs. The convergence theory for DEC on the other hand has lagged behind its application.

With Johnny Guzmán, we developed an analysis framework for DEC convergence and demonstrated its use by analyzing convergence for the Hodge-Laplace PDE. We also made connections between DEC and FEEC by viewing primal cochains as Whitney forms, and dual cochains as generalized Whitney forms on the circumcentric dual mesh.

A well-centered triangulation with its circumcentric dual mesh. The dual cell of one vertex is shaded and one primal edge is drawn with its perpendicular dual edge
A well-centered triangulation (solid lines) and its circumcentric dual (dashed lines), whose vertices are the circumcenters of the triangles. The dual cell of one vertex is shaded. Each dual edge is perpendicular to the primal edge it crosses which is key for the circumcentric Hodge star of DEC.

Discrete homotopy operators

The Poincaré lemma is a well known result in differential geometry which states that closed differential forms are exact on contractible domains. The standard proof is constructive through the use of a so-called Poincaré operator. In DEC and FEEC, discrete differential forms are realized as cochains and Whitney forms respectively. Thus, a natural question is to develop discrete Poincaré operators which map closed discrete differential forms on a contractible domain to exact discrete differential forms. With Johnny Guzmán, Anil Hirani, and Bingyan Liu, we constructed such operators which provide numerical methods for computing grad, curl, and div potentials. We also developed discrete Bogovskiĭ operators, which are analogues to the Poincaré operators preserving homogeneous boundary conditions. These operators also have applications in understanding the discrete wedge product of DEC. In further work with Johnny Guzmán and K. Olav Tyssvang, we extended these ideas to higher polynomial order Whitney forms.

A five-pointed star domain divided into triangles, each shaded by the value of a density: positive near the center, negative in the points of the star

Scalar function

The same triangulation with the discrete vector potential drawn as arrows: they circulate counterclockwise around the center and clockwise in the points of the star z

Vector potential

A discrete vector potential in two dimensions. Left: a scalar piecewise constant function on a triangulated star-shaped domain. Right: its discrete vector potential computed with the discrete Poincaré operator. The vector potential is drawn as the corresponding lowest-order Nédélec vector field. The 2d curl of the vector field on the right gives exactly the scalar function on the left.

Splines on triangulations

I am also interested in the fundamental theory behind splines on triangulations. Such splines are used in finite element methods and in computer-aided geometric design. A fundamental question posed by Strang in the 1970s asked: What is the dimension of the space of C1 piecewise polynomials of degree d on a given planar triangulation? The answer to Strang's question turns out to depend on both the combinatorial structure of the mesh as well as its geometry. Strang conjectured a dimension formula for these spline spaces and this formula was shown to hold for polynomial degree four and higher, and to not hold for degree two. The cubic case was a long-standing open problem which was resolved recently by Wu and Deng (2026) who exhibited a triangulation which breaks Strang's formula.

In a recent preprint, I showed how recent Large Language Models (LLMs) could be used to set up systematic autonomous searches for such triangulations which break Strang's formula. The key turned out to involve the combinatorics of symmetric triangulations, and I developed an algorithm which was able to find new triangulations breaking Strang's formula.

An equilateral triangle divided into 31 triangles with 15 interior vertices, arranged symmetrically about the center; three dashed mirror lines run from each corner through the center
A triangulation which breaks Strang's formula for bivariate C1 cubic splines.
Pratyush Potu speaking at a George Mason University podium in front of slides on exterior calculus
Me giving a talk at the Finite Element Circus, George Mason University, October 2025.
Group photo of the workshop participants on the steps of the Institute for Mathematical and Statistical Innovation in Chicago
Group photo at the DEC workshop at IMSI, Chicago, September 2025.