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Aram Karakhanyan

Publications and source records attributed to Aram Karakhanyan.

At least 19 recordsLinked to original sources

A Monotonicity formula for almost self-similar suitable weak solutions to the stationary Navier-Stokes equations in $\mathbb R^5$

In this paper we show that a suitable weak solution to the stationary Navier-Stokes system in $\mathbb R^5$, cannot behave like a self-similar function of degree negative one if the lower limit of the local Reynolds number is finite. To prove the result we develop a method that uses a monotonicity formula approach, classification of homogenous solutions to the incompressible Euler equations in $\mathbb R^5$, and a projection theorem.

math.AP↗

A new monotonicity formula for quasilinear elliptic free boundary problems

We construct a monotonicity formula for a class of free boundary problems associated with the stationary points of the functional \[ J(u)=\int_ΩF(|\nabla u|^2)+\mbox{meas}(\{u>0\}\cap Ω), \] where $F$ is a density function satisfying some structural conditions. The onus of proof lies with the careful analysis of the ghost function, the gradient part in the Helmholtz-Wéyl decomposition of a nonlinear flux that appears in the domain variation formula for $J(u)$. As an application we prove full regularity for a class of quasilinear Bernoulli type free boundary problems in $\R^3$.

math.AP↗

A monotonicity formula for a classical free boundary problem

We construct a monotonicity formula for the free boundary problem of the form $Δu=μ$, where $μ$ is a Radon measure. It implies that the blow up limits of solutions are homogenous functions of degree one. The first formula is new even for classical Laplace operator. Our method of proof uses a careful application of the strong maximum principle.

math.AP↗

Short-Rate Derivatives in a Higher-for-Longer Environment

We introduce a class of short-rate models that exhibit a ``higher for longer'' phenomenon. Specifically, the short-rate is modeled as a general time-homogeneous one-factor Markov diffusion on a finite interval. The lower endpoint is assumed to be regular, exit or natural according to boundary classification while the upper endpoint is assumed to be regular with absorbing behavior. In this setting, we give an explicit expression for price of a zero-coupon bond (as well as more general interest rate derivatives) in terms of the transition density of the short-rate under a new probability measure, and the solution of a non-linear ordinary differential equation (ODE). We then narrow our focus to a class of models for which the transition density and ODE can be solved explicitly. For models within this class, we provide conditions under which the lower endpoint is regular, exit and natural. Finally, we study two specific models -- one in which the lower endpoint is exit and another in which the lower endpoint is natural. In these two models, we give an explicit solution of transition density of the short-rate as a (generalized) eigenfunction expansion. We provide plots of the transition density, (generalized) eigenfunctions, bond prices and the associated yield curve.

q-fin.MF↗

Potential flows away from stagnation in infinite cylinders

Steady incompressible potential flows of an inviscid or viscous fluid are considered in infinite N-dimensional cylinders with tangential boundary conditions. We show that such flows, if away from stagnation, are constant and parallel to the direction of the cylinder. This means equivalently that a harmonic function whose gradient is bounded away from zero in an infinite cylinder with Neumann boundary conditions is an affine function. The proof of this rigidity result uses a combination of ODE and PDE arguments, respectively for the streamlines of the flow and the harmonic potential function.

math.AP↗

Stable cones in the Alt-Phillips free boundary problem

In this paper we prove a classification result for axially symmetric one phase minimizers of the Alt-Phillips free boundary problem in dimensions 3, 4, and 5. To accomplish this, we establish a stability inequality that extends the one for the Alt-Caffarelli problem.

math.AP↗

On the three-dimensional shape of a crystal

In this paper we completely settle the Almgren problem in $\mathbb R^3$ under some generic conditions on the potential and tension functions. The problem, among other things, appears in classical thermodynamics when one is to understand if minimizing the free energy with convex potential and under a mass constraint generates a convex crystal. Our new idea in proving a three-dimensional convexity theorem is to utilize a stability theorem when $m$ is small, convexity when $m$ is small, and the first variation PDE with a new maximum principle approach.

math.AP↗

The Dirichlet-Neumann Operator for Taylor's Cone

The aim of this paper is to analyse the Dirichlet-Neumann operator in axially symmetric conical domains. We provide a constructive treatment of the generic singularity at the vertex by using a new coordinate system that maps the conical domain to a strip. Building upon the paradifferential theory, we then establish our main Sobolev estimates. We also find the shape derivative, the linearization formula, and the cancellation property for the Dirichlet-Neumann operator. Our results can be viewed as the first step towards establishing the mathematical framework for the perturbations of Taylor's cone which appears in the jet break-up control.

math.AP↗

The Well-posedness of Cylindrical Jets with Surface Tension

In 1879 Rayleigh \cite{Rayleigh} studied the stability of infinite cylindrical jets, inspired by the experiments of Plateau \cite{Plateau}. The principal question that Rayleigh asked is: under what circumstances the jet is stable, for small displacements. In this paper we show that the jet flow is well-posed in short time if the initial condition belongs to some Sobolev space, and the initial jet boundary remains uniformly bounded away from the axis of symmetry. This will be proved by the method of paradifferential calculus and paralinearization. The salient feature of these results is that no smallness assumption is imposed on the initial condition.

math.AP↗

Minimizing the free energy

We prove the sharp quantitative stability in the radial isotropic Almgren problem. In addition, we develop a theory for estimating the sharp modulus in the context of minimal assumptions on the surface tension and the potential and obtain the sharp $ε^2$ in any dimension. Inter-alia, we also solve the problem of calculating the critical mass which was only a priori assumed to exist and which breaks the mass regime into two sets: the one where the energy is concave and the one where it is convex.

math.AP↗

Classification of global solutions of a free boundary problem in the plane

We classify nontrivial, nonnegative, positively homogeneous solutions of the equation \begin{equation*} Δu=γu^{γ-1} \end{equation*} in the plane. The problem is motivated by the analysis of the classical Alt-Phillips free boundary problem, but considered here with negative exponents $γ$. The proof relies on several bespoke results for ordinary differential equations.

math.AP↗

Regularity for the two phase singular perturbation problems

We prove that an a priori BMO gradient estimate for the two phase singular perturbation problem implies Lipschitz regularity for the limits. This problem arises in the mathematical theory of combustion where the reaction-diffusion is modelled by the $p$-Laplacian. A key tool in our approach is the weak energy identity. Our method proves a natural and intrinsic characterization of the free boundary points and can be applied to more general classes of solutions.

math.AP↗

A free boundary problem driven by the biharmonic operator

In this paper we consider the minimization of the functional \[ J[u]:=\int_Ω|Δu|^2+χ_{\{u>0\}} \] in the admissible class of functions \[ \mathcal A:= \left\{u\in W^{2, 2}(Ω) {\mbox{ s.t. }} u-u_0\in W^{1,2}_0(Ω) \right\}. \] Here, $Ω$ is a smooth and bounded domain and $u_0\in W^{2,2}(Ω)$ is a given function defining the Navier type boundary condition. The scale invariance of the problem suggests that, at the singular points of the free boundary, quadratic growth of $u$ is expected. We prove that $u$ is quadratically nondegenerate at the singular free boundary points using a refinement of Whitney's cube decomposition, which applies, if, for instance, the set $\{ u>0\}$ is a John domain. The optimal growth is linked with the approximate symmetries of the free boundary. More precisely, if at small scales the free boundary can be approximated by zero level sets of a quadratic degree two homogeneous polynomial, then we say that $\partial\{ u>0\}$ is rank-2 flat. Using a dichotomy method for nonlinear free boundary problems, we also show that, at the free boundary points $x\in Ω$ where $\nabla u(x)=0$, the free boundary is either well approximated by zero sets of quadratic polynomials, i.e. $\partial\{ u>0\}$ is rank-2 flat, or $u$ has quadratic growth. Differently from the classical free boundary problems driven by the Laplacian operator, the one-phase minimizers present structural differences with respect to the minimizers, and one notion is not included into the other. In addition, one-phase minimizers arise from the combination of a volume type free boundary problem and an obstacle type problem, hence their growth condition is influenced in a non-standard way by these two ingredients.

math.AP↗

Singular Yamabe problem for scalar flat metrics on the sphere

Let $Ω$ be a domain on the unit $n$-sphere $ \mathbb S^n$ and $\mathring{g}$ the standard metric of $\mathbb S^n$, $n\ge 3$. We show that there exists a conformal metric $g$ with vanishing scalar curvature $R(g)=0$ such that $(Ω, g)$ is complete if and only if the Bessel capacity $\mathcal C_{α, q}(\mathbb S^n\setminus Ω)=0$, where $α=1+\frac2n$ and $q=\frac n2$. Our analysis utilizes some well known properties of capacity and Wolff potentials, as well as a version of the Hopf-Rinow theorem for the divergent curves.

math.AP↗

Structure of singularities in the nonlinear nerve conduction problem

We give a characterisation of the singular points of the free boundary $\partial \{u>0\}$ for viscosity solutions of the nonlinear equation \begin{equation}F(D^2 u)=-χ_{\{u>0\}},\tag{0.1} \end{equation} where $F$ is a fully nonlinear elliptic operator and $χ$ the characteristic function. The equation (0.1) models the propagation of a nerve impulse along an axon. We analyse the structure of the free boundary $\partial\{ u>0\}$ near the singular points where $u$ and $\nabla u$ vanish simultaneously. Our method uses the stratification approach developed in [DK18]. In particular, when $n=2$ we show that near a rank-2 flat singular free boundary point $\partial\{ u>0\}$ is a union of four $C^1$ arcs tangential to a pair of crossing lines. Moreover, if $F$ is linear then the singular set of $\partial\{ u>0\}$ is the union of degenerate and rank-2 flat points. We also provide an application of the boundary Harnack principles to study the higher order flat degenerate points and show that if $\{u<0\}$ is a cone then the blow-ups of $u$ are homogeneous functions.

math.AP↗