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Somnath Gandal

Publications and source records attributed to Somnath Gandal.

4 recordsLinked to original sources

Quasilinear problems with critical Sobolev exponent for the Grushin p-Laplace operator

We study the following class of quasilinear degenerate elliptic equations with critical nonlinearity \begin{align*} \begin{cases}-Δ_{γ,p} u= λ|u|^{q-2}u+|u|^{p_γ^{*}-2}u & \text{ in } Ω\subset \mathbb{R}^N, \\ u=0 & \text{ on } \partial Ω, \end{cases} \end{align*} where $Δ_{γ, p}v:=\sum_{i=1}^N X_i(|\nabla_γu|^{p-2}X_i u)$ is the Grushin $p$-Laplace operator, $z:=(x, y) \in \mathbb{R}^N$, $N=m+n,$ $m,n \geq 1,$, where $\nabla_γ=(X_1, \ldots, X_N)$ is the Grushin gradient, defined as the system of vector fields $X_i=\frac{\partial}{\partial x_i}, i=1, \ldots, m$, $X_{m+j}=|x|^γ\frac{\partial}{\partial y_j}, j=1, \ldots, n$, where $γ>0$. Here, $Ω\subset \mathbb{R}^{N}$ is a smooth bounded domain such that $Ω\cap \{x=0\}\neq \emptyset$, $λ>0$, $q \in [p,p_γ^*)$, where $p_γ^{*}=\frac{pN_γ}{N_γ-p}$ and $N_γ=m+(1+γ)n$ denotes the homogeneous dimension attached to the Grushin gradient. The results extends to the $p$-case the Brezis-Nirenberg type results in Alves-Gandal-Loiudice-Tyagi [J. Geom. Anal. 2024, 34(2),52]. The main crucial step is to preliminarily establish the existence of the extremals for the involved Sobolev-type inequality \begin{equation*} \int_{\mathbb{R}^N} |\nabla_γ u|^p dz \geq S_{γ,p} \left ( \int_{\mathbb{R}^N} |u|^{p_γ^*} dz \right )^{p/p_γ^*} \end{equation*} and their qualitative behavior as positive entire solutions to the limit problem \begin{equation*} -Δ_{γ,p} u= u^{p_γ^{*}-1}\quad \mbox{on}\, \mathbb{R}^N, \end{equation*} whose study has independent interest.

math.AP

Three non-zero solutions of a Neumann eigenvalue problems involving the fractional p-Laplacian

In the present paper, we establish a multiplicity result for a following class of nonlocal Neumann eigenvalue problems involving the fractional p-Laplacian. \begin{align} \begin{cases} (-Δ)^{s}_{p}u + a(x) \abs{u}^{p-2}u =λh(x,u) & \text {in } Ω, \mathcal{N}_{s,p}u=0 & \text {in } \mathbb{R}^N \setminus \overlineΩ, \end{cases} \end{align} Precisely, we demonstrate the existence of an open interval for positive eigenvalues $λ$, for which the problem has at least three non-zero solutions in $W^{s,p}_Ω.$

math.AP

The Neumann problem for a class of semilinear fractional equations with critical exponent

We establish the existence of solutions to the following semilinear Neumann problem for fractional Laplacian and critical exponent: \begin{align*}\left\{\begin{array}{l l} { (-Δ)^{s}u+ λu= \abs{u}^{p-1}u } & \text{in $ Ω,$ } \\ \hspace{0.8cm} { \mathcal{N}_{s}u(x)=0 } & \text{in $ \mathbb{R}^{n}\setminus \overlineΩ,$} \\ \hspace{1.6cm} {u \geq 0}& \text{in $Ω,$} \end{array} \right.\end{align*} where $λ> 0$ is a constant and $Ω\subset \mathbb{R}^{n}$ is a bounded domain with smooth boundary. Here, $p=\frac{n+2s}{n-2s}$ is a critical exponent, $n > \max\left\{4s, \frac{8s+2}{3}\right\},$ $s\in(0, 1).$ Due to the critical exponent in the problem, the corresponding functional $J_λ$ does not satisfy the Palais-Smale (PS)-condition and therefore one cannot use standard variational methods to find the critical points of $J_λ.$ We overcome such difficulties by establishing a bound for Rayleigh quotient and with the aid of nonlocal version of the Cherrier's optimal Sobolev inequality in bounded domains. We also show the uniqueness of these solutions in small domains.

math.AP

Asymptotic behaviour of the least energy solutions of fractional semilinear Neumann problem

We establish the asymptotic behaviour of the least energy solutions of the following nonlocal Neumann problem: \begin{align*} \left\{\begin{array}{l l} { d(-Δ)^{s}u+ u= \abs{u}^{p-1}u } \text{ in $Ω,$ } { \mathcal{N}_{s}u=0 } \text{ in $\mathbb{R}^{n}\setminus \overlineΩ,$} {u>0} \text{ in $Ω,$} \end{array} \right.\end{align*} where $Ω\subset \mathbb{R}^{n}$ is a bounded domain of class $C^{1,1}$, $1 \max \left\{1, 2s \right\}, 0 0$ and $\mathcal{N}_{s}u$ is the nonlocal Neumann derivative. We show that for small $d,$ the least energy solutions $u_d$ of the above problem achieves $L^{\infty}$ bound independent of $d.$ Using this together with suitable $L^{r}$-estimates on $u_d,$ we show that least energy solution $u_d$ achieve maximum on the boundary of $Ω$ for $d$ sufficiently small.

math.AP