Articles
![]() |
09/02/2015--
09/02/2015
Adams' inequality with exact growth in the hyperbolic space $\mathbb{H}^4$ and Lions lemma
In this article we prove Adams inequality with exact growth condition in the
four dimensional hyperbolic space $\mathbb{H}^4,$
\begin{align}
\int_{\mathbb{H}^4} \frac{e^{32 \pi^2 u^2} - 1}{(1 + |u|)^2} \ dv_g \leq C
||u||^2_{L^2({\mathbb{H}^4})}.
\end{align} for all $u \in C^{\infty}_c(\mathbb{H}^4) $ with
$\int_{\mathbb{H}^4} (P_2 u) u \ dv_g \leq 1.$
We will also establish an Adachi-Tanaka type inequality in this settings.
Another aspect of this article is the P.L.Lions lemma in the hyperbolic space.
We prove P.L.Lions lemma for the Moser functional and for a few cases of the
Adams functional on the whole hyperbolic space.
Debabrata Karmakar
04/08/2011--
04/08/2011
Effective Cartan-Tanaka connections on C6-smooth strongly pseudoconvex hypersurfaces M3 of C2
In a recent expository article (Notices of the AMS, 58 (2011), no. 1, 20-27),
Ezhov, McLaughlin and Schmalz showed how to perform in an effective way
Tanaka's prolongation procedure valid generally for filtered structures of
constant type when the distribution is equipped with an integrable complex
structure, so as to derive the principal curvature invariants and (co)frame(s)
associated to strongly pseudoconvex real hypersurfaces M3 in C2, an approach
which is alternative and complementary to the `hyperspherical' connection of
Elie Cartan, and to the so-called calculi of Fefferman, of Chern-Moser, of
Webster. By choosing an initial frame for TM which is explicit in terms of a
local graphing function v = f(x, y, u) for M, we provide a Cartan-Tanaka
connection all elements of which are completely explicit in terms of f(x, y,
u), assuming only C6-smoothness of M. The Gaussian requirement for systematic
computational effectiveness then shows - a bit unexpectedly - that the two main
curvatures are rational differential expressions in the sixth-order jet of f(x,
y, u), the lengths of which are about 1000 pages long on a computer - just for
the simplest instance of local embedded CR geometry. Large parts of the memoir
aim at formulating general statements that will be useful for further
constructions of Cartan-Tanaka connections related to the equivalence problem
for (local) embedded CR manifolds whose CR-automorphism group is not
semi-simple, cf. e.g. some model lists by Beloshapka.
Mansour Aghasi
Joel Merker
Masoud Sabzevari
02/01/2021--
04/06/2020
Generalized Picone inequalities and their applications to $(p,q)$-Laplace equations
We obtain a generalization of the Picone inequality which, in combination
with the classical Picone inequality, appears to be useful for problems with
the $(p,q)$-Laplace type operators. With its help, as well as with the help of
several other known generalized Picone inequalities, we provide some nontrivial
facts on the existence and nonexistence of positive solutions to the zero
Dirichlet problem for the equation $-\Delta_p u -\Delta_q u = f_\mu(x,u,\nabla
u)$ in a bounded domain $\Omega \subset \mathbb{R}^N$ under certain assumptions
on the nonlinearity and with a special attention to the resonance case
$f_\mu(x,u,\nabla u) = \lambda_1(p) |u|^{p-2} u + \mu |u|^{q-2} u$, where
$\lambda_1(p)$ is the first eigenvalue of the $p$-Laplacian.
Vladimir Bobkov
Mieko Tanaka
01/04/2007--
12/06/2006
A Phantom does not Result from a Backreaction
The backreaction of nonlinear inhomogeneities to the cosmic expansion is
analyzed in the framework of general relativity with a cosmological constant.
By defining the spatially averaged matter energy density, we find that the
cosmological constant induces a new type of backreaction whose equation of
state is $p=-4/3 \rho$, where $\rho$ and $p$ are the effective energy density
and effective pressure of the backreaction in the averaged Friedmann universe.
However, the effective density is negative, and thus it decreases the
acceleration caused by the cosmological constant.
Hisako Tanaka
Toshifumi Futamase
12/31/2005--
12/30/2005
Non-associative Gauge Theory
We present a construction of gauge theory which its structure group is not a
Lie group, but a Moufang loop which is essentially non-associative. As an
example of non-associative algebra, we take octonions with norm one as a
Moufang loop, with which we can produce an octonionic gauge theory. Our
octonionic gauge theory is a natural generalization of Maxwell U(1)= S^1 gauge
theory and Yang-Mills SU(2)= S^3 gauge theory. We also give the BPST like
instanton solution of our octonionic gauge theory in 8 dimension.
Takayoshi Ootsuka
Erico Tanaka
Eugene Loginov
11/03/2020--
11/03/2020
Numerical verification method for positive solutions of elliptic problems
The purpose of this paper is to propose methods for verifying the positivity
of a weak solution $ u $ of an elliptic problem assuming $ H^1_0 $-error
estimation $ \left\|u-\hat{u}\right\|_{H_{0}^{1}} \leq \rho $ given some
numerical approximation $ \hat{u} $ and an explicit error bound $ \rho $. We
provide a sufficient condition for the solution to be positive and analyze the
range of application of our method for elliptic problems with polynomial
nonlinearities. We present numerical examples where our method is applied to
some important problems.
Kazuaki Tanaka
05/29/2025--
05/29/2025
Can we live in a baby universe formed by a delayed first-order phase transition?
We examine the idea that our universe began as a baby universe and show that
this is feasible in a $U(1)_{B-L}$ extension of the Standard Model with the
classically conformal principle. The framework is consistent with current
cosmological data and predicts a heavy neutral gauge boson, which could be
detected at colliders.
Qing-Hong Cao
Masanori Tanaka
Jun-Chen Wang
Ke-Pan Xie
Jing-Jun Zhang
11/05/2013--
11/05/2013
Remarks on the uniqueness for quasilinear elliptic equations with quadratic growth conditions
In this note we present some uniqueness and comparison results for a class of
problem of the form \begin{equation} \label{EE0} \begin{array}{c} - L u =
H(x,u,\nabla u)+ h(x), \quad u \in H^1_0(\Omega) \cap L^{\infty}(\Omega),
\end{array} \end{equation} where $\Omega \subset \R^N$, $N \geq 2$ is a bounded
domain, $L$ is a general elliptic second order linear operator with bounded
coefficients and $H$ is allowed to have a critical growth in the gradient. In
some cases our assumptions prove to be sharp.
David Arcoya
Colette De Coster
Louis Jeanjean
Kazunaga Tanaka
06/09/2017--
06/09/2017
Remarks on minimizers for $(p,q)$-Laplace equations with two parameters
We study in detail the existence, nonexistence and behavior of global
minimizers, ground states and corresponding energy levels of the
$(p,q)$-Laplace equation $-\Delta_p u -\Delta_q u = \alpha |u|^{p-2}u + \beta
|u|^{q-2}u$ in a bounded domain $\Omega \subset \mathbb{R}^N$ under zero
Dirichlet boundary condition, where $p > q > 1$ and $\alpha, \beta \in
\mathbb{R}$. A curve on the $(\alpha,\beta)$-plane which allocates a set of the
existence of ground states and the multiplicity of positive solutions is
constructed. Additionally, we show that eigenfunctions of the $p$- and
$q$-Laplacians under zero Dirichlet boundary condition are linearly
independent.
Vladimir Bobkov
Mieko Tanaka
08/31/2023--
08/31/2023
Abstract multiplicity results for $(p,q)$-Laplace equations with two parameters
We investigate the existence and multiplicity of abstract weak solutions of
the equation $-\Delta_p u -\Delta_q u=\alpha |u|^{p-2}u + \beta |u|^{q-2}u$ in
a bounded domain under zero Dirichlet boundary conditions, assuming $1<q<p$ and
$\alpha,\beta \in \mathbb{R}$. We determine three generally different ranges of
parameters $\alpha$ and $\beta$ for which the problem possesses a given number
of distinct pairs of solutions with a prescribed sign of energy. As auxiliary
results, which are also of independent interest, we provide alternative
characterizations of variational eigenvalues of the $q$-Laplacian using
narrower and larger constraint sets than in the standard minimax definition.
Vladimir Bobkov
Mieko Tanaka
|
|