Abstract:In this paper we study some properties of anisotropic Orlicz and anisotropic Orlicz-Sobolev spaces of vector valued functions for a special class of G-functions. We introduce a variational setting for a class of Lagrangian Systems. We give conditions which ensure that the principal part of variational functional is finitely defined and continuously differentiable on Orlicz-Sobolev space.2010 Mathematics Subject Classification. 46B10 , 46E30 , 46E40.
“…Next, we will be concerned with the notion of G-function and Orlicz spaces. We refer the reader to [13,17] for more comprehensive information about convex functions and to [2,3,4,18,20] for more information on anisotropic G-functions and Orlicz spaces.…”
We consider the existence of periodic solutions to Hamiltonian Systems with growth conditions involving G-function. We introduce the notion of symplectic G-function and provide relation for the growth of Hamiltonian in terms of certain constant CG associated to symplectic G-function G. We discuss an optimality of this constant for some special cases. We also provide an applications to the Φ-laplacian type systems. * SECyT-UNRC, FCEyN-UNLPam and UNSL † SECyT-UNRC, FCEyN-UNLPam and CONICET 2010 AMS Subject Classification. Primary: 34C25 Secondary: 34B15
“…Next, we will be concerned with the notion of G-function and Orlicz spaces. We refer the reader to [13,17] for more comprehensive information about convex functions and to [2,3,4,18,20] for more information on anisotropic G-functions and Orlicz spaces.…”
We consider the existence of periodic solutions to Hamiltonian Systems with growth conditions involving G-function. We introduce the notion of symplectic G-function and provide relation for the growth of Hamiltonian in terms of certain constant CG associated to symplectic G-function G. We discuss an optimality of this constant for some special cases. We also provide an applications to the Φ-laplacian type systems. * SECyT-UNRC, FCEyN-UNLPam and UNSL † SECyT-UNRC, FCEyN-UNLPam and CONICET 2010 AMS Subject Classification. Primary: 34C25 Secondary: 34B15
“…In this section we briefly recall the notion of anisotropic Orlicz-Sobolev spaces. For more details we refer the reader to [10,1] and references therein. We assume that (G) G : R N → [0, ∞) is a continuously differentiable G-function (i.e.…”
Section: Orlicz-sobolev Spacesmentioning
confidence: 99%
“…It is proved in [10,Theorem 4.5] that for every u ∈ W 1 0 L G the following form of Poincaré inequality holds…”
Section: Orlicz-sobolev Spacesmentioning
confidence: 99%
“…The same is true if F (t, u, v) = G(v), since in this case R G (u n ) → R G (u). The last condition implies desired convergence for {u n } (see [10,Lemma 3.16] and [1, p. 593]).…”
Section: 1mentioning
confidence: 99%
“…(t, u n ,u n ) + F (t, u n , −u) 2 = (t, u,u) + F (t, u, −u) (t, u,u) + F (t, u, −u) 2 dt ≤ (t, u,u) + F (t, u, −u) 2 dt−lim sup I F t, u n ,u n −u 2 dtThusu n →u in L G by[10, Theorem 3.13]. Mountain Pass geometry.…”
Using the Mountain Pass Theorem we show that the problemx with growth condition determined by anisotropic G-function and some geometric condition of Ambrosetti-Rabinowitz type.2010 Mathematics Subject Classification. 46E30 , 46E40.
We will be concerned with the existence of homoclinics for Lagrangian systems in $${\mathbb {R}}^N$$
R
N
($$N\ge 3 $$
N
≥
3
) of the form $$\frac{d}{dt}\left( \nabla \Phi (\dot{u}(t))\right) +\nabla _{u}V(t,u(t))=0$$
d
dt
∇
Φ
(
u
˙
(
t
)
)
+
∇
u
V
(
t
,
u
(
t
)
)
=
0
, where $$t\in {\mathbb {R}}$$
t
∈
R
, $$\Phi {:}\,{\mathbb {R}}^N\rightarrow [0,\infty )$$
Φ
:
R
N
→
[
0
,
∞
)
is a G-function in the sense of Trudinger, $$V{:}\,{\mathbb {R}}\times \left( {\mathbb {R}}^N{\setminus }\{\xi \} \right) \rightarrow {\mathbb {R}}$$
V
:
R
×
R
N
\
{
ξ
}
→
R
is a $$C^2$$
C
2
-smooth potential with a single well of infinite depth at a point $$\xi \in {\mathbb {R}}^N{\setminus }\{0\}$$
ξ
∈
R
N
\
{
0
}
and a unique strict global maximum 0 at the origin. Under a strong force type condition around the singular point $$\xi $$
ξ
, we prove the existence of a homoclinic solution $$u{:}\,{\mathbb {R}}\rightarrow {\mathbb {R}}^N{\setminus }\{\xi \}$$
u
:
R
→
R
N
\
{
ξ
}
via minimization of an action integral.
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