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Standing waves of the quintic NLS equation on the tadpole graph
by
Noja, Diego
, Pelinovsky, Dmitry E
in
Boundary conditions
/ Critical frequencies
/ Differential equations
/ Ground state
/ Nonlinearity
/ Saddle points
/ Standing waves
/ Variational methods
2020
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Standing waves of the quintic NLS equation on the tadpole graph
by
Noja, Diego
, Pelinovsky, Dmitry E
in
Boundary conditions
/ Critical frequencies
/ Differential equations
/ Ground state
/ Nonlinearity
/ Saddle points
/ Standing waves
/ Variational methods
2020
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Standing waves of the quintic NLS equation on the tadpole graph
Paper
Standing waves of the quintic NLS equation on the tadpole graph
2020
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Overview
The tadpole graph consists of a circle and a half-line attached at a vertex. We analyze standing waves of the nonlinear Schr\"{o}dinger equation with quintic power nonlinearity equipped with the Neumann-Kirchhoff boundary conditions at the vertex. The profile of the standing wave with the frequency \\(\\omega\\in (-\\infty,0)\\) is characterized as a global minimizer of the quadratic part of energy constrained to the unit sphere in \\(L^6\\). The set of minimizers includes the set of ground states of the system, which are the global minimizers of the energy at constant mass (\\(L^2\\)-norm), but it is actually wider. While ground states exist only for a certain interval of masses, the standing waves exist for every \\(\\omega \\in (-\\infty,0)\\) and correspond to a bigger interval of masses. It is shown that there exist critical frequencies \\(\\omega_0\\) and \\(\\omega_1\\) such that the standing waves are the ground states for \\(\\omega \\in [\\omega_0,0)\\), local minimizers of the energy at constant mass for \\(\\omega \\in (\\omega_1,\\omega_0)\\), and saddle points of the energy at constant mass for \\(\\omega \\in (-\\infty,\\omega_1)\\). Proofs make use of both the variational methods and the analytical theory for differential equations.
Publisher
Cornell University Library, arXiv.org
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