We consider the focusing mass-supercritical semilinear Schrödinger
equation with a repulsive Dirac delta potential on the real line
:
where
,
denotes the Dirac delta with the mass at the origin, and
.
By a result of Fukuizumi, Ohta, and Ozawa (2008), it is
known that the system above is locally well-posed in the energy
space and there exist
standing wave solutions
when
, where
is a unique radial
positive solution to
.
Our aim in the present paper is to find a necessary and sufficient condition on the data below the
standing wave
to determine the global behavior of the solution. The similar result for NLS without
potential ()
was obtained by Akahori and Nawa (2013); the scattering result was
also extended by Fang, Xie, and Cazenave (2011). Our proof of the
scattering result is based on the argument of Banica and Visciglia (2016),
who proved all solutions scatter in the defocusing and repulsive case
() by the
Kenig–Merle method (2006). However, the method of Banica and Visciglia cannot be
applicable to our problem because the energy may be negative in the focusing case.
To overcome this difficulty, we use the variational argument based on the work of
Ibrahim, Masmoudi, and Nakanishi (2011). Our proof of the blow-up result is based
on the method of Du, Wu, and Zhang (2016). Moreover, we determine the global
dynamics of the radial solution whose mass-energy is larger than that of the standing
wave
.
The difference comes from the existence of the potential.
Keywords
global dynamics, standing waves, nonlinear Schrödinger
equation, Dirac delta potential