**Riccardo Adami**,^{[a]} **Enrico Serra**,^{[b]} and **Paolo Tilli**^{[c]}

*Nonlinear dynamics on branched structures and networks
*

**Pages:** (* in press *)

**Received:** 6 February 2017

**Accepted in revised form:** 4 May 2017

**Mathematics Subject Classification (2010):** 35R02, 35Q55, 81Q35, 49J40.

**Keywords:** Minimization, metric graphs, critical growth, nonlinear Schrödinger Equation.

**Author address:**

[a],[b],[c]: Dipartimento di Scienze Matematiche, Politecnico di Torino, Corso Duca degli Abruzzi 24, Torino, 10129, Italy

**Abstract:**
In these lectures we review on a recently developed line of research, concerning
the existence of ground states with
prescribed mass (i.e. \(L^2\)-norm) for the *focusing* nonlinear Schrödinger
equation with a power nonlinearity,
* on noncompact quantum graphs*.
Nonlinear dynamics on graphs has rapidly become a topical issue with many
physical applications, ranging from
nonlinear optics to Bose-Einstein condensation. Whenever in a
physical experiment
a ramified structure is involved (e.g. in the propagation of signals, in a circuit of quantum wires or
in trapping a boson gas),
it can prove useful to approximate such a structure by a *metric graph*, or *network*.
For the Schrödinger
equation
it turns out that the *sixth* power in the nonlinear term of the energy (corresponding to the *quintic*
nonlinearity in the evolution equation) is *critical*
in the
sense that below that power the constrained energy is lower
bounded irrespectively of the value of the mass (*subcritical case*). On the other hand, if the nonlinearity
power equals six,
then the lower boundedness depends on the value of the mass: below a *critical mass*, the
constrained energy is lower bounded,
beyond it, it is not.
For powers larger than six the
constrained energy functional is never lower bounded, so that it is
meaningless to speak about ground states (*supercritical case*).
These results are the same as in the case
of the nonlinear
Schrödinger equation on the real line. In fact, as regards the existence of ground states, the results for systems on graphs differ,
in general, from the ones for systems on the line even in the subcritical case: in the latter case, whenever the
constrained energy
is lower bounded there always exist ground states (the *solitons*, whose shape is explicitly known),
whereas for graphs
the existence of a ground state is not guaranteed.
More precisely, we show that the existence of such constrained ground states
is strongly conditioned by the topology of the graph. In particular,
in the subcritical case we single out a
topological hypothesis
that prevents a graph from having ground states for every value of the mass.
For the critical case, our results show a phenomenology much richer than the analogous on the line:
if some topological assumptions are fulfilled,
then there may exist a whole interval of masses for which a ground state exist.
This behaviour is highly non-standard for \(L^2\)-critical
nonlinearities.

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