In this paper we study the fast adiabatic-like expansion of a one-dimensional
Bose-Einstein condensate (BEC) confined in a harmonic potential, using the
theory of time-optimal control. We find that under reasonable assumptions
suggested by the experimental setup, the minimum-time expansion occurs when the
frequency of the potential changes in a bang-bang form between the permitted
values. We calculate the necessary expansion time and show that it scales
logarithmically with large values of the expansion factor.
In this article we study the frictionless cooling of atoms trapped in a
harmonic potential, while minimizing the transient energy of the system. We
show that in the case of unbounded control, this goal is achieved by a singular
control, which is also the time-minimal solution for a "dual" problem, where
the energy is held fixed. In addition, we examine briefly how the solution is
modified when there are bounds on the control.
In this letter, we apply optimal control theory to design minimum-energy
$\pi/2$ and $\pi$ pulses for the Bloch system in the presence of relaxation
with constrained control amplitude. We consider a commonly encountered case in
which the transverse relaxation rate is much larger than the longitudinal one
so that the latter can be neglected. Using the Pontryagin's Maximum Principle,
we derive optimal feedback laws which are characterized by the number of
switches, depending on the control bound and the coordinates of the desired
final state.
In this report, we apply Optimal Control Theory to design minimum energy
$\pi/2$ and $\pi$ pulses for Bloch equations, in the case where transverse
relaxation rate is much larger than longitudinal so the later can be neglected.
Using Pontryagin's Maximum Principle, we derive an optimal feedback law and
subsequently use it to obtain analytical expressions for the energy and
duration of the optimal pulses.