Localized structures named "fingers" form in the vicinity of the unwinding
transition of a cholesteric liquid crystal subjected to an electric field a
nd to homeotropic boundary conditions. Several types of fingers exist, with
different static and dynamic properties. For instance, cholesteric fingers
of the second species (CF-2) can drift perpendicular to their axes and for
m spirals in ac electric fields, whereas fingers of the first species (CF-I
) crawl along their axes. In this article we show that CF-2's are much easi
er to nucleate in thick samples (with respect, to the pitch) than in thin o
nes and may form loops like the CF-l's, with or without defects. We show th
at looped CF-l's always collapse in thick samples at increasing voltage, wh
ereas they can form cholesteric bubbles in thin samples. By contrast, we ne
ver observe the formation of a bubble from a loop of a CF-2 except when it
possesses a point defect. We also recall that CF-I segments always collapse
at increasing voltage, whereas CF-2 segments systematically give cholester
ic bubbles in similar conditions. To qualitatively explain these transforma
tions, we use a simplified representation on the unit sphere S2 of the dire
ctor field within the fingers. While the CF-l's are described within the st
andard model of Press and Arrot, we use for the CF-2's a recent model of Gi
l and Gilli, which we prove to explain most observations. We also describe
the growth and collapse dynamics of a loop of a CF-2 in close connection wi
th the spiral dynamics. Finally, we show experimentally and numerically tha
t the CF-2's get abruptly thinner when the electric field exceeds the spino
dal limit of the CF-1's. This transformation is reversible, but strongly hy
steretic. [S1063-651X(99)08205-7].