Recently, we suggested a type of self-trapped optical beams that can propag
ate in a stable form in (2 +1)D self-focusing Ken media: Necklace-ring beam
s [M. Soljacic, S. Sears, and M. Segev, Phys. Rev. Lett. 81, 4851 (1998)].
These self-trapped necklaces slowly expand their ring diameter as they prop
agate as a result of a net radial force that adjacent "pearls" (azimuthal s
pots) exert on each ether. Here, we revisit the self-trapped necklace beams
and investigate their properties analytically and numerically. Specificall
y, we use two different approaches and find analytic expressions for the pr
opagation dynamics of the necklace beams. We show that the expansion dynami
cs can be controlled and stopped for more than 40 diffraction lengths, maki
ng it possible to start thinking about interaction-collision phenomena betw
een self-trapped necklaces and related soliton effects. Such self-trapped n
ecklace-ring beams should also be observable in all other nonlinear systems
described by the cubic (2+1)D nonlinear Shrodinger equation-in almost all
nonlinear systems in nature that describe envelope waves.