  The properties of a two-dimensional (2D) electron system can be drastically
altered by a magnetic field applied perpendicular to the 2D plane. In
particular, the frequency of its bulk collective excitations becomes gaped at
the cyclotron frequency, while the low-frequency localized excitations, the
edge magnetoplasmon (EMP), appear near the system's edge. A new type of the
delocalized low-frequency excitations, the gradient magnetoplasmon (GMP), was
recently shown to exist in a 2D electron system with a linear density gradient
that breaks the system's cylindrical symmetry [Phys. Rev. B \textbf{103},
075420 (2021)]. Like EMP, these new excitations are gapless and chiral, and
originate from the classical Hall effect. Here we show that a similar
magnetoplasmon mode can exist in a system with strongly-inhomogeneous radial
distribution of the electron density that preserves the cylindrical symmetry.
This is experimentally demonstrated in a pristine system of surface electrons
on liquid helium and is confirmed by a numerical simulation. This result
extends the variety of known collective excitations in a 2D charge system and
presents electrons on helium as a promising model system for their study.
