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We calculated the decay widths of the $1^3F_2$ and $1^3F_4$ $s\bar{s}$ mesonsand compared them to the measured properties of the $\xi(2220)$ (now known asthe $f_4(2220)$). Including previously neglected decay modes we found that thewidth of the $^3F_2$ state $s\bar{s}$ meson is much larger than previouslybelieved making this explanation unlikely. On the other hand the predictedwidth of the $^3F_4$ state, although broader than the observed width, isconsistent within the uncertainties of the model. This interpretation predictslarge partial widths to $K K^*(892)$ and $K^*(892) K^*(892)$ final states whichshould be looked for. A second possibility that would account for the differentproperties of the $\xi(2220)$ seen in different experiments is that twohadronic states exist at this mass. The first would be a broader $^3F_4$$s\bar{s}$ state which is seen in hadron beam experiments while the secondwould be a narrow state with high glue content seen in the gluon rich $J/\psi$radiative decay. Further experimental results are needed to sort this out.Comment: Revised version to be published in Phys. Rev. D. Minor changes. Latex  file uses revtex version 3 and epsfig, 3 postcript figures are attached. The  full postcript version with embedded figures is available at  ftp://ftp.physics.carleton.ca/pub/theory/godfrey/ocipc9511.ps.

physical review. d. particles, fields, gravitation, and cosmology/physical review. d. particles and fields

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ξ(2220) reexamined: Strong decays of the 13F2and 1