A　method　is　presented　for　generating　highly　squeezed　states　in　a　cavity　field.　In　this　scheme,　a　sequence　of　two-level　atoms　is　sent　through　a　resonant　cavity　and　driven　by　a　strong　classical　field;　then　the　atomic　states　are　measured.　In　this　way,　the　cavity　field　may　collapse　onto　a　superposition　of　several　coherent　states,　which　exhibits　strong　squeezing.