Abstract
The transition from quasiperiodicity to chaos in an NMR laser with delayed feedback is investigated both experimentally and numerically. We concentrate on the low-delay-time region where stable tori arise either from a sequence of two Hopf bifurcations or from an ``interaction'' between mutually transversal unstable limit cycles. Transitions to chaos via intermittency and crises have been observed, as well as the ``fractalization'' of tori.
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